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== Limits of current human knowledge == | |||
__TOC__ | |||
Looking over the article and all the archived discussions, one basic thought occurs to me: Humans do not fully and clearly understand why airfoils generate lift. There are various competing explanations, and there is no broad, general, and complete consensus among scientists as to why airfoils generate lift. This is an astounding fact. I think this aspect of current human understanding should be mentioned in the introduction to the article. It is remarkable with the wide-spread use of airfoils throughout history (age of sail, age of flight) that humans do not fully and clearly understand why the airfoil works. --] (]) 18:06, 20 March 2013 (UTC) | |||
== Lift force: New Theory of Flight == | |||
:I rather strongly disagree with the assessment that "there is no broad, general, and complete consensus among scientists as to why airfoils generate lift." In fact I would say just the opposite, that the science and engineering of airfoils and lift is a mature subject that is well understood and "settled" science. If you have gotten the opposite impression from the article, I apologize. | |||
The following information to the reader is being removed by Dolphin51 | |||
:Where there ''is'' disagreement is in how to explain these rather complicated and sophisticated ideas in layman's terms. This disagreement over ''pedagogy'' is quite distinct from any controversy over the underlying science. | |||
1. There is no commonly accepted explanation of the generation of large lift at small drag of a wing as expressed as late as 2020 in Scientific American as “No one knows what keeps planes in the air”. | |||
:I am now more inclined to agree with J Douglas McLean's statement upthread that "the quote by John D. Anderson gives the misleading impression that there are disagreements over the science itself, not just the qualitative explanations" and will remove that material. ] (]) 19:02, 20 March 2013 (UTC) | |||
2. Any reference to the peer reviewed published work New Theory of Flight, Journal of Mathematical Fluid Mechanics, 2017, by Hoffman and Johnson, which offers a new explanation, is being removed. | |||
::I agree that when read by a layman, the article certainly gives the impression that lift is not "settled" science. To the layman, it certainly reads as if there are various competing explanations for the underlying science. For example, this introductory section definitely gives the impression of various competing explanations of the underlying science: ''"There are several ways to explain how an airfoil generates lift. Some are more complicated or more mathematically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton’s laws of motion and explanations based on Bernoulli’s principle. Either can be used to explain lift."'' Does the Newton explanation conflict with the Bernoulli explanation? Newton and Bernoulli are not alternative explanations of lift; rather they are both in effect simultaneously to create lift, aren't they? Then why present them as two alternatives? It is relatively easy for the layman to understand the Bernoulli effect, but the key question that the article never explains clearly to a layman is: Why does the air on the top flow faster than the air on the bottom? This is the key point. Later the article says "Explaining lift while considering all of the principles involved is a complex task and is not easily simplified." To me, this is a cop out as far as Misplaced Pages is concerned. The article is basically saying "We're going to punt on any attempt to explain this to a layman, and instead divert into scientific mumbo-jumbo that you will never understand." Is it really so hard to explain why the air on top is flowing faster than the air on bottom? Overall I am quite disappointed in this Misplaced Pages article. --] (]) 19:29, 21 March 2013 (UTC) | |||
I think the whole concept of "multiple explanations" is the wrong way to approach this topic. It leads to deep confusion in the layman. If it is settled science, there should be one explanation which can be presented in greater or lesser levels of depth. --] (]) 19:38, 21 March 2013 (UTC) | |||
:I think that the problem being described here is the one about the way science is taught (in some schools). First there are phenomena in the real world, then there are scientific theories and mathematical models that attempt to explain the phenomena. There's nothing ''after'' that - no point at which physical phenomena stop being what they were and start following the dictates of the mathematical models, rather than their own inscrutable processes. That does not mean that science is wrong or badly understood, but that the scientific models and equations we have, are all we have, apart from the mysterious wonders of nature itself. People try to use similar arguments to rubbish climate science - "If this is all just a theory, then let's wait until it's been sorted out", etc. Lift ''is'' settled science - jet airliners fly every day to within tolerances very close to those their designers intended - but there isn't one simple explanation. We just have to get used to that. --] (]) 20:35, 21 March 2013 (UTC) | |||
What is the motivation to hiding 1 and 2 from the public? ] (]) 07:00, 31 July 2021 (UTC) | |||
:1. The Scientific American article titled “No-one can explain why planes stay in the air” is an article that has been seen here before, and has been analysed in some detail. We weren’t much impressed. See ]. | |||
:<i>>... there should be one explanation which can be presented in greater or lesser levels of depth.</i> | |||
::If you want to initiate a discussion about this Scientific American article you are welcome to do so on this Talk page, but you can see how it has been regarded in the past. ] ''(])'' 07:44, 31 July 2021 (UTC) | |||
:Alas, the world is not that simple. Almost every scientific principle admits multiple explanations. For instance, there are at least nine ways to prove the fundamental theorem of algebra, and this is an area that has been "settled" for centuries. As another example, many problems in Newtonian physics can be approached in multiple ways - conservation of energy, conservation of momentum, direct application of newton's laws, the principle of least action, etc. These are just different ways of looking at the same problem. | |||
:2. I reverted the following text: ''A New Theory of Flight first presented in Computational Turbulent Incompressible Flow as a new explanation of the generation of large lift at small drag of a wing based on computing turbulent solutions of Euler's equations supported by mathematical analysis, has been developed by J. Hoffman, J. Jansson and C. Johnson.'' See my . | |||
:Much of the controversy surrounding lift is due to some individuals thinking that there is "one true explanation" that is correct and therefore all other explanations must be incorrect. Unfortunately, one of the most common explanations actually ''is'' incorrect; were this not the case I surmise that the differing explanations would simply sit quietly side-by-side as they do in most topics. | |||
::This text said almost nothing about the new theory of flight, but it gave prominence to the authors. On Misplaced Pages, the authors of cited sources are not identified in the article, but they should be identified in an in-line citation. | |||
:I agree that the sentence "Explaining lift while considering all of the principles involved is a complex task and is not easily simplified." adds little to the article, and we have contemplated removing it. Maybe its time has come? Opinions form other editors? | |||
::If you are one of Hoffman, Jansson or Johnson, or you have a close association with them, there may be a ]. | |||
:Finally, to answer your question "Why does the air on the top flow faster than the air on the bottom?" there's a very simple answer: | |||
::There may be a case for adding this information to the article but it should be added in accordance with encyclopaedic standards. I recommend you have a look at some or all of the following: | |||
::When air follows a path that is curved, the pressure is lower on the inside of the curve than on the outside. So, there's a region of lowered pressure on the top side of the wing. When the air flows from atmospheric pressure into this lower pressure region, there is more pressure behind than in front resulting in a net force on the air which speeds it up. (the last sentence is basically Bernoulli's principle in a nutshell) | |||
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:Regards, ] ''(])'' 08:57, 31 July 2021 (UTC) | |||
:Perhaps something like this should be added to the article. I've never considered "why does the air speed up" to be a "key point" since lift can be explained (albeit incompletely) without even mentioning the speed changes. But if our readers are coming here looking for the answer to that question, perhaps we should present it. ] (]) 20:42, 21 March 2013 (UTC) | |||
The book Understanding Aerodynamics by Doug McLean gives hard evidence that a common agreement on a scientific explanation of the generation of large lift at small drag of an airplane wing is missing, as just one piece of evidence to this very remarkable fact expressed in the Scientific American article. Why should Misplaced Pages hide this state affairs from the public? | |||
::I agree with Mr Swordfish, and I disagree with Westwind273 when he writes ''Humans do not fully and clearly understand why airfoils generate lift.'' I disagree for two reasons. Firstly, science does not address questions about ''why'' the universe operates the way it does. That is a question for theology. Science merely observes the universe and attempts to determine principles and laws which describe these things. As a simple example, scientists understand and apply Newton's first law of motion but science does not bother with the question of ''why'' a force is necessary to cause an object to accelerate. Theologians might explain that a force is necessary because God dictated that it would be so, but scientists find Newton's observations, and his laws of motion, to be entirely adequate. Similarly, Bernoulli observed the flow of fluids and the interchange of speed and pressure and described it all in his famous principle; but he didn't bother to include any speculation about ''why'' it is so. That would not be science. | |||
::Secondly, Westwind273 has grasped John Anderson's statement that scientists and engineers disagree over what is the most fundamental way to explain the phenomenon of aerodynamic lift. Westwind273 has misunderstood Anderson to be referring to some remarkable mystery about aerodynamic lift. If it is true that humans do not fully and clearly understand these things, then that is equally true of any scientific phenomenon. Westwind273 should also be writing that humans do not fully and clearly understand magnetism, electricity, meteorology, thermodynamics, and so on. There is nothing specially intractable about aerodynamic lift which is a splendid application of Bernoulli's principle, ], Newton's third law of motion, the principle of ] and so on. Each person contemplating the phenomenon of aerodynamic lift, whether that person is a student pilot, college student, professional engineer or research aerodynamicist, must choose whichever of these scientific principles is most satisfactory for him. There is no ''one true explanation'' for any scientific phenomenon, and certainly not aerodynamic lift. ] ''(])'' 23:28, 21 March 2013 (UTC) | |||
Why is any reference to the New Theory of Flight, which gives the first full scientific explanation backed by solid math and computation, , removed? | |||
I think it's understandable that ] got the mistaken impression from the current article that there is a lack of consensus on the science of lift. And I largely agree with the responses by ], ], and ], but with some quibbles below. I have a suggested revised version of the article in my sandbox ] that I think would avoid the mistaken impression that ] got. It sets the record straight on the science and also answers the question of why the flow over the upper surface speeds up a little differently from the way ] did. I'd appreciate it if ] would read my suggested version and provide feedback. | |||
Are you open to a section explaining the essence of the New Theory of Flight? Yes I am one of the authors (Johnson). <!-- Template:Unsigned --><span class="autosigned" style="font-size:85%;">— Preceding ] comment added by ] (] • ]) 08:59, 31 July 2021 (UTC)</span> | |||
The answer by ] to the question "Why does the air on the top flow faster than the air on the bottom?" is a good start, but it needs to be added that the cause-and-effect relationship between the pressure field and the velocity field is circular, as explained in my suggested revision. Both flow curvature and changes in flow speed are caused by differences in pressure, and the differences in pressure are sustained by the changes in flow direction and speed. | |||
:You have written about a "common agreement on a scientific explanation of ... lift ..." You have also referred to "this very remarkable fact". In the past decades we have seen many examples of people who believe there can only be one truly correct explanation of aerodynamic lift. These people seem to think "my explanation is correct so all other attempts at explanation must be incorrect." Similarly, there is no reason to expect that scientists will reach agreement on one truly correct way to explain aerodynamic lift. The majority of Users who work regularly on the topic of lift reject as nonsense these suggestions that there is only one truly correct explanation of lift. We also reject as nonsense the suggestion that scientists should reach agreement on one explanation of lift, or that there is something mysterious or sinister in the fact that different scientists display expertise in different ways to explain lift. | |||
The issue of cause-and-effect and "why" has come up before, and I still don't entirely agree with the hard-line take on that topic by ]. I agree that for some fundamentals like Newton's second law we don't understand the "why". But at other levels, I think it's perfectly reasonable to talk about causation and "why", as in saying that a force causes an acceleration. So "why" does something accelerate? Because of a force. "Why" are force and acceleration related the way they are? We don't know. ] (]) 02:07, 6 April 2013 (UTC) | |||
:The reason your edits have been erased has nothing to do with wishing to hide your theory from public view - it has everything to do with the way it is written and presented in the article. To see how a theory should be written and presented, look closely at the various theories already firmly entrenched in the article - see Sections 2, 4 and 6 in the list of Contents. Also look at the 5 guidance articles I linked in my previous edit. Of course we are open to a section covering a new theory of flight - but it needs to be written in a way that is compatible with the encyclopaedic standards applied across Misplaced Pages. I recommend you draft the section and present it on this Talk page, or on your own personal sandbox, and then use the Talk page to invite interested Users to peruse it and make their comments. | |||
:Please remember to sign your Talk page edits with four tildes. ] ''(])'' 13:06, 31 July 2021 (UTC) | |||
::Your latest addition to the article (see the ) looks like an advertisement for a book or a public lecture, rather than a scholarly entry in an encyclopaedia. It contains no in-line citation of the kind required on Misplaced Pages. You have written "The new theory reveals the true physics of generation of large lift ..." The ''true physics'' - wow, that is a bold claim indeed! It is not an appropriate claim to make on an encyclopaedia, especially when you have correctly revealed that you have a potential conflict of interest in all matters of the New Theory of Lift. | |||
::I suggest you look carefully at the existing content of this article and revise your additions so they look consistent with the rest of the content. ] ''(])'' 13:19, 31 July 2021 (UTC) | |||
:::It also only cites one primary source and a self-published source. According to the manual of style's guidance for ]: | |||
::::Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors. | |||
:::So, the latest edit fails to meet basic inclusion criteria. ] (]) 23:06, 31 July 2021 (UTC) | |||
:My opinion is that this article has long suffered from the fact that we editors are sometimes too close to the subject matter and get caught up in meta-discussions about the material instead of just presenting the material in a srtraightforward manner. We've all read the great Bernoulli/Newton debates of the 90s, and while this is interesting to folks who already know quite a bit about the subject I do not think it is helpful to re-hash that debate here. Perhaps it belongs in its own wikipedia article, but the purpose of this article is to introduce the basic ideas in a manner understandable to the lay reader. It seems to me that when we write about how we're we're going to explain the actual subject, we've made the artcle harder to understand by encapsulating it in a second layer of meta-analysis. | |||
I appreciate that I can have a discussion with Misplaced Pages on the important scientific question about "what keeps planes on the air" citing Scientific American 2020 reporting that "nobody knows". The fact that this question does not have a proper answer more than 100 years after the take off of powered human flight in 1903 is very remarkable, impossible to understand for the general general public, and kept as a secret kept within the scientific community of fluid dynamics hidden from the public. Yet it is true, and the evidence is massive. There is no convincing theory of flight in the standard scientific literature, and this is clearly evidenced by the Misplaced Pages article on Lift presenting lots of material but no theory claimed to be correct, because there is none. If there was a correct theory, known to be correct, then Misplaced Pages would present this theory and all incorrect theories now being presented would serve no role. The New Theory of Flight is a new scientific theory for the generation of lift at small drag of a wing with massive support from computation and mathematical evidence developed by leading academicians and published in leading peer reviewed journals opening a new window in the AIAA HiLift Workshops. Misplaced Pages can here serve an important role to expose this new theory to the scientific community for scrutiny and the general public for information. Can we agree on this mission?] (]) 18:39, 31 July 2021 (UTC) | |||
Regarding the Scientific American article, it's a pretty clear case of journalistic malpractice. John D. Anderson said "There is no simple one-liner answer to this...” The author misrepresented his statement as "What Anderson said, however, is that there is actually no agreement on what generates the aerodynamic force known as lift." which is a completely different statement. | |||
:The result is that some readers, such as Westwind, get the mistaken impression that there is a lack of scientific consensus. Doug has suggested that we add language to correct that impression, eg; ''The mathematical theories are scientifically rigorous, are supported by empirical observations, and have been agreed upon by the scientific and engineering communities since the early 20th century.'' My take is that this should go without saying, ''of course'' the theories are rigorous and well accepted - having to state it explicitly seems like we "doth protest too much". | |||
This was further compounded by the headline writer (often headlines are written by someone other than the author of the article, so I don't know precisely who to blame here) who turned that into the sensationalist click-bait headline "No One Can Explain Why Planes Stay in the Air" It's utter crap. That said, if the author had turned down the hyperbole there's a decent article there. | |||
:To put a finer point on it, ''everything'' in science has multiple explanations; ''all'' science is rigorous (otherwise it wouldn't be science). There is no need to apologize for choosing one explanation over another, or to have to make assurances that the science is actually ''science''. | |||
Regarding Hoffman et. al. to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. As such it's ]. Perhaps that will change, but until it does, their work doesn't belong in the article. Maybe Doug can add some perspective here. | |||
:So, I would advocate editing the article to downplay the Bernoulli/Newton "controversy", and to avoid giving the impression that these are two or more competing theories. As an example, take a look at the ] article itself - it states that BP can be derived from either conservation of momentum or by directly integrating newton's 2nd law. To my eyes, it does so without implying that one is correct and the other is wrong, or that there's any controversy over which derivation is correct. The subtext is that ''both'' are correct; somehow that subtext seems to be missing in this article. I do think that this article should present both explanations, but I think we can do so without making such a fuss over it. In fact, the more I think about the subject, the more I am persuaded that it's really one big explanation that fits together in harmony, rather than multiple competing theories. | |||
While it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic, from internal combustion engines to cheese making. There's nothing mysterious going on here - there are very well established models of lift that are quite well understood, at least by practicing aerodynamic professionals. What has happened is that for the better part of the 20th century the most common simple explanation turned out to be just plain wrong, and when that was pointed out, people being human held tightly on to it because nobody ever wants to admit that they were wrong. Much debate and argument followed, with disagreement on how best to take a complex subject and explain it simply. That's very different than "nobody knows" or even "there is no agreement on the (mathematical) theory." Were we to propagate the "nobody knows" shibbolleth we'd be remiss in our duties as wikipedia editors. ] (]) 21:46, 31 July 2021 (UTC) | |||
:By way of analogy, this subject reminds me of the ]. It's a great parable, but here we're writing an article describing elephants, not the arguments of the blind men. Statements like "some say the elephant is like a snake and some say it is like a wall" doesn't really advance the article. | |||
Yes, it is a good idea to call in Doug McLean who has written an excellent book on flight theory with an attempt to come up with something better than the standard theories all know to be incorrect. I have written which I ask you to read and answer the questions posed at the end. Will you do that?] (]) 11:00, 1 August 2021 (UTC) | |||
:In other matters, Doug has pointed out a definite shortcoming of the current article - the airfoil affects the flow over a wide area around it - and this fact along with the reasons why it occurs (ie the self re-enforcing interplay between pressure and fluid motion) should be incorporated into the article. I'll take a swat at this in coming days, most likely just stealing Doug's text. ] (]) 21:20, 8 April 2013 (UTC) | |||
::The blind men and the elephant is spot on. Avoid the arguments between the blind men, and ignore those who ask "Why is there an elephant in the room anyway?" This is an article about lift, and the main conceptual and mathematical models that enable pilots and engineers to understand and manipulate lift. People who want to know why, or how did we get here, are looking for different topics, for which there may or may not be articles at this time. --] (]) 22:33, 8 April 2013 (UTC) | |||
:Yes, I have read your blog as you requested. I deplore the fact that you have named {{ping|Mr swordfish}} in your blog in the way you have done, presumably without their consent or prior knowledge. This is immature behavior that is unlikely to find any support in the scientific community. | |||
I understand the urge to simplify things by downplaying the "meta-analysis", but I think it would be a mistake. | |||
:At the end of your blog you ask several questions. All your questions are ]. I'm sure you don't know what a rhetorical question is, so I will explain. A rhetorical question is one that is asked without any genuine expectation of an answer; usually because no answer exists or because no answer is wanted. For example, "Why do we have to endure this horrible Covid pandemic?" is a rhetorical question. In a genuine scientific or philosophical dialogue people say what they mean; they don't ask rhetorical questions. | |||
:I am building a picture of User:SecretofFlight as a somewhat immature and petulant person; someone more interested in advertising his theory than promoting the best quality article on Misplaced Pages. Please grow up or I will stop communicating with you. ] ''(])'' 12:51, 1 August 2021 (UTC) | |||
You say regarding Hoffman et. al to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. You are not well informed. The New Theory is now through Jansson an important discussion point at the collecting world leading competence. | |||
If we were the only ones who had ever discussed alternate explanations of lift, and if the controversies were limited to our little talk-page circle, then I'd agree that those discussions would be out of place in the article. But that's not the situation. The public folklore on this topic is full of misconceptions and erroneous explanations. And the controversies have been out there in public view for decades. I'll bet many of the potential readers of this article have already read a Bernoulli explanation (likely based on longer path length) or deflection explanation of lift and have probably also read somewhere that one or the other is wrong. And they're also very likely to have already gotten the impression from somewhere that the science is unsettled. | |||
You say that while it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic. This is a misconception about what science is. The main objective of science is to give correct explanations of natural phenomena and it is crucial to distinguish correct theory from false theory. The fact that there is no theory of flight accepted as a correct theory is truly remarkable and efforts to cover up this fact is not science and not in the interest of the public. ] (]) 11:20, 1 August 2021 (UTC) | |||
So the fact that the science on this particular topic is in good shape doesn't speak for itself. It needs to be spelled out. And given what's out there in the popular culture, we'd be short-changing the reader if we left out discussion of the pros and cons of the alternate explanations (and the outright errors in some versions). Whether we like it or not, these issues are now part of the topic of lift. Just the straight facts will not be enough to enable a reader to see through the fog. | |||
I did not get any answer on my question posed on my blog so I repeat it here: Why does Misplaced Pages censor any reference to the well documented New Theory of Flight in a Misplaced Pages article on Lift (force), which is only an account of old theories all known to be incorrect? | |||
Mr. Swordfish (]), you suggest that we should present "both explanations" of lift in the same way that the ] article presents its two alternate derivations. I don't entirely agree. Both derivations of Bernoulli ''are'' actually correct and self-sufficient. Our two simpler explanations of lift are both correct to some extent but also have significant shortcomings. The shortcomings shouldn't be swept under the rug. | |||
I guess the reason is that the Wikipedians exercising the censorship (Dolphin51 and Mr swordfish) do not themselves carry the scientific expertise required to properly evaluate the merits of the New Theory of Flight and so take the simple way out to dismiss it without any scrutiny. But if so, this is not in the interest of the public. If there is a correct theory of flight, it should not be hidden to the people, in particular not to all people relying on safe air transportation. So I add the following question: Which experts are Misplaced Pages relying on, when dismissing/censoring the New Theory of Flight? ] (]) 18:58, 1 August 2021 (UTC) | |||
:The very simple answer as to why the material was removed is that it does not conform to the various wikipedia policies regarding notability, sourcing, and possibly conflict of interest. Dolphin and I have provided links to the help pages that clearly explain the policies and the reasoning behind them. I would suggest you read them, especially ], ], ], and ] I'd also suggest you drop the allegations of censorship - they just make your case look weak. | |||
Mr. Swordfish, you also say you're persuaded that the two simpler explanations really amount to "one big explanation that fits together in harmony". If you follow that idea to its logical conclusion and try to write it out as an explanation of lift, including the ideas of flow influence over a wide area and mutual interaction between pressure and velocity, what you arrive at is my "more comprehensive explanation" in my proposed revised version in my sandbox ]. The hard work is already done, including integrating the "one big" explanation with the simpler ones in the pedagogically favored order. | |||
:I'm sorry that your theory has apparently not attracted the attention you feel it deserves, but wikipedia is not the place to drum up notoriety. In fact it works exactly the opposite way - first the material must become notable, and only then does it warrant inclusion here. In other words, you need to do your PR work elsewhere first; come back when you have the requisite citations. I'll repeat myself, in case you missed it above: | |||
My proposed revision also attempts to put the mathematical theories and the various qualitative explanations in perspective in the new sections "The understanding of lift as a physical phenomenon", "Popular physical explanations of lift" and "Shortcomings of the popular explanations". Not all the material in these sections is new, but I think organizing it in this way makes things clearer. It explains the science in a way that would prevent misunderstandings like the one expressed by ], and it provides the necessary "meta-analysis" of the qualitative explanations. ] (]) 22:33, 17 April 2013 (UTC) | |||
:From ]: | |||
:I get the science vs theology thing. For example, we know a lot about how gravity works, but we don't actually know why it works. We feel confident that there are such things as photons, but are there such things as gravitons? We don't know. But I think the explanation of lift should be much closer to science than theology. I strongly agree with the statements above that the article's explanation bends strongly toward circular reasoning: Why does the air move faster on top? Because there is lower pressure. Why is there lower pressure? Because the air is moving faster. This circular reasoning really turns off the layman reader, and I think it is reasonable to ask science to avoid this kind of circular reasoning without resorting to theology. The air on top is being made to both go faster and become lower pressure, but why? The best I can figure is that it is some sort of combination of surface cohesion for the molecules closest to the top of the wing, and a whiplash effect for the molecules a bit further away from the wing. This surface cohesion and whiplash combo creates both the lower pressure and faster airflow on top. Is this correct? | |||
::Misplaced Pages articles should be based on reliable, published <b>secondary sources</b> and, to a lesser extent, on tertiary sources and primary sources. <b>Secondary or tertiary sources are needed to establish the topic's notability</b> and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors. | |||
:One very clear problem with your edits is that you haven't established ''notability''. Feel free to come back when you can. ] (]) 21:30, 1 August 2021 (UTC) | |||
:I think the authors of this article need to realize how uniquely odd this article is in beginning the explanation with the "There are several ways to explain..." paragraph. I challenge you to find any other scientific article on Misplaced Pages that starts an explanation in this way. For example, look at the Misplaced Pages articles on nuclear fission or freezing. The explanation is straightforward and does not wade into this "several different ways" explanation. --] (]) 04:50, 30 January 2014 (UTC) | |||
The only reasonable thing to do is to subject New Theory of Flight to scrutiny by some expert such as Doug McLean. My case is strong because I have hard evidence published in leading journals, while the Misplaced Pages article on Lift (force) is very weak as made very clear in the Talk statement above by Doug. The Misplaced Pages article starts out with (see also ): | |||
::I was not saying that the current article "bends strongly toward circular reasoning", and I don't think it does. What I was saying is that the article should be revised so as to state explicitly that the cause-and-effect relationship between pressure and velocity in an airfoil flow is circular. Circular cause-and-effect is not the same thing as "circular reasoning", which generally refers to a false argument that purports to establish something that was assumed a priori and for which there is no support other than a circular argument. The circular cause-and-effect relationship between pressure and velocity in fluid flows isn't in the circular-reasoning category because it's the way the physics actually works. | |||
"There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift". | |||
This is very serious disinformation Mr Swordfish. Very serious. You apparently agree with the statement above by Anderson: "There is actually no agreement on what generates the aerodynamic force known as lift". You thus know very well that there is no scientific explanation of lift agreed to be correct (only incorrect ones agreed to be incorrect), yet you let Misplaced Pages inform the people of the World that there is one, or even better that there are many although most (all?) of them are incorrect. You must understand that this against the most basic of all Misplaced Pages principles your refer to: Misplaced Pages should not mislead the people. Who is telling you to do that? To cover up what is a fact reported by experts in serious media. | |||
::Of course Newton's second law is the key physical principle here. In many applications of Newton's second law, it's appropriate to think of the force as the "input" and the motion as the "output", but that way of thinking misses part of the picture in continuum fluid flows. The motion of a local parcel of fluid does depend on the net force exerted on it by all the adjacent parcels in contact with it, consistent with Newton's second law. But that force depends on the motions of the adjacent parcels, which depend on the motions of the parcels adjacent to them, and so on. Because we're dealing with the motions of many parcels, all interacting with their adjacent neighbors, we effectively have a situation in which the motions depend on the forces, and the forces depend on the motions, i.e. circular cause-and-effect. | |||
I want to bring this case to highest level at Misplaced Pages. It is very serious and of great concern to the people. How do I proceed?] (]) 06:54, 2 August 2021 (UTC) | |||
::So of course science should avoid circular reasoning, but circular cause-and-effect between pressure and velocity is a fact of life in aerodynamic flows, and a good qualitative explanation of lift needs to make that clear. | |||
::'''User:SecretofFlight''': To bring this case to the highest level of knowledge of physics at Misplaced Pages you should take it to the Physics Project team (see ]). You can do this by posting your case at ]. ] ''(])'' 12:31, 2 August 2021 (UTC) | |||
::One way to summarize the relationship between pressure and velocity is as follows: The pressure gradient causes a fluid parcel to accelerate (consistent with Newton's second law), and the combination of the parcel's inertia and acceleration causes the pressure gradient to be sustained. The necessity of acceleration to sustain the pressure gradient involves Newton's third law. When the pressure gradient is nonzero, a fluid parcel experiences a net pressure force exerted by it's neighbors. A net force on a fluid parcel can exist only if the parcel pushes back, consistent with Newton's third law. In the effectively inviscid flow outside the boundary layer, a fluid parcel can push back only through the combination of its inertia and acceleration. | |||
::Another course of action, which will more likely bring it to the attention of the "highest level", is to raise the issue on one of the various noticeboards. There is a process for resolving disputes that cannot be resolved on the talk page, and I think this one qualifies. See https://en.wikipedia.org/Wikipedia:Noticeboards#List_of_Wikipedia's_noticeboards ] (]) 13:47, 2 August 2021 (UTC) | |||
Thanks for this information. I will now prepare material to take the case New Theory of Flight vs Misplaced Pages Lift (force) to the Physics Project Team and also to Noticeboards.] (]) 16:02, 2 August 2021 (UTC) | |||
::I'll admit that the idea that the parcel's acceleration "sustains" the pressure gradient isn't that east to grasp intuitively. Does "sustain" mean the same thing as "cause" in this case? I think the answer is yes, but a bit indirectly. I found it helpful to think of a simple example from solid mechanics. | |||
:Please post a link here when you have filed your case(s). Thanks. ] (]) 19:11, 2 August 2021 (UTC) | |||
::{{ping|SecretofFlight}} When a dispute exists a User will sometimes post their case in two different places on Misplaced Pages. When this is realised one of the posts gets deleted promptly so Misplaced Pages’s effort is not divided into two places, potentially producing an ambiguous outcome. I suggest you post first on the Project Physics Talk page and see what happens. If you don’t see a suitable outcome after, say a week, then take it to a Dispute Resolution site. If you post at the Dispute site first it is highly likely that you will be asked to raise the matter first with the subject specialists at Project Physics so they have the opportunity to contribute their views, and their views will be highly valued by others who are trying to arbitrate on any dispute. ] ''(])'' 22:26, 2 August 2021 (UTC) | |||
:::Seems to me that {{ping|SecretofFlight}} has larger issues with how wikipedia makes these kinds of editorial decisions than what is within the normal set of issues that ] deals with. I'm not sure which noticeboard is the best venue to adjudicate this dispute, but my sense is that he will receive a more thorough response at the noticeboards than at ]. But I'll leave it up to him to choose the venue. ] (]) 02:14, 3 August 2021 (UTC) | |||
{{ping|Mr. swordfish,Dolphin51}} Before I take the case further I pose the following basic questions connecting to e.g the Scientific American article with headline "No One Can Explain Why Planes Stay in the Air. Do recent explanations solve the mysteries of aerodynamic lift?" (i) Is this a correct description of the state of the science of lift according to Misplaced Pages? If not, what is incorrect? (ii) Is there an accepted scientific theory/explanation of the generation of lift at small drag of an airplane wing? If yes, which is this theory/explanation? | |||
(iii) Mr. Swordfish states above "It is true that there is no simple, correct, and complete theory of lift". Does this mean that there is a non-simple, correct and complete theory, if so which, or no such thing? (iv) The Misplaced Pages article starts out: "There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift". There seems to be a contradiction between (i)+(ii)+(iii) and (iv), that is a contradiction between the statements (a) There is a commonly accepted scientific explanation of lift, and (b) There is no commonly accepted scientific explanation of lift. Which of (a) and (b) is the view of Misplaced Pages? I want a clear answer, not handwaving that (c) they are both correct since there are many theories carrying different elements, some true some false. It is against this background the New Theory of Flight stands out as the first explanation in both mathematical and physical terms of the generation of lift at small drag of a wing with solid documentation in the scientific literature, which you remove from visibility on Misplaced Pages. The matter is serious. The role of Wikepedia is to give correct information to the people, not double messages that there both is and is not a scientific explanation of lift. Ok?] (]) 06:57, 3 August 2021 (UTC) | |||
:My views on this matter, and my answers to your questions, are all evident in the posts I have made to this thread. I suggest you take your case further. I will respond there. ] ''(])'' 12:40, 3 August 2021 (UTC) | |||
::Think of a square block of wood, a couple of inches on a side, resting on a rigid table. Center your thumb on the top of the block and press downward. The forces exerted on the external surface (your thumb pushing down on the top and the table pushing up on the bottom) cause the stress field throughout the interior of the block to be altered. For one thing, there will be a non-uniform distribution of vertical compression stress, likely more concentrated directly under your thumb and more spread out at the bottom of the block where it presses on the table. This will be balanced by a non-uniform distribution of shear stress such that the net force on any parcel of material in the interior is zero, consistent with Newton's second law. At the local level at any point in the interior, the only cause we can identify for the compression-stress gradient is the shear-stress gradient. Locally, the two stresses are engaged in a mutual interaction, i.e. circular cause-and-effect. At the global level (the whole block), the cause of the whole non-uniform compression-stress field is the forces applied at the surface. There is circularity at this level as well because the distribution of compression stress applied by your thumb depends on the deformation of your thumb, which depends on the distribution of stress. This is not circular reasoning, just circular cause-and-effect associated with a mechanical interaction. | |||
:I agree. We've both already responded to most of this upthread. I fail to see the utility in discussing it further here. ] (]) 13:43, 3 August 2021 (UTC) | |||
{{ping|Mr. swordfish,Dolphin51}} No, you have not answered my questions in your posts! To take the case further it is necessary to make the present standpoint of Misplaced Pages clear on the matter of scientific explanation of lift. You say you will respond in the next instance. I ask you to do this right away, so that we will not have to start all over again. You have a responsibility to all the readers of Misplaced Pages and to the scientific community you are representing to answer my questions. What are your answers? ] (]) 13:59, 3 August 2021 (UTC) | |||
::We can apply the same line of reasoning to an airfoil flowfield. Because the shear stress in most of the field is insignificant, the compression-stress gradient (i.e. the pressure gradient) acting on any fluid parcel must be balanced by fluid acceleration instead. At the local level, the interaction between the pressure gradient and the acceleration is mutual, or circular, just as it was with the two interacting stress gradients in the solid. At the global level, the cause of the non-uniform pressure field (and thus also of the non-uniform velocity field) is the force applied to the flow by the airfoil, acting at the airfoil surface. As in the case of the wood block, the pressure field in the flow is just a state of stress in the interior of the domain, resulting from the application of forces at the boundaries, and distributed in a manner consistent with the laws of motion throughout the field. | |||
{{ping|Mr. swordfish,Dolphin51}} If you are unable/unwilling to answer the most basic question concerning the article Lift (force) for which you have responsibility, a question of utter scientific importance, then you are not, as I can see, filling the role of a true Wikipedian, which I think will not be appreciated by Misplaced Pages when made clear in the next instance. Do you see my point? You say that answers are to be found in your posts on this thread. Then point me to them! The world expects clear answers. What are your answers?] (]) 14:34, 3 August 2021 (UTC) | |||
::I think this answers the questions that crop up a little later in the exchange between Westwind and Swordfish: Why does the flow above the upper surface follow a curved path? And why is there a pressure gradient associated with that curvature? At the local level, the answer is in the mutual interaction between pressure and velocity that I've already described. At the global level, the ultimate cause of the non-uniform pressure and velocity fields is the force exerted on the flow by the airfoil. This sounds unsatisfyingly circular because that force is just the equal-and-opposite reaction to the lift force that we're trying to explain. But that's how the physics works. The force exerted by the airfoil makes the flow non-uniform, and the non-uniform flow exerts force on the airfoil. The cause-and-effect is circular even at this global level, but it's all tied together by the facts that the airfoil shape and angle of attack impose a boundary condition on the velocity at the surface and that Newton's second law applies throughout the field. This is circular cause-and-effect, but not circular reasoning. | |||
{{ping|Mr. swordfish,Dolphin51}} You can choose between two roles as Wikipedians: (i) You can go to history by opening to a much needed scientific discussion on theory of flight with in particular new input from New Theory of Flight, in a situation where there is no commonly accepted correct scientific theory of flight and all current theories basically dating back more than 100 years, are known to both experts and people through popular science press, to be incorrect/incomplete. (ii) You can act as gate keepers with a cover up that for sure there are (many) theories of flight, that science is settled and that New Theory of Flight has no place on Misplaced Pages. Which role do you prefer? For help to come to a decision I invite you to with in particular the videos and . ] (]) 15:26, 3 August 2021 (UTC) | |||
::On a related issue raised by Westwind273, the following of the curved surface by the flow has nothing to do with "surface adhesion". Air molecules don't adhere in significant numbers to solid surfaces, and air can't be put in tension. The background atmospheric pressure is high enough that the pressure at the airfoil upper surface, though lower than ambient, is still strongly positive in an absolute sense. So the flow follows a curved path and is able to follow the convex upper surface because it is pushed from above by higher pressure. There is no pulling from below. And the following of the curved surface has nothing to do with viscosity either. ] (]) 19:45, 3 April 2014 (UTC) | |||
Here is state of art of standard fluid mechanics as expressed by Doug McLean in his book Understanding Aerodynamics concerning scientific understanding of lift: | |||
"So in one sense, the physics of lift is perfectly understood: Lift happens because the flow obeys the NS equations with a no-slip condition on solid surfaces. On the other hand, physical explanations of lift, without math, pose a more difficult problem. Practically everyone, the nontechnical person included, has heard at least one nonmathematical explanation of how an airfoil produces lift when air flows past it. Such explanations fall into several general categories, with many variations. Unfortunately, most of them are either incomplete or wrong in one way or another. And some give up at one point or another and resort to math. This situation is a consequence of the general difficulty of explaining things physically in fluid mechanics, a problem we’ve touched on several times in the preceding chapters." | |||
::If readers see circular reasoning when they are trying to find a satisfying explanation for lift, it is most likely because the question "Why does the air move faster on top?" is not a particularly serious scientific question. (I think the best answer to this question would be "Because air observes the laws of physics"; but this is unlikely to satisfy many of the people who ask "Why does the air move faster on top?") It is a bit like ]. Science is absolutely fascinated that the planets move in such a regular, repeatable and predictable manner that Kepler was able to postulate three laws that accurately summarise their motion; but science is not at all interested in the question "Why do the planets obey Kepler's laws of planetary motion?" If someone (presumably a layman) set about trying to give a fundamental explanation as to why the planets move in a regular, repeatable and predictable manner, it is my guess that he would end up presenting circular reasoning. | |||
::Similarly, the air moves around an airfoil in such a regular, repeatable and predictable manner that we can see its motion is consistent with ], the ], ] etc. If the air did not move faster across the top of an airfoil, it would demonstrate a flaw in these fundamental laws of physics. | |||
::The scientific approach to lift is firstly to select Newton's laws of motion or the Kutta condition or Bernoulli's principle, explain it in some detail and then present the phenomenon of lift on an airfoil as a practical example of Newton or Kutta or Bernoulli. If it is done in this way, the question "Why does the air move faster on top?" doesn't arise because the air moving faster on top is exactly what the Kutta condition predicts for airfoils and lots of other bodies with sharp edges. | |||
::If ] attempts to answer this question, or give the impression it is attempting to answer this question, there is grounds for amending the article to avoid that impression. ] ''(])'' 05:48, 30 January 2014 (UTC) | |||
We read that generation of lift of a wing is a secret deeply hidden in the Navier-Stokes equations with no slip (but uncomputable because of very thin boundary layer), while scientific understanding in physical terms is a difficult problem, apparently unresolved (as expressed in Proposed revision of simplified explanations of lift below). | |||
:::Dolphin, I'm going to disagree with you here. ''Why does the air move faster on top?'' is perfectly reasonable scientific question, and the article does explain it, although in a somewhat roundabout (but not circular) manner. It's not presented in this order in the article, but the pieces are there to fit together the following explanation: | |||
The New Theory of Flight reveals the secret of lift hidden in the Euler/Navier-Stokes equations with slip (without boundary layer and thus computable) in a description of slightly viscous incompressible flow around a long wing as potential flow modified by 3d rotational slip separation at the trailing edge into a turbulent wake, with potential flow generating large lift by attaching to the upper surface while gliding with very small friction as expressed by slip combined with 3d rotational slip separation at the trailing edge without the pressure rise of full potential flow destroying lift. | |||
::::''Why does the air move faster on top?'' | |||
::::Because there is a region of low pressure along the top of the wing. According to Bernoulli's principle when air flows into a region of low pressure it speeds up. This is because there is more pressure behind than in front which results in a net force on the air molecules. Consequently they accelerate to a higher speed. | |||
::::''Ok, so why is there a region of low pressure on top of the wing?'' | |||
::::''So, why does the air follow a path that is curved?'' | |||
::::It is deflected by the wing, with the geometry of the flow path dependent on the shape of the wing and the angle of attack. It's obvious why it is deflected downward by the bottom the wing - the wing is solid and there is nowhere else for the air to go. Along the top, the air follows the surface of the foil, resulting in a curved path. | |||
::::''Why does the air follow the surface of the foil instead of just continuing on in a straight line?'' | |||
::::At this point we're getting beyond the scope of the article, but this is usually explained using viscosity. | |||
In short: Standard CFD as Navier-Stokes with no-slip is uncomputable and hides the secret of lift, while Euler/Navier-Stokes with slip is computable and opens to reveal the true secret in a New Theory of Flight in the form of potential flow modified by 3d rotational slip separation. It is as simple as that. Details on ] (]) 07:48, 2 August 2021 (UTC). | |||
{{ping|SecretofFlight}} {{ping|Mr swordfish}} {{ping|Dolphin51}} I read "The Secret of Flight" paper and found the description to be compelling but somewhat hyperbolic in its claims. Although this material is not yet covered in secondary sources, it is not fringe, and it is recent and I think sufficiently strong to be included here in the article on lift. I've included a short description towards the end of the article, in Three Dimensional Flow, where it seems to fit best. Please consider keeping it, making changes, or delete it if you think this is not a valuable addition to the article, as I believe it is. ] (]) 21:52, 15 August 2021 (UTC) | |||
:::I don't think ''Why does the air move faster on top?'' is ''central'' to the topic of lift, so I wouldn't re-structure the article to answer it. But the answer is there if the reader is willing to hunt for it. And the reasoning is not circular. | |||
:{{ping|Dilaton}} Thanks for your thoughts on this one. I concede that this new theory might be regarded as sound in some quarters, and might one day be widely accepted among mathematicians as a theory of flight. At present I see nothing to suggest that it is sufficiently mature to warrant mention in Misplaced Pages or any other encyclopaedia aimed at a general audience. We have seen two attempts at describing what this new theory of flight looks like, but I am none the wiser. For example, expressions like: | |||
:::Regarding Kepler's laws of planetary motion, they can be derived from Newton's laws (including the law of gravity), although since Kepler died a dozen years before Newton was born he obviously didn't derive them that way. So a reasonable non-circular explanation of Kepler's laws would be to start with Newton and proceed from there - Kepler's laws are true because they are a logical extension of Newton's laws. Of course, this begs the question of ''Why are Newton's laws true?'', and the answer to that is that you've got to start somewhere and the reason we accept them (without a logical proof starting from more fundamental assumptions) is the millions of observations and experiments confirming them. | |||
:*''3D vortices''. There appears to be nothing on Misplaced Pages to explain 3D vortices so this expression cannot be linked to any existing article to enable the reader to find something about these vortices. (Is this just an alternative to line vortex or vortex filament? Or is it somehow different?) | |||
:* ''potential flow modified by 3D rotational slip separation at the trailing edge into a turbulent wake''. This is inaccessible to a general audience. It looks like something from a PhD thesis. Misplaced Pages is not the place for such a thesis. | |||
:* ''the potential flow generates large lift by attaching to the upper surface while allowing a wing to glide with very small drag from turbulent vortex attachment at the trailing edge.'' Potential flow attached to the upper surface? Surely every application of potential flow around an airfoil since the time of d’Alembert has assumed the flow is attached to the upper surface, and to the lower surface as well? Sentences like this serve more to confuse than to explain. | |||
:If it is to earn a place in this article, it must be described in a way that a general audience might comprehend. Despite your best efforts, your recent addition to the article is unlikely to be comprehended by a specialist audience of fluid-dynamic-literate users, much less by a general audience. | |||
:My view is that your recent addition should be removed. I will wait to see what {{u|Mr swordfish}} and other Users think. ] ''(])'' 07:35, 16 August 2021 (UTC) | |||
::{{ping|Dolphin51}} Thanks for considering an addition. "3D vortices" is an attempt to convey that these are a collection of vortex filaments of unequal alternating vorticity, with ends attached to the trailing edge. It is essentially a more accurate refinement of the Kutta condition, in which the sheet of shear leaving the trailing edge is now understood as a sheet of turbulent vortices. The improvement of understanding comes in now seeing that this is where the majority of the drag originates on an airfoil. Perhaps the paragraph I attempted to add could be improved with this or other language? ] (]) 15:38, 16 August 2021 (UTC) | |||
:::All this said, I do agree that the various physical phenomenon surrounding lift (a net force, pressure differences, speed differences, air changing direction etc.) can be explained starting from basic principles. And I think the present article does this. ] (]) 15:54, 30 January 2014 (UTC) | |||
:Misplaced Pages policy is abundantly clear that there must be secondary sources to include material. So far, there has been none for the "new theory of flight" despite a decades long PR campaign that often spills over into Misplaced Pages. The academic article itself has been accessed about 720 times and has garnered a total of 6 citations in the literature. Now, it may be that as Dolphin says it "...might one day be widely accepted among mathematicians as a theory of flight." but for now it's not. I've removed it since it clearly does not meet the standards for reliably sourced material. ] (]) 14:48, 16 August 2021 (UTC) | |||
::{{ping|Mr swordfish}} I understand your concern and respect your adherence to secondary sources; however, ] does state that primary sources published in reliable places can be used with care, and I think this published article may thus qualify and be used carefully. Or we can do as you wish and wait for someone else to write about it. I do think that would be a bit of a loss, as the improvement of understanding of drag from attached vortices seems significant. ] (]) 15:38, 16 August 2021 (UTC) | |||
::::Mr Swordfish wrote: ''Because the air is following a path that is curved. Euler's equation, which is derived directly from Newton's laws says that whenever a fluid follows a curved path there are pressure differences, with lower pressure on the inside of the curve and higher pressure on the outside. The flow turning causes a region of low pressure along the top of the wing.'' | |||
:::{{ping|Dilaton}}While you are correct that primary sources may be used with care, there must be some secondary sources to support notability. At the risk or repeating what I posted upthread, Misplaced Pages policy on ] says: | |||
::::This is what I don't understand. Your explanation of the first and third questions here helped me a lot, but it is this middle second one that still seems unexplained to me. Specifically, why does air that follows a curved path have lower pressure on the outside? I know that Euler's equation says that it does, but why? Is it simply that the outside path is longer and therefore the molecules get spread out over a greater distance? This seems remarkably close to the equal-transit-time theory, which we know is false. Is the answer to this theology? I think it should not be. I read the Misplaced Pages article on Euler's equation for fluid dynamics, and it did not help me. --] (]) 20:37, 30 January 2014 (UTC) | |||
::::Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. '''Secondary or tertiary sources are needed to establish the topic's notability''' and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors. | |||
:::Here, we have a paper that was published five years ago and in response the world has shrugged. Now, perhaps it is truly the major scientific breakthrough that the authors claim it to be. Perhaps even you agree that it is and think that the world needs to be told about it. Fine. Go do that. But do it somewhere else. Come back when there are sufficient secondary sources to support the notion that it merits inclusion here. ] (]) 23:39, 16 August 2021 (UTC) | |||
:::::Sorry, I was being a bit imprecise. When I said "Euler's equation" I meant the one referenced in this article, which is different than the one treated at ]. So, it's unsurprising that that article didn't shed much light on it. Mathematically, the equation in question (dp/dr = rho*v^2/R) is derived by just writing an expression for centripetal force, applying F = ma and doing a bit of algebra. Babinsky's paper ( http://iopscience.iop.org/0031-9120/38/6/001/pdf/pe3_6_001.pdf ) has a concise derivation at the very end. | |||
I have to say that the sheer volume of debate on these talk pages leads me to believe that the Scientific American article was right after all. --] (]) 05:43, 1 September 2021 (UTC) | |||
:::::To get an intuitive notion of why it's true, ie why there is less pressure on the ''inside'' of the curve, imagine riding on a train between two cushions pressing equally on you from the sides - as the train goes around a curve, your body will press on the outside cushion and pull away from the inside cushion; less pressure on the inside and more pressure on the outside. The tighter the turn and the faster the train is moving, the greater these pressure differences become. The analogy only goes so far, but air following a curved path experiences the same forces. It's just a consequence of the centripetal force necessary to make the air follow a curve. ] (]) 22:28, 30 January 2014 (UTC) | |||
:The Scientific American article comprises two distinct elements: firstly there is the title “No-one can explain why planes stay in the air.” and secondly there is the body of the article. | |||
::::::Yes, this is what I was trying to understand. It is quite similar to what I was saying before. The overall airflow follows the curve of the wing on top because of the tendency of the air molecules to adhere to the wing, once they come in contact with it. But at the same time, there is a kind of whiplash centripetal force that is throwing the air molecules away from the top of the wing. The result is a powerful spreading out of the air molecules in the area above the wing, resulting in lower pressure there and the resulting lift. Does this sound right? Could the article be modified to give some kind of explanation like this to the layman? --] (]) 00:38, 31 January 2014 (UTC) | |||
:My impression of the body of the article is that it contains little to support the title. If you believe the body of the article contains some text addressing what the title says, please let us know what you see - please return to this Talk page and quote the wording you are looking at. Many thanks. ] ''(])'' 05:59, 1 September 2021 (UTC) | |||
== Proposed revision of simplified explanations of lift == | |||
:::::::There is no force "throwing the air molecules away from the top of the wing". However, there is inertia which would make the air follow a straight line in the absence of any force. Since there is a force pulling the air down towards the wing surface, the air changes direction. | |||
There is a proposal for a revised treatment of simplified explanations of lift available at | |||
:::::::I'm not sure what you mean by "a powerful spreading out of the air molecules in the area above the wing", but if you mean the air becomes less dense (fewer air molecules per unit volume) that is incorrect. In a first approximation, the air is ''incompressible'' meaning the density remains constant throughout the airflow. This is not strictly true since air does compress at sufficiently high airspeeds, but trying to explain lift via changes in air density is barking up the wrong tree. ] (]) 14:58, 31 January 2014 (UTC) | |||
https://en.wikipedia.org/User:J_Doug_McLean/sandbox | |||
::''I think the authors of this article need to realize how uniquely odd this article is in beginning the explanation with the "There are several ways to explain..." paragraph. I challenge you to find any other scientific article on Misplaced Pages that starts an explanation in this way. '' | |||
I think in general it is very good. I think it could be improved by addressing the following issues: | |||
::Two that come to mind immediately are ] which states: "The Bernoulli equation for incompressible fluids can be derived by either ] ] or by applying the law of ]" and ]. Granted, the latter doesn't call a lot of attention to the fact that there are dozens of different lines of reasoning that can be used to arrive at the result, it just presents them. The phrases "yet another" and "still another" occur numerous times. | |||
# The current article states "The downward turning of the flow is not produced solely by the lower surface of the airfoil, and the air flow above the airfoil accounts for much of the downward-turning action." This has been removed in the draft. I think it needs to be stated somewhere in the article, otherwise readers may come away with "skipping stone theory"; I'm not seeing a better place than its current location, but I could be persuaded otherwise. | |||
# it doesn't adequately present the streamtube pinching explanation. Probably most of us reading this are already familiar with this "explanation" which can be found in Anderson and Clancy, but the typical reader will probably have no idea what we're talking about. The current article does present it, and I think if we're going to include this material we should explain it more fully than the draft does. | |||
# it asserts : <blockquote>the "streamtube pinching" explanation also starts by arguing that the flow over the upper surface is faster than the flow over the lower surface</blockquote>That's not my understanding of the argument. In the current version of the article (<s>which I believe accurately reflects the reliable sources</s>) the streamtube pinching explanation starts with the fact that theory predicts and experiments confirm that the streamtubes narrow on the top of the wing, and proceeds from there. | |||
# it lumps streamtube pinching into an "incorrect" subheading, but I'm unconvinced that streamtube pinching is actually incorrect. My view, <s>which I think is born out by the reliable sources</s>, is that it is a correct description of the physical phenomena, but with the logical problem that it begs the question of why the streamtubes change size. | |||
# it claims that speed/Bernoulli explanations come in two basic versions, but there is a third: the half-venturi tube "explanation". There are probably others. I think this can be easily written around, assuming we don't want to drag half-venturi into the article, by replacing "These explanations come in two basic versions" with "There are two common versions of this explanation" | |||
# The final subsection "Alternative explanations, misconceptions, and controversies" is reduced to only one explanation, misconception, or controversy after moving previously contained material upwards. It might be appropriate to address half-venturi, skipping stone, "squeeze the soap" and others here. Or just remove this subsection. | |||
There are probably some other minor edits to avoid repetition and improve readability, but I think if the issues above are addressed the revised material will be ready for publication. Thanks for your efforts on this. ] (]) 00:42, 1 August 2021 (UTC) | |||
::A quick search or two ( https://en.wikipedia.org/search/?title=Special%3ASearch&profile=default&search=several+ways+to+explain&fulltext=Search , https://en.wikipedia.org/search/?title=Special%3ASearch&profile=default&search=multiple+explanations&fulltext=Search ) turns up thousands of wikipedia articles that present multiple explanations. Which is unsurprising, since there are usually several ways to explain any phenomena. Insisting on only presenting one when the literature presents several would violate ] ] (]) 16:25, 30 January 2014 (UTC) | |||
:::Hi Mr Swordfish. Thank you for taking the time to write such detailed explanation on the subject. I don’t have any major objection to what you have written. I think my only objection is that your explanations, regardless of their correctness, are not answering the question “Why does the air move faster on top?” but that is not because there is anything wrong with your answer; it is because the question is not a good one. | |||
:::Let me illustrate my thinking. Person A might ask “Why do ripe apples fall to the ground?” Person B might answer “Because of Newton’s law of universal gravitation.” Person A might be entirely satisfied with this answer, but I don’t find it a satisfying answer at all. Ripe apples were falling to the ground for many millions of years before Newton was born so Newton cannot possibly be part of the explanation of falling apples. (Science is fascinated that ripe apples, and all other unrestrained objects, always fall towards the center of mass of the Earth with predictable initial acceleration, but science has little or no interest in why.) | |||
:::I would prefer the conversation go like this: “We observe that ripe apples always fall to the ground. Is Newton’s law of universal gravitation consistent with this observation?” To which the answer is “Yes, Newton’s law of universal gravitation appears to be consistent with this observation.” (Albert Einstein made some observations and found that Newtonian mechanics were not consistent with the observations, so Einstein developed a replacement system of mechanics that more closely match his observations. The universe does not change its ways in order to behave in accordance with our laws!) | |||
:::In your explanation of why there is lower pressure on the inside of a curve than on the outside, you have strayed too close to suggesting it is because of Euler’s equation. The pressure gradient across curved streamlines existed for millions of years before Euler’s birth so Euler’s equation is not an explanation of why this pressure gradient has always existed. However, it is reasonable to say “We observe a pressure gradient across curved streamlines. Is there any scientific principle that matches this observation?” To which the answer is “Yes, Euler’s equation is consistent with these observations”. Euler’s equation has stood the test of time and we confidently use it to predict pressure gradients and the curvature of streamlines, but we should not imagine Euler or his equation is an answer to the question “Why is there a pressure gradient across curved streamlines?” That is not a sound question for a scientist. ] ''(])'' 06:23, 31 January 2014 (UTC) | |||
:Thanks for the feedback. To respond to the issues raised above: | |||
::::My background is mathematiics, so I'm used to working with axiomatic systems. To me, Newton's laws of motion are like axioms, and if I can deduce that something logically follows from the axioms I'm satisfied - "''why does X happen?'' because it's logical consequence of Newton's laws" - is a perfectly acceptable explanation of ''why'' in my book. I understand that not everyone will agree, and that I'll never get an answer to ''why'' the axioms (Newton's laws) are correct. | |||
::1. Yes, let's put this back. And let's find a source to cite for it. | |||
::::If someone asks me "why is the sky blue" or "why are there infinitely many prime numbers" or "why is a catamaran harder to tack than a monohull?" I'll try to give them an answer based on scientific principles and logic. I don't scold them for asking an unsound question, or say that we can never know ''why'' about anything. Agree that we can never ''really'' know ''why'', but we can explain complex things in terms of simpler, easier to understand concepts. Anyway, we've kind of gotten away from discussing the article, so I'll let you have the last word if you care to. ] (]) 15:47, 31 January 2014 (UTC) | |||
::2-3. I think the whole paragraph taken together describes the arguments correctly, but I see how it can be confusing if you look at the first sentence by itself. I'll try a rewrite. I don't support retaining the current article's opening statement on what experiments and analyses show. It's a true statement, but no reliable source I know of uses it in the context of a streamtube-pinching explanation of lift, and the current article cites no source for it. My objective is still to stick with the classical sources that propose a reason for the pinching, even if we end up pointing out that the reason doesn't make sense. | |||
{{od}}I have been grappling with the difficulty I see whenever Misplaced Pages pretends to answer scientific questions that begin with “Why” such as "Why does an airfoil generate lift?" | |||
::4. I agree with your comment on "versions". But I still think streamtube pinching belongs under the "incorrect" heading because its two main steps (streamtube pinching causes higher flow speed, and higher flow speed causes lower pressure) run opposite to actual physical cause-and-effect. In addition to not providing a good reason for the pinching, it has the flaw that conservation of mass isn't a satisfying physical reason why the flow would speed up. Really explaining why something speeds up requires identifying the force that makes it accelerate. I'll add the second "flaw". | |||
It is true that Misplaced Pages (and others) give answers in response to these questions but I don’t believe the question they are answering is the one beginning with “Why”. Superficially, it appears that an answer has been given to the Why question, but philosophically I doubt it. | |||
::5. The upper-surface-as-an-obstacle and the upper-surface-as-a-half-Venturi are really the same argument. Your rewording is OK with me. | |||
I would prefer it if Misplaced Pages answered the question “How does an airfoil generate lift?” It is easy to give a genuine answer to this question by referring to the flow pattern: | |||
:''When a symmetric airfoil is moving relative to the surrounding air but it isn’t generating lift, the flow patterns above and below the airfoil are identical. At each point in the atmosphere above the airfoil, the flow speed and air pressure are identical to the flow speed and air pressure at the corresponding point below the airfoil. The force of the air pressure acting on the top surface of the airfoil is equal to the force acting on the bottom surface. The two forces balance and no lift is generated. But when a symmetric airfoil is generating lift, the air is approaching the airfoil with a non-zero angle of attack and the flow pattern above the airfoil is significantly different to the flow pattern below the airfoil. At each point in the atmosphere above the airfoil, the flow speed and air pressure are different to the flow speed and air pressure at the corresponding point below the airfoil. In particular, the streamlines adjacent to the top surface are closer together than the streamlines adjacent to the bottom surface. The air is moving past the top surface faster than it is moving past the bottom surface and the force of the air pressure acting on the top surface is less than the force acting on the bottom surface. The two forces don’t balance and the resultant is called lift.'' | |||
I think this kind of response is an answer to the question “How does an airfoil generate lift?” rather than the question “Why does an airfoil generate lift?” Everyone agrees on the answer; it is the question that still perplexes us! ] ''(])'' 06:31, 26 February 2014 (UTC) | |||
::6. I'm going to try removing the "Alternative explanations..." subhead and move the "Controversy regarding Coanda effect" sub-subhead up with the flow-deflection explanation, as that's the explanation to which it relates. | |||
++++ | |||
The OP stated that humans do not understand why airfoils generate lift. | |||
I've implemented these changes in my sandbox. Thank you for the suggestions. ] (]) 17:23, 4 August 2021 (UTC) | |||
Now, "Humans understand lift" could mean several different things. The answer depends upon the meaning assigned to the proposition. | |||
: I have gone through the proposed text and I find it excellent, and an improvement over the current state of the article. I have a few minor language/typographic fixes in mind, which I think will be better carried out once the text is integrated in the article. -- ] (]) 07:09, 5 August 2021 (UTC) | |||
But the common interpretation in the scientific community isn't at all that vague. It might be stated: "broadly accepted scientific theory (in this case, mainly the laws of Newtonian fluid dynamics) accounts for the all the salient observed facts concerning lift, without arbitrary ad hoc assumptions, as confirmed by repeatable experiments." If we were to accept this interpretation, then it would remain only to ask ourselves, do we agree or not? I think that all experts on fluid dynamics would agree that the proposition is true. If so, then the article should reflect that accepted dogma, until and unless it is superseded by a new paradigm. | |||
:Thanks for your consideration of my suggestions. | |||
::1. I have added a citation for the assertion that the upper surface produces "much" of the lift. I'd like to find a better one, but I think this will do for now. | |||
::2. My working hypothesis is that the vast majority of our readers will not be familiar with the streamtube pinching explanation. It can be found in Anderson's ''Introduction to Flight, Eighth Edition'', but not in earlier editions (or at least I couldn't find it there), in Clancy's ''Aerodynamics'', and in Eastlake's article for The Physics Teacher. I have been unable to find it elsewhere. A year or so ago I was of the opinion that it was sufficiently obscure that it didn't merit attention in the article, but after acquiring Clancy and seeing it there, my opinion has changed. My best guess is that most people who have taken a college level class in aeronautical engineering have seen it, but it remains mostly unknown to the general population. | |||
::Since we can't expect the reader to already be familiar with it, we should provide a more detailed description - the current draft states "When streamtubes become narrower, conservation of mass requires that flow speed must increase." This is certainly true, but a sentence or two along with a picture will help many readers to understant ''why'' narrow streamtubes imply faster flow. | |||
It is understandable that some participants in the discussion are not experts: they don't know Napier's equation, they don't understand what it does and doesn't say about causality, they don't understand the relationship in science between theoretical models and experiments, etc. But the article should not reflect their ignorance...it should reflect humankind's current best understanding of the subject. | |||
::3. I think you are correct that the current article's treatment is at variance with the sources. Re-reading Anderson, he starts with "obstruction theory" to explain streamtube pinching, not "Starting with the flow pattern observed in both theory and experiments..." so we should present it his way. Eastlake doesn't explicitly explain why the streamtubes change size, but he alludes to the flow passing "the thickest part of the airfoil" and putting your thumb over the end of a hose, so I'll place him in the "obstruction theory" camp. I don't have my copy of Clancy with me and won't for several weeks, so someone else will need to check that reference. | |||
That's just my opinion. Do you agree? | |||
] (]) 00:33, 27 March 2014 (UTC) | |||
:I agree. | |||
:There is a temptation to imagine that to fully and clearly understand why airfoils generate lift, the explanation must be esoteric, complex, with lots of advanced math. There is no reasonable ground to imagine that. Different people will prefer different explanations of lift, and all those different explanations can be legitimate. For example, in one of John D. Anderson's books he goes looking for the simplest explanation of lift and concludes that it is based on the observation that the pressure on the upper surface of an airfoil is different to the pressure on the lower surface, resulting in an ]; lift is the component of the aerodynamic force perpendicular to the vector representing the relative motion between the airfoil and the free stream of fluid moving past it. That is a simple explanation but it is entirely legitimate as an explanation of how (or why) airfoils generate lift. Many people, including those who embrace Anderson's simple explanation, are entitled to object to the OP's suggestion that ''Humans do not fully and clearly understand why airfoils generate lift.'' ] ''(])'' 05:41, 27 March 2014 (UTC) | |||
::4. The authors of the current section must have been engaging in an act of charity to re-factor the streamtube pinching explanation so that it is not actually incorrect. Seems that we both agree that the current version is not actually incorrect, but it is different than what is to be found in the cited sources. Since the sources present the explanation as a result of obstruction, we should too. And when we do, I think it is appropriate to lump it under the "Incorrect" heading. | |||
+ + + + + + | |||
I agree that the science allows multiple formulations of explanation or presentation. This an inherent characteristic of Newtonian physics; it is a set of definitions, assumptions, and equations, and the equations can be transformed mathematically without changing their meaning. Often, for example, one can present the predictions of science, in a given case, in terms of forces, or alternatively in terms of energies. You can present Newton's original way of describing the evolution of a system, or you can use the form developed later, the law of least action, to describe the very same system evolution. As a final example, you can present Maxwell's laws in differential form or in integral form. Same science, same math, different presentation. | |||
::One thing I'd like to see carried over from the current article is | |||
But that is an entirely different question from that of presenting the explanation of lift as the result of net force on the body, as Anderson does. This is a *stage* in the explanation, not a *form* of the explanation. I think we would all agree that it is a necessary introductory stage. But it is only the beginning. Any curious reader will be happy to understand at this simple level but will immediately want an explanation of the pressure field and velocity field itself: "OK, I understand that if that is the velocity field, then that is the pressure field, and the conclusion is that there is lift. But now I want to know WHY those are the fields". The next stage, I think all of us would perhaps agree, is to proceed to a very simple model (called ironically "complex" potential) that accounts for a particular solution for the two fields that is consistent with lift (and an infinite number of others consistent with the boundary condition but NOT consistent with the observed lift!). But again a persistent reader will say, "ok, I see how ONE of the infinite number of possibilities yields the observed lift, but you have not explained why nature always settles on JUST THAT ONE, the one that happens to produce the observed lift." The next stage, I think you will agree, is to allow a slightly more realistic model...still far from the truth, still no turbulence, no separation, no chaos...but one which can account for the solution (Kutta condition, other approximations concerning effective shape of the foil rather than its actual shape) which nature has been proven experimentally to choose, very approximately. | |||
:::Sometimes a geometrical argument is offered to demonstrate why the streamtubes change size: it is asserted that the top "obstructs" or "constricts" the air more than the bottom, hence narrower streamtubes. For conventional wings that are flat on the bottom and curved on top this makes some intuitive sense. But it does not explain how flat plates, symmetric airfoils, sailboat sails, or conventional airfoils flying upside down can generate lift, and attempts to calculate lift based on the amount of constriction do not predict experimental results. | |||
A good explanation for this article, I think, would allow the reader to pick his own level of advance. If he didn't understand the first stage about net force, he could understand just that much and be satisfied to stop. If he had the next obvious question, he could get a clear exposition of that. If he still were curious, he could pursue the next level, which allows for friction and thus the Kutta condition. If he were still curious, he could move on to boundary layer, and then to turbulence, and then to separation, and then to chaos.... | |||
::The material expressed in the first sentence has been carried over, but the rest has not. Since the third sentence above is one of the better (best?) arguments why obstruction theory is lacking I think it makes sense to continue to include it. | |||
] (]) 00:36, 29 March 2014 (UTC) | |||
::5. Seems to have been taken care of. Thanks. | |||
== A major revision proposed to be installed soon == | |||
::6. Moving the Coanda material up and removing the depleted section on "Alternative theories" makes logical sense. My issue with this version of the draft is that the article now spends more time discussing what is essentially a semantic issue than it does treating the much more central idea of lift as a consequence of conservation of momentum. Moving the Coanda material down in the article would be an acceptable solution, but I'm not sure where to move it. Like the streamtube pinching explanation, I think the "Coanda controversy" is limited to folks who have done some formal study or aerodynamics and not widespread in the general population, so perhaps we don't really need to address it. Or perhaps find a more concise way to present it. | |||
Some of us have been saying for some time that this article needs revisions, to clarify the relationship between the mathematical theories and the qualitative physical explanations, to make clear the incomplete nature of the popular explanations, to offer a better explanation that emphasizes the spread-out nature of the flowfield and the reciprocal nature of the interaction between pressure and velocity, and so on. Over a year ago ] offered to take a "swat" at incorporating these last two points into the article, but it hasn't happened yet, so I'm proposing adoption of my own revisions, which do essentially the same thing Mr. Swordfish proposed, among other things. | |||
::Thanks for considering my suggestions. I think we're making real progress here. ] (]) 14:28, 5 August 2021 (UTC) | |||
A draft of my proposed revised version is in my sandbox ]. I've just made major revisions to it, and I think it's now worthy to replace the current article, but I hope others will suggest corrections and improvements, so I'll leave it for a few weeks before I install it in place of the current version. | |||
:::@Mr Swordfish: If at 3. you are alluding to the citation of Clancy p.76 “This lift force ... ... downward momentum of the air” I can confirm that this is an accurate quotation from Section 5.15 ''Lift and Downwash'' (which is on p.76 in my copy.) ] ''(])'' 00:19, 6 August 2021 (UTC) | |||
The reasons revisions are needed have been discussed at length on this page, by me and several others (Zapletal recently made some very good points), so I'll touch on them here only in summary form. | |||
::::@Dolphin: My recollection is that Clancy presents the streamtube pinching explanation, but I don't recall whether he starts with "obstruction theory" or proceeds from some other premise (e.g. the "theory & experiment" approach the article uses). We don't cite Clancy in this subsection, so you'll have to look beyond our citations. If you have your copy handy, I'd appreciate if you could take a look at Clancy's approach and report back. Thanks. ] (]) 18:18, 6 August 2021 (UTC) | |||
:::::@Mr Swordfish: I have had a quick look through Clancy. He explains lift using the Circulation Theory and the Kutta-Joukowsky theorem. The book appears to contain no linking of lift on an airfoil and stream tube pinching. There are several diagrams that show streamlines of varying spacing around a circular cylinder with circulation, and around an airfoil-shaped cylinder with different amounts of circulation. In the explanatory text adjacent to the diagram of the circular cylinder with circulation Clancy draws attention to the varying spacing of streamlines and links this to pressure variation using Bernoulli (Section 4.5 ''Circular Cylinder with Circulation'' on p.38) In the text adjacent to diagrams of airfoils Clancy makes no attempt to draw attention to streamline spacing and its implication for pressure. | |||
The proposed new version is longer than the current one, but I would argue that the additional material is needed to clarify the issues and avoid confusion on the part of the reader. If you don't think this kind of clarification is needed, just read the discussion on this page. The typical reader of the article is likely to be puzzled by some of the same questions that puzzle the participants in this discussion. Questions such as why the flow speeds up over the upper surface, why the flow follows a curved path, and why the pressure changes in the ways that it does. My draft attempts to make the answers to such questions clearer than they are in the current article. Read my draft carefully. If you find it leaves you with questions unanswered, let me know, and I'll try to fix it. | |||
:::::In para 4.5(b) Clancy writes “The effect of the circulation is generally to increase the speed over the upper surface of the cylinder and to reduce the speed over the lower surface. This effect is shown by the spacing of the streamlines in Fig 4.4” | |||
:::::In para 4.5(c) he writes “From Bernoulli’s Theorem, therefore, it follows that the pressure is generally reduced on the upper surface and increased on the lower surface. As a result, there is a net force vertically upwards. This is lift.” ] ''(])'' 13:49, 7 August 2021 (UTC) | |||
::::::I stand corrected about streamtube pinching appearing as an explanation of lift in Clancy. I'm now back to wondering if presenting this explanation here is giving it ]. ] (]) 14:17, 7 August 2021 (UTC) | |||
I've been re-reading the Help article on ], first in the context of the streamtube pinching "explanation", but then in the context of the apparent controversy over the Scientific American article that claims "nobody understands lift". The article on weight states | |||
::Neutrality requires that mainspace articles and pages fairly represent all significant viewpoints that have been published by reliable sources, in proportion to the prominence of each viewpoint in the published, reliable sources. Giving due weight and avoiding giving undue weight means articles should not give minority views or aspects as much of or as detailed a description as more widely held views or widely supported aspects. | |||
The proposed new version cites my own book, but I think the citations are relevant and not excessive, and thus in keeping with Misplaced Pages guidelines. | |||
The current version of the article states succinctly "...there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift." The proposed revision does an about face and states "...neither approach, by itself, is a completely satisfactory explanation." (And then there's the SA article, which I'm going to ignore as ].) | |||
The proposed revision preserves some later sections of the current article, with minor changes: "Pressure integration", "Lift coefficient". and "Lift forces on bluff bodies". Otherwise, the changes are major, and the headings are new. | |||
Both of these are valid opinions that are supported by reliable sources. I tend to agree with the latter as my own opinion, but when I put on my editing hat I find it problematical to clearly come down on one side or the other. If we're going to present this controversy, we're supposed to present both sides and "teach the controversy". That said, I don't want to waste our readers' time by rehashing the great Bernoulli v Newton debate that raged back in the late nineties. My preferred solution is to sidestep the issue and avoid sweeping statement about whether both are right, or neither is right, (or whether nobody really knows). The proposed revision clearly explains each approach and its limitations or shortcomings. I think the readers can draw their own conclusions without us having to make sweeping statements like the above examples. | |||
The title is proposed to be changed to "Lift (aerodynamic force)" to be less ambiguous. The introductory section and a new section, "Lift is a result of pressure differences and depends on airfoil shape, angle of attack, air density, and airspeed", describe what lift is and its general behavior, i.e. the "what" of lift, but without explanation of "how" or "why". | |||
I'll copy the present proposal over to my sandbox and make the proposed changes there so we retain an easy to access "clean" copy of Doug's proposal. | |||
Next, "The understanding of lift as a physical phenomenon" is an all-new section that tries to establish a key distinction that isn't clear in the current article, i.e. the settled status of the science compared with the less settled status of the qualitative physical explanations, to set the stage for going into the details in following sections. | |||
Regarding the streamtube pinching, or "obstruction theory", I'm in agreement that it's essentially the same argument as the "half venturi tube" approach, which seems to be more prevalent in the sources so we should give more prominence to it. I'll take a whack at that, along with an attempt to provide a more concise treatment of the Coanda material. ] (]) 13:44, 10 August 2021 (UTC) | |||
"Popular physical explanations of lift, and their shortcomings" covers much of the same ground as the current article, but the organization and most of the words are new. It integrates the explanations and their shortcomings into a single section to make the shortcomings more prominent. The "blind-men-and-the-elephant" problem is part of the folklore of explaining lift and thus should not be swept under the rug. I think this section, combined with the discussion in "The understanding of lift as a physical phenomenon", puts it all in perspective and equips the reader with enough background to avoid the common misunderstandings. | |||
:My view is that there are multiple explanations of lift, each derived from one or more of the various conservation laws and other laws of physics that are applicable to a solid object immersed in the flow of a fluid. We make use of multiple explanations of lift to serve the needs of the multiple audiences that have an interest in the subject. Even within one audience there are multiple purposes and objectives that cannot be satisfied by just one explanation. For example: | |||
"A more comprehensive physical explanation" is a shorter version of the explanation in my book, but with different graphics to avoid copyright issues. It does not incorporate Zapletal's suggestion to adopt Lanchester's "wave of sustenance" metaphor, because I don't regard the wave idea as helpful. To understand Lanchester's "wave", you have to go into the details of the interaction between the pressure and velocity fields, as my explanation already does. Once you've done that, I don't think the "wave" idea adds anything. The resemblance of an airfoil flow to a wave is superficial, not fundamental, it seems to me. | |||
:*An explanation of lift that can be presented to 19-year olds will be unsuitable for 13-year olds. An explanation that is both satisfying and satisfactory for student pilots will be unsuitable for students of physics and engineering. | |||
:*An explanation that helps explain lift in 2-dimensional flow will not be satisfactory if the objective is to help explain lift-induced drag. | |||
:I support the sentiment in the present article: “Either can be used to explain lift.” I don’t support the sentiment that "...neither approach, by itself, is a completely satisfactory explanation." It will be unhelpful, unnecessary and unsound to apologise for certain explanations of lift, or to suggest that no satisfactory explanation exists, or that no-one knows what it is. Misplaced Pages is able to demonstrate its maturity and soundness by not engaging in a search for a "completely satisfactory explanation". Nor should Misplaced Pages support a notion that every incomplete explanation must be incorrect. | |||
"Mathematical theories of lift" attempts to make the nature of the theories clearer without going into too much detail. It does not incorporate Zatletal's suggestion to get into the history of fluid mechanics. That might be a good topic for another article, but it would be out of place in this one. In this article I think it's appropriate to explain the physical principles involved, as currently understood, not the history of their discovery. | |||
:When we search for the most appropriate explanation of lift for our purposes we are engaging in applied science or applied math or engineering but we aren’t engaging in pure or fundamental science. Bernoulli’s principle and Newton’s laws of motion have universal application and so qualify as fundamental science, but an explanation of lift on an airfoil is simply one of many examples of Bernoulli and Newton in action. There will never be a Committee of eminent scientists whose task is to determine by arbitration the one true explanation of lift. | |||
"Lift of three-dimensional wings" is an all-new section that tries to remedy the current article's lack of information on lift in 3D. | |||
:When we talk about the explanation of lift based on Bernoulli’s principle, it would really be more accurate to say we are using lift as an example of Bernoulli’s principle in action. Similarly, when we talk about the explanation of lift based on Newton’s laws, it would really be more accurate to say we are using lift as an example of Newton’s laws in action. The pure science is always more fundamental than the application of that science to one of a multitude of everyday observations. | |||
"Viscous effects: Profile drag and stalling" explains how viscosity produces profile drag and limits the lift curve (stalling) in more detail than the current version. "Coandă effect is not relevant to explaining lift" takes a firmer stand on the relevance of Coandă and debunks the idea of a role for viscosity in the flow's ability to follow the upper surface. It also debunks the idea that the flow "sticks" to the upper surface and is "pulled down" toward it. | |||
:I look forward to seeing your latest proposal on your sandbox. ] ''(])'' 12:10, 11 August 2021 (UTC) | |||
The "Further reading" and "External links" sections have been shortened by the deletion of a few items that were less than helpful for one reason or another or already in the reference list. | |||
::Dolphin, Agree that different audiences require different explanations, and it is appropriate for us to present several, starting with the easier to understand and proceeding to the more rigorous. I think we need to be careful about using words like "satisfying" and "satisfactory" because they beg the question of "satisfying to whom?" My hunch is that most people are completely satisfied to know nothing about this topic. Those who bother to read the article may come away satisfied after a section or two, or they may read further until they are "satisfied". | |||
::Moving on.... | |||
::The opinion “Either can be used to explain lift.” is just that - an ''opinion''. So is the opinion "...neither approach, by itself, is a completely satisfactory explanation." If we're going to include either one, we need to present the other, present both as opinion, and provide some context for how widespread each is in the reliable sources. I'd rather not do that, especially early on in the article. Perhaps a later section on the "Bernoulli v Newton Controversy" would be in order, or perhaps a separate article instead. My preference is to just sidestep it as a distraction and present the various approaches, starting from simple and moving to the complex, with some context to address whatever shortcomings or limitations each approach has. And let the material speak for itself without making unnecessary sweeping generalizations. | |||
I look forward to constructive feedback and to getting these revisions installed. | |||
::To that end, I don't think we need the first section "Understanding lift as a physical phenomenon". The article starts with qualitative physical explanations without math and proceeds to the various mathematical models. That is apparent from the table of contents, so I don't think we need to state it explicitly; readers will get it if they bother to read that far. I'm going to remove it from my draft. Comments appreciated. | |||
::My view is that no version is 100% complete nor is any version 100% correct. When we do physics, we make abstract models, and in order to make the models tractable we make some simplifying assumptions along the way so the model doesn't exactly describe the actual physical phenomena. That doesn't mean that the models are bad, just that they are always limited, and when criticized for that variance the criticism is often warranted. For instance, 2D potential flow doesn't predict stall, drag, or downwash. But it does a surprisingly good job at predicting lift without making the math impossible. IOW, it's a good but limited model. | |||
::Which is to say that ''every'' explanation is incomplete to some degree. So, I'm not sure it's "fair" to label the explanation based on flow deflection and Newton's laws that way in the title. I do think it's fair to state that it's incomplete in the body, so I'm removing it from the title but leaving it in the body. | |||
] (]) 19:19, 23 May 2014 (UTC) | |||
::Regarding "Bernoulli-based" explanations, the two we discuss in that section are clearly incorrect. Correct explanations involving Bernoulli (or more properly, explanations that are based on models that have some predictive power) always include many other physical principles to the extent that it's a misnomer to call them "Bernoulli-based". To put a finer point on it, they always include conservation of momentum at some level. Bernoulli's principle is just one piece of the puzzle. | |||
:My apologies for not following through my promise to incorporate your proposed changes. I have not forgotten, but other matters have garnered my attention and this one went on the back burner. | |||
: |
::That said, I think a serious shortcoming of this draft as it stands is that readers may come away with the notion that Bernoulli's principle is somehow wrong, or that it is always incorrect to use it when explaining lift. I think we need so say something along the lines of "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." But I'm not sure where to put it or how best to phrase. Suggestions appreciated. ] (]) 18:32, 14 August 2021 (UTC) | ||
:::UPDATE: I've added "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." to the draft. ] (]) 18:49, 14 August 2021 (UTC) | |||
I've not gotten much feedback on the draft in my sandbox. I'm not sure if that's because other editors don't like it, or because they think it's fine as is. Assuming the latter, I'll give it a couple of days and if no objections I'll deploy the material in my sandbox. ] (]) 22:02, 19 August 2021 (UTC) | |||
:I will be happy to give some feedback in the next day or two. ] ''(])'' 22:42, 19 August 2021 (UTC) | |||
::Thanks. It's more important that we get it right than that we do it fast. But I want to keep the process moving. ] (]) 01:41, 20 August 2021 (UTC) | |||
:::It looks good to me and I don’t see much to comment on. I have provided my feedback at ]. ] ''(])'' 13:31, 20 August 2021 (UTC) | |||
I think the proposed new section "Understanding lift as a physical phenomenon" is important. It clarifies the status of the qualitative explanations relative to the rigorous scientific understanding embodied in the mathematical theories. In so doing, it says a lot more than what a reader could infer from the TOC or what he would be likely to realize even after reading the entire article. I think it makes what follows much easier to understand. | |||
:Doug, | |||
I think we should keep the "Obstruction..." explanation. Anderson is a very prominent author, and this book is a prominent source. | |||
:I have now had a chance to read the proposed revision in some detail. | |||
I've put up a new candidate in my sandbox. It avoids the "satisfactory" wording and removes the value judgements from the headings. It also incorporates Swordfish's shortened version of the Coanda section and his separate subheads for "Equal transit time" and "Obstruction...". I added another subhead to separate out the issues common to both explanations that had been swallowed into the "Obstruction..." subsection. I also incorporated his wording on Bernoulli not being incorrect as a principle, with the added qualification that Bernoulli is applicable outside the boundary layer. Comments? | |||
:I think the revision is much improved from the one from last January and it is clear that you have put quite a bit of thought and effort into it. However, I still do not think it is an improvement on the current article, and would not support changing it out wholesale. Apologies for repeating myself, but the current article's structure is based on the work educators who have written about the pedagogy of explaining lift. As the American Association of Physics Teachers states: | |||
] (]) 19:21, 21 August 2021 (UTC) | |||
:I've copied Doug's latest draft over to my sandbox for the purposes of comparison. The diff is here: https://en.wikipedia.org/search/?title=User%3AMr_swordfish%2Fsandbox&type=revision&diff=1040264566&oldid=1039805588 I'll have more to say in a day or so. ] (]) 17:29, 23 August 2021 (UTC) | |||
::"At least for an introductory course, lift on an airfoil should be explained simply in terms of Newton’s Third Law, with the thrust up being equal to the time rate of change of momentum of the air downwards." | |||
Comments on the latest drafts (24 Aug 2021): | |||
'''o''' The first thing I noticed when looking at the diff was that the latest version from Doug is some 10,000 characters shorter. This is mostly refs that didn't make it over. I don't think it will be controversial to restore the refs, although some may be ripe for pruning. I'll restore all of them in my next draft, and if any are deemed to be unnecessary we can remove them on a case-by-case basis. | |||
:The decision to present the material the way it is currently ordered was informed by the AAPT and other peer-reviewed articles addressing pedagogy. My strong preference is to state early and explicitly that "lift is a reaction force" and explain it in terms of Newton's 3rd law. Any revision that presents a more complicated explanation ''first'' will not have my support. | |||
'''o''' Regarding the first section ], it reads to me as an opinion rather than a simple statement of fact. The current version of the article also includes the opinion that "Either can be used to explain lift." I prefer the simple factual statement in my previous draft, which I think adequately foreshadows the qualitative vs mathematical dichotomy to come. | |||
:I do recognize that a pressure based approach is favored by aerodynamic engineers, and surely that approach should appear in the article. We just need to start with the simpler Physics 101 explanation such as provided in Halliday and Resnick. | |||
:There are several ways to explain how an airfoil generates lift. Some are more complicated or more mathematically rigorous than others; some have been shown to be incorrect. Most simplified explanations follow one of two basic approaches, based either on Newton's laws of motion or on Bernoulli's principle. | |||
:You have written much that is of value that should be incorporated into the article. I have been remiss in not following through with my promised integration. I hope to have a first pass up in my sandbox in a week or so. ] (]) 21:45, 30 May 2014 (UTC) | |||
'''o''' I looked into other wikipedia articles that link directly to sub-headings, and only found one that would be affected by the current drafts. I added an anchor tag to that section. We should make sure that it makes it into the final version. | |||
'''o''' Agree to keeping the obstruction/constriction/streamtube-pinching explanation. While it's not nearly as widespread as the ETT fallacy, it seems to be common enough for us to reference it here (although I'd be open to an argument that it's not if anyone wants to make it). I think it's worth expending a single sentence on NASA's "Venturi tube" version of it since NASA's site may be the most widely read version. | |||
::I think the proposed change has lost the focus on explaining what lift is and why it happens - the proposed changes seem to focus more on giving a critique of various "simplified explanations". While there might be a case for having an article on that topic, putting it at the top of this article seems likely to add to the confusion of the typical reader of this article, rather than reducing it. ] (]) 22:43, 31 May 2014 (UTC) | |||
'''o''' I don't think labeling the incorrect explanation as "incorrect" is a value judgement. Seems to be simply a statement of fact, so I'd advocate restoring that in the titles. | |||
:::First for the response from ] (]). Thank you for the encouraging words. But I don't see the basis for your objection that my draft "presents a more complicated explanation first". I don't think it does. In "Lift is a result of pressure differences and depends on airfoil shape, angle of attack, air density, and airspeed" I do say that lift is a result of differences in pressure, but that's just part of describing what lift is; it's not explaining lift in terms of the physical principles involved. The first explanation presented in my draft is "Flow deflection", the same one advocated by the AAPT. | |||
'''o''' I like the additional subhead to address issues common to both - I wanted to do that myself, but couldn't come up with a good title. | |||
:::In the quote from the AAPT, they advocate explaining lift "simply in terms of Newton's third law", but then they equate the force to a "time rate of change of momentum". This is the domain of the second law, not the third. When you use both laws you should explicitly mention both, as my draft and the current article do. | |||
'''o''' I'm unconvinced that it's necessary to state that "Bernoulli's principle is applicable to the flow outside the boundary layer." at this point in the article. I think simply stating "Bernoulli's principle can be used correctly as part of a more complicated explanation of lift." is sufficient for the intended audience for this portion of the article. If we're going to address when Bernoull's principle applies and when it doesn't, that should wait until later in the article. | |||
:::So it seems to me that we've both followed the AAPT recommendation in spirit, if not to the letter. | |||
'''o''' Regarding "This explanation is correct as far as it goes but is incomplete. " I've come to agree with Dolphin's ] that "as far as it goes" is a colloquial idiomatic expression, that while common in the US may not be understood the way it's meant to by someone unfamiliar with the expression. If we were writing this for a US audience I'd advocate to keep it, but since we're writing for the broader English-speaking world I think the phrase should be excised. | |||
:::Regarding the structure of the article, I think it's important to present a sufficient description of "what" lift is before presenting explanations of "how" it works, i.e. how the principles of physics apply to it. The fact that lift is exerted in the form of differences in pressure is a key part of an adequate description, independent of any physics-based explanation as to how the pressure differences come about. | |||
We have two candidates for the material at this point: | |||
:This explanation is correct but it is incomplete. It doesn't explain how the airfoil can impart downward turning to a much deeper swath of the flow than it actually touches. Furthermore, it doesn't mention that the lift force is exerted by pressure differences, and doesn't explain how those pressure differences are sustained. | |||
and | |||
:::The current article muddles the distinction between description and explanation by presenting its explanations under headings that bill them as "description", i.e. "Description of lift on an airfoil" and "A more detailed physical description". | |||
:Flow deflection combined with Newton’s laws is a helpful way to explain some aspects of lift. It leaves some questions unanswered; it doesn't explain how the airfoil imparts downward turning to the flow, and it doesn't mention that the lift force is exerted by pressure differences. It doesn't explain how those pressure differences are sustained. | |||
:::Pedagogically speaking, describing something adequately before you present the physics-based explanations is just common sense. I doubt that the educators at the AAPT would object to the way I've structured things. | |||
I prefer the concise "correct but incomplete" phrasing, but could be persuaded otherwise. | |||
I'll merge the the latest draft from Doug with mine, incorporating the ideas above. Comments as always welcome. ] (]) 16:32, 24 August 2021 (UTC) | |||
:::As for explicitly stating that lift is a "reaction force", I don't think it's a good idea. It seems to me that the term is either misleading or practically meaningless, depending on how it's couched and understood. The first sentence of the current article's "Deflection" section, i.e. "Lift is a reaction force—an airfoil deflects the air as it passes the airfoil", is misleading because it implies that causing an acceleration is part of the definition of a "reaction force". After this misleading introduction, one has to study the subsequent sentences to get the straight story. Of course the correct definition of a reaction force has nothing to do with causing acceleration, as is clear in the article "Reaction (physics)" to which the reader is redirected in that first sentence. When "reaction force" is properly understood as simply a force that has an action/reaction partner in accordance with Newton's third law, the statement "Lift is a reaction force" is practically meaningless because the same can be said of any other force. If we were to keep this section of the current article, I would at least delete the first clause, "Lift is a reaction force". Then you'd have something close to my draft, but I think my draft is more clearly worded. | |||
==Oversimplification== | |||
:::So it doesn't seem to me that your objection to my proposed structuring of the article is justified, or that you've suggested any real improvement to my draft, at least so far. I think my draft represents a marked improvement over the current article, in both structure and content. Unless you or someone else suggests improvements soon, I'll go ahead and make the replacement. BTW, I've changed the proposed title to "Lift (fluid-dynamic force)" to be consistent with identifying "aerodynamic force" as a special case, as is done in the current article. | |||
The current version of that section still refers to Bernoulli's Principle as "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." This sounds great, but it isnt correct, as it is a (fairly significant) oversimplification of his work. In the context of aviation and aerodynamic lift, it is only accurate along a streamline where no heat is being transferred between the wing and the air. Does the cited work include this gross oversimplification? As importantly, does the gross oversimplification make the concept clearer to the reader? ] (]) 08:26, 23 August 2021 (UTC) | |||
:{{ping|PrimalBlueWolf}} Where you have written “but it isn’t correct ...” do you mean Bernoulli’s principle doesn’t correctly represent the reality; or our article doesn’t correctly reflect the principle described by Bernoulli? | |||
:::I disagree with the response by ] (]). Just focusing on a straightforward explanation sounds appealing in its simplicity. But given the history of multiple, mostly flawed explanations that have been presented to the public over the years, just presenting yet another explanation, without discussion of the earlier ones, would cause confusion. Given the history of this topic, context-setting is essential if confusion is to be avoided. Again, just look at the confusion manifested in the discussion on this talk page. My proposed revisions are intended to reduce this kind of confusion by providing context. | |||
:It is well known, and always acknowledged in reliable published sources, that Bernoulli’s principle doesn’t take account of viscous forces within the fluid, nor does it apply to a flow field in which heat is being transferred. Despite these assumptions Bernoulli’s principle is a very powerful tool in analysing the subsonic flows around streamlined bodies. I don’t agree with your characterisation that the Misplaced Pages article represents a “gross oversimplification.” Please explain further. ] ''(])'' 13:57, 23 August 2021 (UTC) | |||
That it doesn't correctly represent the principle as represented in Hydrodynamica. The current version of the article alleges that you can determine velocity and pressure of any other point using Bernoulli's Principle knowing only the velocity and pressure of one point, and the velocity of one other point. That is only valid along a streamline, but the article doesn't acknowledge that. ] (]) 21:25, 23 August 2021 (UTC) | |||
:::] (]) 22:35, 3 June 2014 (UTC) | |||
:It is often stated that "Bernoulli's principle is only valid along a streamline" but this is a misconception. Within a flow field that exhibits uniform flow as the initial condition, BP applies throughout the flow field. This assumes that the energy is constant, i.e. it assumes no heat loss (as one would find in the example of an airplane wing) or no net work done (as one would find in the example of a sailboat). If one is going to pick nits, BP is not applicable to any real world airfoil due to these energy considerations, however it is commonly used as a ''approximation'' or ''simplification'' to make mathematical models tractable. Physics is full of these approximations, e.g. assuming sin(x)=x for sufficiently small x. And if we're not going to assume constant energy, BP doesn't apply along a streamline either. | |||
] wrote: ''Unless you or someone else suggests improvements soon, I'll go ahead and make the replacement.'' | |||
:The statement "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." is consistent with how BP is used in practice in mathematical analysis of fluid dynamics. Granted, it's a calculational shortcut that does not precisely model the actual physical world. But it's close enough for engineering work. Note that the section is about "simplified explanations" and is not the proper place for a long technical discussion of exactly when BP applies and when it doesn't. ] (]) 03:28, 24 August 2021 (UTC) | |||
I'm sorry, Doug, but that is not the way wikipedia works. The objective is to arrive at a ] that the proposed changes to the article are an improvement. Thus far, I have not seen any evidence of such a consensus here on the talk page, either with this iteration or the one you proposed last January. To issue an ultimatum that you will "go ahead and make the replacement" unless certain terms are met is at variance with the wikipedia processes. | |||
{{od}}{{ping|PrimalBlueWolf}} As you can see, I have moved your posts and the responses from me and {{ping|Mr swordfish}} to their own thread under this new heading. | |||
I agree with ]'s criticism above. | |||
You have written “That is only valid along a streamline, …” That is incorrect in the case of a wing generating lift in the atmosphere. Consider the following: | |||
Moreover, the proposed revision has other problems at the moment: | |||
In '''Fluid Mechanics''' by V.L. Streeter (1951 McGraw-Hill), section 3.7 ''The Bernoulli Equation'' says: | |||
*Major sections have no citations at all. (e.g. A more comprehensive physical explanation) | |||
<blockquote>The constant of integration (called the Bernoulli constant) in general varies from one streamline to another but remains constant along a streamline in steady, frictionless, incompressible flow. These four assumptions are needed and must be kept in mind when applying this equation. | |||
*Other sections have insufficient citations. | |||
Under special conditions each of the four assumptions underlying Bernoulli's equation may be waived. | |||
*Controversial assertions are made in a somewhat opinionated manner, with the only reference being to your book. This violates both ] and ] (e.g. Coandă effect & viscosity) | |||
1. When all streamlines originate from a reservoir, where the energy content is everywhere the same, the constant of integration does not change from one streamline to another and … may be selected arbitrarily, i.e. not necessarily on the same streamline.</blockquote> | |||
*In many places it reads more like a personal opinion than a neutral encyclopedia piece. | |||
In '''Aerodynamics''' by L.J. Clancy (1975 Pitman Publishing) section 3.4 ''Bernoulli's Theorem for Incompressible Flow'' says: | |||
I think it is a good article, but I don't think it is a good ''wikipedia'' article. I would like to continue to work towards incorporating some of it, and I'm hoping that you, I, and the other editors can work together to improve the current article . | |||
<blockquote>Further, at some distance upstream of the aircraft, the flow consists of a uniform stream. It follows that on any given streamline in this region the value of p + 1/2 ρ v<sup>2</sup> is the same as it is on any other streamline.</blockquote> | |||
In '''Fundamentals of Aerodynamics''' by John D. Anderson (1984 McGraw-Hill) section 3.2 ''Bernoulli's Equation'' says: | |||
At this point I'd like to solicit the opinions of other editors. What's your take? ] (]) 14:44, 4 June 2014 (UTC) | |||
<blockquote>For a general, rotational flow, the value of the will change from one streamline to the next. However, if the flow is irrotational, then Bernoulli's equation holds between any two points in the flow, not necessarily just on the same streamline.</blockquote> | |||
In the language of fluid dynamics we say Bernoulli's principle applies equally at all points on all streamlines in a region of ]. A wing operates in a stationary atmosphere so there are no viscous forces or vorticity in the air outside the boundary layers. The flow around a wing is irrotational everywhere except in the boundary layers. | |||
:Thanks for the response. I'm sorry about the ultimatum. I am appropriately chastised and won't let it happen again. Still, there's a lot about the current article that needs changing, and I'm eager to get things off top-dead-center. And I still intend to push for large parts of the article to be replaced, either by me or by others. | |||
You have also written “… only accurate along a streamline where no heat is being transferred between the wing and the air.” I assume you are referring to transonic and supersonic flow. The Misplaced Pages article presently only refers to lift in subsonic flight. In low-speed flight there is no significant amount of heat being transferred. ] ''(])'' 04:32, 24 August 2021 (UTC) | |||
:I can see now how I got on the wrong side of ] regarding Coanda and viscosity, and possibly on the popular explanations of lift. I've reworked those parts to take a more neutral point of view in the writing, while still making clear that there are reliable sources whose position is that some arguments are incorrect. When there are two opposing views on something, there is by definition a "controversy". But it doesn't follow that both views should be labeled "controversial". When one view is supported by the science (and can be verified as such by reliable citations), and the other is not, the physically sound view isn't controversial, to my way of thinking. In the case of the Coanda effect, the primary issue is the questionable use of a term, so I've labeled it "controversial". In the case of the purported role of viscosity in flow turning, it's not just semantics. On this one the science is clear, so I've labeled the "pro" statement a "misconception" and provided a citation of Milton Van Dyke, a leading authority on fluid-flow theory, whose mathematical analysis convincingly supports the "con" statement, i.e. it shows that viscosity plays no significant role in supporting flow curvature in boundary layers. In contrast, the sources for the pro side of this argument (Anderson and Eberhardt, and Jeff Raskin) provide only arm-waving statements with no mathematical support. In a case like this, it seems to me that not all sources should be given equal weight. | |||
I'm glad to take the correction and agree with the reasoning. Thanks for the detailed and well sourced explanation. ] (]) 07:19, 24 August 2021 (UTC) | |||
:I don't see how I've violated ]. As I've said, I think the citations of my book are relevant and not excessive. Boeing, with which I now have no relationship, holds the copyright, and I have no financial interest in the book's sales. And my book is not the only source I cite for the argument that Coanda is not relevant to lift. There are three others. So I think the citations are OK there, but I have revised that section to take a neutral point of view. | |||
== Proposed new version of simplified explanation continued == | |||
:You wrote "Major sections have no citations at all. (e.g. A more comprehensive physical explanation)". I'm sure there are places where more citations would be good, but I found no section that had none at all. "A more comprehensive physical explanation" cited my book in the opening paragraph. In one sense that should be sufficient, since everything in the section can be found in that reference. This explanation of lift is my original work, but it is not "original research" by Misplaced Pages's definition because it has a citable source. I know of no other source that has put all of these ideas together in one explanation, so if we're to include this explanation I think we have no choice but to cite my book. The constituent ideas (e.g. the spread-out effects of the airfoil on the flow, the reciprocal relationship between pressure and velocity, and the acceleration of fluid parcels by the pressure gradient), on the other hand, are all well established in fluid mechanics, and there are other sources that can be cited for them. I've added some and continue to look for more. If you see other places that could benefit from more citations, I'd appreciate it if you'd point them out specifically. | |||
The last thread had gotten rather long, so starting a new one. | |||
:] (]) 22:48, 5 June 2014 (UTC) | |||
Latest version now available in my sandbox.https://en.wikipedia.org/User:Mr_swordfish/sandbox | |||
I opted to keep the opening section, at least for now, but as it stands now there is substantial repetition between it and the first paragraph of the next section. Not sure what is the best solution, but I'm out of time for the day. Comments and suggestions appreciated. ] (]) 15:33, 26 August 2021 (UTC) | |||
::I don't claim that it is perfect, or even ready (yet) to replace the current article. Since it is a mash-up of two different articles the writing style varies a bit. It would be nice to address that. In particular, the cites from the current article are very "web friendly' with hyperlinks where available and brief quotations of the relevant supporting text. In the main article space the reader can mouse-over the footnote and see for him or herself the supporting material without having to go find a book in a library (unfortunately, the mouse-over feature doesn't work in a sandbox). It would be nice to flesh out the citations in the new material to take advantage of this feature. | |||
:I spent some time today looking at other Misplaced Pages articles on technical, mathematical, or scientific subjects. I came away with two observations: | |||
::Regarding ], I did not mean to accuse anyone of ethical lapses or attempting to profit off our efforts here. Merely that Misplaced Pages's COI policies are rather strict - an author citing his own work and unilaterally editing an article over the objections of other editors would be a problem. As long as it is a group effort with other editors involved we should be in the clear. | |||
#The articles discuss the topic at hand, rather than discussing the article and how it covers the topic. | |||
::Not everything from both articles made it into the integration. Arguments in favor of "restoring" certain sections cheerfully accepted. But when combining two rather long articles it's inevitable that some material would be cut. Perhaps more should be cut or moved to a separate article. | |||
#None of them have language that implies that the topic is difficult to explain or to understand. | |||
:With that in mind, the opening section "Understanding lift as a physical phenomena" would be an outlier in terms of Misplaced Pages style. The more matter-of-fact treatment in the section that follows is in keeping with wider Misplaced Pages standards. | |||
::Some material is repeated. Since we're not making a set of mathematical axioms or constructing a normalized database, repetition in itself is not a problem. But there are redundancies that probably should be removed. | |||
:See ], ], ], ], ], ], ] for a few examples. | |||
::So, I'm soliciting comment on this draft. Whether that happens here on this talk page or the talk page in my sandbox shouldn't matter. Since the proposed revision is a release candidate, edits in place are welcome. I'll continue to make edits over the next few days, then I'm on vacation for a while. I'm thinking maybe a target date of July 1 to get it in order and replace the current article, subject to reaching consensus here, of course. ] (]) 21:11, 10 June 2014 (UTC) | |||
:On that basis I'm going to remove the section from the draft while repurposing some of the language into the new first section. At this point, I think we have a release candidate. Comments? ] (]) 15:31, 27 August 2021 (UTC) | |||
== Integration of McLean's proposed changes and current article == | |||
::I agree. I encourage you to release the latest version. ] ''(])'' 13:35, 28 August 2021 (UTC) | |||
The integration is up in my user space at https://en.wikipedia.org/User:Mr_swordfish/Lift. Please make general comments here, and please start a new section for each specific topic so that we can discuss unrelated issues one at a time. ] (]) 21:49, 10 June 2014 (UTC) | |||
:::It's been released. Thanks to everyone who contributed. ] (]) 21:06, 28 August 2021 (UTC) | |||
:After spending only a few minutes looking at in-line citations I noticed that some merely nominate an author and a year; no page or section number, no title, no publisher etc. That standard does not meet Misplaced Pages's guidelines. For complex referencing tasks, I recommend ]] ''(])'' 01:08, 11 June 2014 (UTC) | |||
::Note that the author/date citations in the "Notes" section refer to entries in the alphabetized "References" list that give the title and publisher. True, some of them need to have a page or section number added. This is a format I've seen in the article on Navier-Stokes equations and in the Journal of Fluid Mechanics. I think the alphabetized list makes some things much easier for the reader, such as answering questions like "does this article cite Lanchester?" The "Notes" section is now a mixture of this new format and the original format. In the original entries that include quotes out front, author information is deeply buried and thus not so easy to find in a quick visual scan. A change that would be helpful, but would take some work, would be to put all the notes in a name/date/section/quote format and put all the all the other information on the references in the "References" list. ] (]) 20:01, 20 June 2014 (UTC) | |||
Sorry for not weighing in sooner on the latest changes. I've been away for a few days. | |||
==Proposed changes to early sections of the integration== | |||
I see that the proposed new section has been removed again and that some of the language has been "repurposed" into the following section. It seems to me that these changes have negatively impacted the article's organizational clarity. The first mention of the mathematical theories now comes under the heading "Simplified explanations.....", and with this placement the mathematical theories are now categorized as one of "several ways to explain how an airfoil generates lift". This isn't an accurate reflection of where the mathematical theories fit in the overall picture. The mathematical theories are the basis of the rigorous scientific understanding of lift. They're not "explanations" of lift. | |||
This integration is a good start. With this as a starting point, I'm proposing some moves and revisions for the early sections. I've installed them in my sandbox ] for your review, and I'll explain my rationale here. | |||
I think the proposed new section reflected the facts of the matter more clearly. Except for the phrase (referring to the simplified explanations) "and most readers will likely already have been exposed to one or more of them", which I propose we delete, everything that remains is a straightforward statement of fact. Even the one bit of "meta" information ("These issues are discussed in connection...") is a factual statement that more detail on the issues just raised is coming later in the article, not a "discussion" of "how the article covers the topic". | |||
I propose moving my new section "The understanding of lift as a physical phenomenon" back to a prominent position, just after the overview. It doesn't fit with the rest of the material in the "A more comprehensive physical explanation" section and would be much less effective there. Discussions over the years on this talk page have convinced me that there's widespread misunderstanding of the status of the hard science and how the qualitative explanations relate to it, so I think this context-setting section should come before the explanations start. I also propose adding words to the effect that the qualitative explanations cannot provide quantitative information for engineering. That's a property of all qualitative explanations, so I think it belongs here rather than in its current place as a limitation of flow deflection. | |||
I don't think that providing a bit of factual meta information is out of place in a Misplaced Pages article. Nor is it out of place to say that a correct qualitative explanation of lift is difficult, given that it's a statement of fact supported by the checkered history of qualitative explanations and by the sources (my TPT paper, at least). | |||
The integration's "Description of lift on an airfoil" section seems to me to mix explanation and description in a way that's not coherently organized and thus not as easy to follow as it could be (e.g. several of the subheadings under "Newton's laws: lift and the deflection of the flow" don't fit there.). I think the whole section could benefit from reorganization. | |||
I've tweaked the proposed new section and removed its heading, which makes it part of the "Overview" section, where I think it fits well. I've also taken a crack at removing the resulting duplication from the intro to "Simplified physical explanations..." in my sandbox. My recommendation is to merge these changes into the article in place of the recently released version. ] (]) 19:27, 2 September 2021 (UTC) | |||
So I'm proposing rearranging this as two main sections. The first is "Simplified physical explanations of lift on an airfoil", which gives the deflection explanation first, in keeping with the AAPT advice. I put the points covered by the current "Flow on both sides of the wing" in with the deflection explanation. I kept separate headings for limitations of deflection and Bernoulli, but I'm proposing changes to what's included in those sections. Failure to produce quantitative information is no longer a limitation of deflection, as it's been covered above. I also propose a change under the limitations of Bernoulli (see below). | |||
:Thanks for your continued effort on this page. I've made an attempt to merge your latest version with the current article. It's in my sandbox. https://en.wikipedia.org/User:Mr_swordfish/sandbox#Overview Comments appreciated. ] (]) 20:12, 4 September 2021 (UTC) | |||
I propose putting everything else in the current "Description..." section under "Basic attributes of lift", with the current "Summary" statement moved to the front, and keeping the subheadings other than "Flow on both sides of the wing", the main points of which are would now be covered under flow deflection. I'd really prefer to put this section between "Overview" and "The understanding of lift as a physical phenomenon", but putting it after the simplified explanations, so that flow deflection can come earlier, is a compromise I can live with. | |||
I |
::Mr Swordfish: I have no objection to the current version in your sandbox being released. ] ''(])'' 12:52, 6 September 2021 (UTC) | ||
:::Mr Swordfish: Your rendition of the addition to "Background" is more cryptic than my draft, but I'm on board with all of it except the last sentence, which seems to me to be ambiguous. Actually, I think all, not just some, of the simplified explanations we present have the flaw of leaving important things unexplained, even the ones that also have incorrect elements. A possible revision: | |||
:Apologies for taking some time off from this article. We didn't make the July 1st deadline, but hopefully we can get things moving again in the next several weeks. | |||
::::There are also many simplified explanations, but all leave significant parts of the phenomenon unexplained, while some also have elements that are simply incorrect. | |||
:I think the section https://en.wikipedia.org/User:J_Doug_McLean/sandbox#The_understanding_of_lift_as_a_physical_phenomenon is a fine section and don't disagree with anything in it. However, I do not think it deserves to be the opening section fight after the overview. I recognize that opinions may vary about this, but my issue is that the section is rather meta- that is, it talks about the explanation rather than simply giving it. At some point some amount of meta-analysis about the explanation is in order, but I prefer to cut to the chase and go right in to the explanation. ] (]) 20:29, 22 July 2014 (UTC) | |||
::I |
:::I think we're almost done and on the verge of completing a significant improvement of the article. ] (]) 00:54, 7 September 2021 (UTC) | ||
::::I have implemented the suggested change in my sandbox and will deploy that version. However, I failed to start with the latest version from the real article and several changes have been made since I deployed the version from my sandbox so I can't just do a cut and paste or it will override those changes. So, there will be several intermediate versions in my sandbox as I reconcile the two. ] (]) 13:46, 8 September 2021 (UTC) | |||
== Coandă effect criticism == | |||
==Proposed change to limitations of Bernoulli== | |||
The following sentence was recently added: | |||
Under limitations of Bernoulli, I propose deleting the third bullet item because it implies that the assumptions behind the steady incompressible Bernoulli equation are invalid for "real world airfoils" in general. Actually, for low-Mach-number steady flow outside the boundary layer in the reference frame of the airfoil, the Bernoulli equation is highly accurate, contrary to what this paragraph and its sources imply. Significant limitations to the Bernoulli equation apply only in circumstances different from those of the usual airfoil explanations (e.g. accelerating flow or high-speed flow). The arguments in the four cited sources are seriously flawed, and I can give you my detailed reasons if you wish to see them. | |||
:A criticism of the Coandă effect as an explanation for aerodynamic lift is that the Coandă effect itself is not well understood. | |||
I look forward to feedback on this proposed change. ] (]) 20:01, 20 June 2014 (UTC) | |||
With a cite to https://digitalcommons.usu.edu/cgi/viewcontent.cgi?article=1096&context=etd | |||
:I have no objections to this. I've implemented this proposed change in my version of the draft. https://en.wikipedia.org/User:Mr_swordfish/Lift#Limitations_of_explanations_based_on_Bernoulli.27s_principle ] (]) | |||
The relevant part of that paper says: | |||
==Proposed changes to "Mathematical theories"== | |||
<blockquote>The Coanda effect has been widely used in the both aeronautics and medical applications , air moving technology, and other fields. Nevertheless, this phenomenon is not completely understood, especially for three-dimensional flow as in the CSM design. The nature of the Coanda effect, with boundary layer separation and entrainment interaction, make for difficulty in solving the flow numerically and analytically.</blockquote> | |||
The integration makes some changes to the new section "Mathematical theories of lift". The added explanation of getting velocity vectors from CFD and then the pressure from Bernoulli isn't applicable to CFD in general, only to potential-flow methods. I've taken a crack at fixing that and at dealing with the repetition regarding the Kutta condition. | |||
I'm not seeing where the source ''criticizes'' the usage of the Coandă effect to explain lift, so this material appears to be ]. A bigger problem is that saying that "the Coandă effect itself is not well understood" is a very broad statement that would need stronger backing than the carefully worded excerpt from the cited Masters Thesis above. Reading the ] article I don't see anything supporting the assertion that it is not well understood - were this truly the case I would expect it to be treated in that article. | |||
I look forward to feedback on these proposed changes. ] (]) 20:01, 20 June 2014 (UTC) | |||
Of course, that wikipedia article is not dispositive - we're supposed to look at reliable sources, and other wikipedia articles are not reliable sources - but it strikes me that if we're going to publish a broad assertion like that the proper venue for discussing it and presenting the source material would be the talk page for that article, not this one. | |||
:I'm ok with this. I've replaced this section in my draft with the version from your draft. ] (]) 20:42, 22 July 2014 (UTC) | |||
I'm removing the material pending the production of better citations. ] (]) 20:32, 9 March 2022 (UTC) | |||
==Proposed deletion or substitution of two figures== | |||
:I agree with Mr. Swordfish that better citations are necessary. However, as far as I have been able to determine, there are no sources that offer a well thought out explanation for why or how the Coandă effect applies to aerodynamic lift. The popular references quoted in the main article (references 33 and 34) certainly do not offer that explanation. This lack of a source making a detailed argument for applying the Coandă effect to aerodynamic lift is not apparent in the main article. I tried to make this deficit of a source argument, not vey well I must agree, but one that should be made. It is difficult to make this argument since there are no referenceable sources that point out this deficit of a source offering a valid explanation. ] (]) 16:51, 10 March 2022 (UTC) | |||
The figure currently illustrating streamtube pinching, with the caption "Streamlines around an airfoil in a wind tunnel. ..." seems to me to be contradictory. The horizontal bars appear to be intended to represent wind-tunnel walls, but the streamlines don't appear to be constrained by the walls. And wind-tunnel walls are not relevant to the explanation anyway. I propose, as I show in my sandbox, replacing this figure with the flow animation, with a caption tailored to the streamtube pinching explanation. | |||
::Were I writing this article for myself, I'd include something like: | |||
:::People often try to explain why the air is deflected on the top of the wing by saying it's because of the Coandă effect, but this doesn't actually ''explain'' anything, it just gives it a fancy European name. | |||
::But I'm not allowed to just make stuff up on my own and I haven't seen this idea expressed elsewhere so I don't have a source for it. And that means I can't add it to the article. That said, I agree with the sentiment that it's poor pedagogy to explain something via material that the reader doesn't understand either. And I think the article would be improved with a short statement like the one above or something similar to what you added, but unless we can find reliable sources to cite we can't add it. If you find a good source for this I'm all ears. ] (]) 23:23, 10 March 2022 (UTC) | |||
Anderson and Eberhardt's "Understanding Flight" (McGraw-Hill, 1st ed. 2001) is the one source I know of that appeals to the Coanda effect in a lift explanation and also tries to explain how Coanda works in physical terms. They attribute the Coanda effect entirely to viscous "shear forces." On p. 23, after explaining no-slip at the surface and the resulting formation of a boundary layer, they say: | |||
:"The differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer. This causes the fluid to try to wrap around the object." | |||
This explanation of Coanda is easy to rebut. However, my own book ("Understanding Aerodynamics", Wiley, 2012) is the only citable source I know of that does so explicitly. With reference to using Coanda in lift explanations, I say in sec 7.3.1.7: | |||
:"The Coanda effect is erroneously seen as implying that viscosity plays a direct role in the ability of a flow to follow a curved surface. Anderson and Eberhardt assert that viscous forces in the boundary layer tend to make the flow turn toward the surface, specifically, as they put it, that the 'differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer.' Actually, there is no basis in the physics for any direct relationship between shear forces and the tendency of the flow to follow a curved path." | |||
In the paragraphs following the above, I explain in detail my reasons supporting the statement in that last sentence. The gist of it is that the curving of the flow is a result of the interaction between the pressure field and the velocity field, as we explain in the article under "A more comprehensive explanation." It has practically nothing to do with viscous or turbulent shear stresses. As long as the boundary-layer doesn't separate, the curving of the flow to follow the curved surface is an essentially inviscid effect. | |||
] has invited us to identify a citable source for his naming-isn't-explaining objection to relying on Coanda. Again, the only one I know of is my own book. In sec 7.3.2 I list things to avoid in an explanation of lift. Item 5 is: | |||
The figure caption "Uniform flow plus vortex flow (circulation) gives the total flow below" is not technically accurate. To get the flow around the NACA 0012 you would need to add a particular distribution of vortex strength along the chord (not just simple circulation), as well as a distribution of sources and sinks to represent airfoil thickness. I propose just deleting this figure. ] (]) 06:13, 21 June 2014 (UTC) | |||
:"'Naming' as a substitute for explaining, as, for example, in saying that a jet flow follows a curved surface because of the Coanda effect, where 'Coanda effect' is just a name for the tendency of jet flows to follow curved surfaces." | |||
So we have citable sources for a couple of possible additions to the Coanda subsection that would be of interest to some readers. I'm not enthusiastic about doing it, however, because I think we may already be giving Coanda more prominence than it deserves. On the other hand, I could argue that the article as it stands doesn't present enough of the case against Coanda, and that the additions we're considering here would balance things better and help justify the word "Controversy" in the article's section heading.] (]) 20:20, 3 April 2022 (UTC) | |||
:Thanks very much Doug. {{u|Mr swordfish}} and I will ensure your book is cited as a source where it is appropriate to do so in relation to Coanda effect. ] ''(])'' 23:49, 3 April 2022 (UTC) | |||
::Now that we have a cite I've been trying to craft language along these lines, but so far haven't come up with anything that doesn't seem out of place or unencyclopedic. I'll keep trying. Suggestions cheerfully considered. ] (]) 23:56, 11 April 2022 (UTC) | |||
:::{{u|Mr swordfish}} and {{u|J Doug McLean}} I have inserted a paragraph that, hopefully, begins to capture some of Doug's wisdom from above. See my . ] ''(])'' 04:41, 27 September 2022 (UTC) | |||
::::I have also added a sentence on "naming is not explaining". ] (]) 18:55, 28 September 2022 (UTC) | |||
== A new simplified lift explanation == | |||
:I agree that the diagram depicting streamtube pinching leaves something to be desired, but it is what's available in the public domain. That said, I think it does a better job of depicting streamtube pinching than the animated picture (https://upload.wikimedia.org/wikipedia/commons/9/99/Karman_trefftz.gif). Ideally, we'd find a better diagram. I'll see what I can turn up. | |||
As if things weren't complicated enough, I have developed a new simplified explanation for aerodynamic lift that I would propose as a add-on to the present version. I am looking for comments and recommendations at this point. | |||
:Agree that the other diagrams are not ideal either. The idea was lifted from one of Anderson's books, but I did the graphics and I'm a terrible graphic artist. I've deleted them from my draft since they may give a too-simplified impression. I do think that a picture representation of the idea of vortex flow + steady flow == total flow helps with a layman's understanding of circulation. But maybe it doesn't need to be in this article. | |||
The proposed text is available in my sandbox at https://en.wikipedia.org/User:David_Weyburne/sandbox | |||
:In coming days I hope to take a good look at both versions of the opening sections and attempt further integration. What would be nice would be to get a third (or fourth or more) editor(s) to help with this. ] (]) 20:58, 22 July 2014 (UTC) | |||
The proposed explanation is based on a graphical interpretation of the mathematical equations governing fluid flow. The key to the approach is the graphical plots of the velocity profiles and the pressure gradient profiles taken at a bunch of locations along the airfoil surface. This permits a one-to-one correspondence between the flow governing equations and the plotted profiles. By invoking the momentum conservation equation in this way, the explanation provides the connection between the velocity and pressure fields that is missing in the other simple explanations. ] (]) 13:38, 17 September 2022 (UTC) | |||
::I found a better picture for the streamtube pinching. ] I think this depicts it better than the animated diagram, and it doesn't have the issues you mention that the old/current picture have. ] (]) 14:14, 23 July 2014 (UTC) | |||
:Where a Misplaced Pages User develops a new explanation for something it is called Original Research. Such an explanation is not published in Misplaced Pages - see ]. | |||
== Release candidate? == | |||
:Your explanation cannot be described as simplified. I find it mystifying. Some of your sentences are statements of the obvious and therefore unnecessary in your description; and others are either incorrect or misleading. If you wish to continue with your work on this subject in order to publish it in an appropriate place, it needs a lot of refinement. | |||
:You are relying on four sources but three have been published by yourself. This is usually unwise and I have commented at ]. ] ''(])'' 23:20, 17 September 2022 (UTC) | |||
::Thanks for the feedback. As to original research comment: I do not think any of the explanations presented in the Simplified Explanations section would constitute original research that would be appropriate for a journal article. The explanation may be original but it is not something that can be tested and verified by other research groups. As to the rest of the comment: I am sorry you find it mystifying but I am hoping that is not the case for the majority of readers. You claim there are obvious statements that are unnecessary: I have tried to make the explanation readable for the non-expert and would hope that the expert reader would allow for that. You also claim there are misleading and incorrect statements: It is hard to comment on this claim since you did not bother to outline which statements are false or misleading. ] (]) 12:54, 21 September 2022 (UTC) | |||
:::{{u|David Weyburne}} Thanks David. On 18 September I made some introductory comments about statements I regard as superfluous, and others I regard as misleading. Those comments are on one of your Talk pages - see ]. ] ''(])'' 23:05, 21 September 2022 (UTC) | |||
I've spent some time further integrating Doug's draft into my draft, adopting much of his organizational structure and copying entire sections. At this point I think we have a release candidate. | |||
:::Sorry, I initially missed your comments in my sandbox. I appreciate your detailed comments and I have replied to the comments in the Talk section. At this point I will leave the explanation as is and would add that a more detailed explanation is available in the supplied references. ] (]) 12:40, 22 September 2022 (UTC) | |||
::One further note as to the observation that three of the sources were published by myself and is therefore inappropriate. I would point out that one is a YouTube video, another is an Air Force Technical Report, and the third is an e-book collection of my Air Force Tech Reports. All of them lay out a more detailed version of the condensed simplified explanation provided in my Sandbox. The reason the references are all mine is that I believe that my simplified explanation is original. However, as I stated before, this type of simplified explanation is not something that would be appropriate to be published in a standard journal. It is appropriate for providing a simplified explanation in an encyclopedia-style format. ] (]) 12:45, 23 September 2022 (UTC) | |||
:::As the author of the proposed cited articles you may be subject to ]. I would suggest familiarizing yourself with that policy. I appreciate the fact that you have disclosed that you are the author of those articles, but that fact remains and is germane and therefore not inappropriate. | |||
:::That said, the fact that the proposed additional material uses your articles as their source doesn't mean that the material can't be added to the article, or that your articles can't be cited. We've encountered this issue before with a prominent author, who provided some very valuable insights into this topic and helped improve the article. But he made very few edits himself, instead working with the other editors to reach consensus about any proposed revision to the article. I think we are on solid grounds if we follow that model. ] (]) 19:38, 23 September 2022 (UTC) | |||
::::Sorry, been busy. I understand that referencing my own work is problematic. To explain the reason for doing this, I need to give a little background. My simplified explanation for aerodynamic lift is based on showing "graphically" how the conservation of mass, momentum, and energy occurs for a flow around an airfoil. To do this, I start using a simple word-based argument to say that mass diversion results in velocity changes while being diverted around an airfoil. These velocity changes result in a speed up for the flow on the airfoil. How do you graphically show this speed-up? It is possible to use streamline, contour, or vector plots of the velocity but because of the large spatial variations, this approach is not very effective. Hence, most simplified explanations for lift regress to simply stating that "the velocity speeds up". For my simplified explanation I switched to a series of "velocity profile plots" along the airfoil. The profiles show the velocity behavior from a point on the airfoil to a point deep in the free stream above the airfoil. What you see are velocity peaks near the airfoil surface that slowly return to the free stream over distances of ~two chords. These peaks are important in that it gives a visual confirmation of velocity changes and give a one-to-one comparison to the momentum equation du/dy term. The momentum equation says these velocity changes must be conserved which is done, in part, by pressure changes. I then can show a plot of the pressure gradient profiles above and below the wing at the same location as the velocity profiles. The difference in the pressure profile areas, the pressure difference, shows graphically how mass and momentum conservation results in lift. | |||
::::So what is the problem, why do I only reference my own work? The reason is there is no one doing anything similar using velocity profiles. This velocity profile "peaking" behavior is not discussed or plotted anywhere in the literature that I could find (other than the simple text saying "the velocity speeds up"). Many textbooks show schematics of boundary layer profiles but not ones that show the peaks, the velocity speedup behavior. I observe it my airfoil simulations and in raw mesh data provided by other researchers, but nowhere in the literature. If I had references showing that these velocity and pressure profile peaks exist, I would be less dependent on referencing my own work. For the record, I think for the non-expert, my 15 min. graphics-based YouTube video does a better job of explaining this aerodynamic lift argument than my e-book version. | |||
::::I would be willing to work with any editor to resolve this issue. ] (]) 15:03, 23 March 2023 (UTC) | |||
== Recent changes to equal transit time section == | |||
The immediate question is whether it is an improvement over the current article. If so, we should replace the current article now and move forward with further improvements in-place. No article is ever "done" on wikipedia; refinements, additions, and improvements will likely be made in coming months and years. | |||
The diff is here: https://en.wikipedia.org/search/?title=Lift_%28force%29&diff=1228641725&oldid=1227711027 | |||
If the draft is not an improvement then let's discuss how to improve it so that it ''is'' better than the current article. | |||
I don't read the previous version as claiming that equal transit time never happens, only that it cannot be assumed. The "offending" passage is: | |||
My own opinion is that it's a stronger article. Many thanks to Doug for his effort and patience. | |||
:This is because the assumption of equal transit time is wrong. There is no physical principle that requires equal transit time and experimental results show that this assumption is false. | |||
By way of analogy, regarding flipping a coin we could write: | |||
The draft is at https://en.wikipedia.org/User:Mr_swordfish/Lift Please take a look and share your opinion here. ] (]) 14:02, 25 July 2014 (UTC) | |||
:This is because the assumption of it always landing heads-up is wrong. There is no physical principle that requires a coin to always land heads-up and experimental results show that this assumption is false. | |||
:Great work! I have had a quick look at the release candidate and left a couple of comments at ]. I will try to do more in coming days. ] ''(])'' 06:38, 26 July 2014 (UTC) | |||
I don't think that anyone would read that as claiming that coins ''never'' land heads-up, only that they don't ''always'' land heads-up. Likewise, ETT is not a general physical principle, but that doesn't imply that it never happens. I don't think we need this level of clarification and the recently added/changed language seems to me to make the section more difficult to read. Perhaps we could simply add a sentence to the effect of "ETT does occur in some situations, but when it does there is no lift." But I don't know that it's really necessary. I'll wait for other editors to weigh in before reverting the edit. ] (]) 14:24, 12 June 2024 (UTC) | |||
::I agree that it's a stronger article, and by that criterion it qualifies for release. But I'd still like to advocate for some further changes that I think would improve it further, if you'll bear with me. | |||
:Prior to my recent edit, Misplaced Pages’s emphasis was that equal transit time (ETT) is wrong, false, incorrect, misleading etc. In fact, the opposite is true. ETT represents the flow past most solid bodies. Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT. It is only lifting flows that don’t exhibit ETT. Let’s say 99% of flows around solid objects can be described as exhibiting ETT; and only 1% of flows cannot be described in this way. Saying “the assumption of equal transit time is wrong” is a statement that can be soundly challenged unless it is clear that it is confined to lifting flows. | |||
::The first has to do with the section "The understanding of lift as a physical phenomenon". We have agreement that it should be included, but not on where to put it. I still think it should precede the qualitative explanations because it seems to me that when things aren't put in perspective at the start, the article ends up giving a misleading impression. If you just "go right in to the explanation" as you prefer, the article gives the impression, intended or not, that that's how lift is understood, and that the rest, including the mathematical theory, is just filling in the details. I think that's a misleading picture of how we really understand lift. And I don't think that reading the meta-analysis later in the article, assuming the reader even gets that far, will be very effective in undoing the impression. Better, I think, not to give the impression in the first place. | |||
:ETT is a very simple 3-word expression. Doug McLean describes it as “an argument that is widespread in explanations aimed at the layman.” (See ''Understanding Aerodynamics'', section 7.3.1.4) A more sophisticated way of saying ETT is “the ] is equal to zero”. There are many reliable sources that talk about flows where circulation is equal to zero. | |||
:Prior to my recent edit, Misplaced Pages said {{tq|there is no physical principle that requires equal transit time ...}} This statement can be soundly challenged unless it is clear that it is confined to lifting flows. The ] is a fundamental theorem in the field of aerodynamics and it clearly implies that a non-lifting flow around a body must have a circulation of zero! Similarly it implies that if the circulation is zero, the lift will also be zero. For circulation equal to zero, the layman may read ETT. | |||
:Misplaced Pages needs to say that ETT does not exist around a lifting body or around an airfoil experiencing lift but we need to be careful to avoid versions of this statement that are so universal in their applicability that they can be readily challenged. It can be challenged if Misplaced Pages implies that ETT is inherently false, or universally inapplicable. ETT is the usual state of affairs, and it is only in the very narrow field of lifting flows that it does not prevail and cannot be assumed. ] ''(])'' 06:15, 13 June 2024 (UTC) | |||
::> ''Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT.'' | |||
::Is this true? Usually power lines, wires in fences, and flagpoles sway and move in the wind. What force is causing that movement? Do raindrops always fall straight down, or is there sometimes asymmetrical airflow that causes a horizontal force? | |||
::Flows with zero circulation are nice simple models so there are lots of textbook examples of that idealized condition. I'm highly skeptical that they occur in nature as the rule rather than the as a first order model in theory; for it to occur, I think you'd need to have the solid object be perfectly symmetrical, not rotating, and the airflow non-turbulent. Perhaps you can provide a reference for your 99% claim? Regardless, this tangent distracts from the main thrust of the section i.e. ETT is not a physical law like conservation of momentum, energy, or mass so it can't be assumed. | |||
::The previous version states that "the ''assumption'' of ETT is wrong". That's correct. And "There is no physical principle that requires ETT" That is also correct. We should stick by that. ] (]) 12:56, 13 June 2024 (UTC) | |||
:::Interesting article that addresses the history of ETT. It's not peer reviewed so we can't cite it as a reliable source, but worth a read. | |||
:::https://arxiv.org/pdf/2110.00690 | |||
:::'''On the Origins and Relevance of the Equal Transit Time Fallacy to Explain Lift''' | |||
:::Graham Wild | |||
:::School of Engineering and Information Technology, UNSW ADFA, Canberra, Australia | |||
:::G.Wild@ADFA.edu.au | |||
:::1st of October 2021 | |||
:::Preprint | |||
:::Not Peer Reviewed | |||
:::Abstract | |||
:::Recently, aerodynamics syllabi have changed in high schools, pilot ground training, and even | |||
:::undergraduate physics. In contrast, there has been no change in the basic theory taught to | |||
:::aeronautical or aerospace engineers. What has changed is technology, both experimentally and | |||
:::computationally. The internet and social media have also empowered citizen science such that | |||
:::the deficiencies in the legacy physics education around flight and lift are well known. The long- | |||
:::standing equal transit time (ETT) theory to explain lift has been proven false. If incorrect, why | |||
:::was it ever taught? Through a historical analysis of relevant fluid and aerodynamics literature, | |||
:::this study attempts to explain why ETT theory is part of our collectively lower-level cognitive | |||
:::understanding of lift and flight. It was found that in 1744 D’Alembert himself assumed this to | |||
:::be a feature of moving fluids, and while this initial intuition (ETT 1.0) was incorrect, the | |||
:::property of ETT (ETT 2.0) was derived in 1752 when applying Newton’s laws of motion to | |||
:::fluids. This incorrect result was independently confirmed in 1757 by Euler! The conclusion is | |||
:::that an over simplified treatment of fluids predicts ETT, along with no lift and drag. This then | |||
:::leads to the open question, can ETT be taught at an appropriately low level as an explanation | |||
:::for lift? ] (]) 12:51, 14 June 2024 (UTC) | |||
:::I don’t accept your arguments. I explained my arguments in significant detail but you haven’t engaged with that detail or responded to it adequately. For example, I have written about non-lifting flows and you have responded with a little original research suggesting that flows with zero circulation are non-existent or rare. | |||
:::If you wish, you could make a reasonable defence of the sentence I amended by arguing that the surrounding context makes it clear to all readers that the entire section, and the article, apply exclusively to lifting flows so if Misplaced Pages says {{tq|the assumption of ETT is wrong}} it is not referring to non-lifting flows. I won’t automatically buy that argument but perhaps I will eventually if it is explained persuasively. It is an argument that has much greater potential than the arguments you put forward in your previous edit. | |||
:::You have written “the assumption of ETT is wrong. That’s correct.” No, it’s not correct in the case of non-lifting flows. I have explained that in detail. | |||
:::You have written “There is no physical principle that requires ETT. That is also correct.” No, it isn’t correct. The Kutta–Joukowski theorem is a physical principle and it requires ETT in non-lifting flows. I have explained that in detail. ] ''(])'' 13:13, 14 June 2024 (UTC) | |||
::::I think we both agree that ETT is not a valid assumption for an airfoil with lift. I think we also both agree that there is a body of scholarship that does make the simplifying assumption of ETT in some specific examples. That doesn't imply to me that ETT is the usual state of affairs any more than the assumption of a ] implies anything about the shape or real-world cows. | |||
::::You assert that "ETT represents the flow past most solid bodies". But you have not provided a citation for that. I'm highly skeptical that this is true since just about everything moves and flutters in the wind. As Norman Smith's paper states: | |||
:::::...the claim that the air must traverse the curved top surface in the same time as it does the flat bottom surface...is fictional. We can quote no physical law that tells us this. | |||
::::That is, ''in general'' there is no physical law that requires ETT. That's not to say it never happens, or that no physical models ever make that simplifying assumption (and when they do, the result is zero lift). Whether "most solid bodies" exhibit ETT is somewhat orthogonal to this section, so perhaps we don't need to settle that here. I do think that the recent additions and changes are a distraction and make the section less readable. I'll take a look at improving the readability while keeping your concerns about overstating the invalidity of ETT. ] (]) 16:04, 14 June 2024 (UTC) | |||
:::::You and I both have a thorough understanding of the ]. I believe the expression “equal transit time” may be a layman’s way of saying the ] is equal to zero; I hope we agree on that. | |||
::The mathematical theory is the bedrock of human understanding of lift. The qualitative explanations are secondary, really just attempts to square the theory with our intuition. And that's a hard thing to do, given that the continuum flow in effect consists of innumerable little parcels of fluid moving in concert to get around the airfoil, each one obeying the 2nd law in a mutual interaction with its neighbors. The theory handles this complexity correctly by requiring the solution of a set of PDEs, but our intuition doesn't do so well when faced with an entire flowfield. For one thing, how the pressure field comes about in such a flow is very difficult to grasp intuitively. The popular explanations either avoid the question altogether (the deflection explanation) or do it badly (the Bernoulli explanations), and even my "more comprehensive explanation" is shaky on this point. | |||
:::::A small part of the problem is that ETT is not a well-defined or rigorously defined expression. To the best of my knowledge this expression is only used by authors who are repudiating this attempt at an explanation of aerodynamic lift. To the best of my knowledge none of the authors and institutions that resort to this naïve explanation of lift actually use the expression “equal transit time“; no-one actually asserts that “ETT” is true or correct. There are only people like us who assert that ETT is not correct (when applied to a body generating lift.) | |||
:::::Your quote from Norman Smith describes a body with “the curved top surface” and “the flat bottom surface.” He is not referring to “most solid bodies” - he is describing an airfoil! | |||
:::::I can supply a quotation from Anderson’s “Fundamentals of Aerodynamics” that will help on this topic. I expect to get access to my copy of Anderson within 7 days. ] ''(])'' 14:30, 15 June 2024 (UTC) | |||
::::::Agree that ETT is not well defined, and that it doesn't appear to be used other than by those repudiating it. Searching for the phrase (or even the word "equal") on my user page collection of works presenting ETT as correct only finds that in the references, not the actual works themselves. Similarly, the obstruction explanation is sometimes derisively referred to as "hump theory" but it's proponents don't use that phrase. | |||
::::::A typical turn of phrase is "The air moving on the top has to travel a greater distance in the same amount of time." or "Air flowing over the top has a greater distance to travel in the same time; that's why it flows faster." | |||
::::::I don't know that the expression “equal transit time” is a layman’s way of saying the ] is equal to zero, since I would surmize that those advancing the idea probably don't know what circulation is. That said, here's a source basically confirming that ETT and Γ=0 are the same idea.<ref>{{Cite book | title = Flight Physics: Essentials of Aeronautical Disciplines and Technology, with Historical Notes | date = 2009 |edition = 1st | publisher = Springer | location = | isbn = 1-4020-8663-6 | pages = 144 | quote = In conclusion, there is no possibility that the particles passing above and below the aerofoil would arrive simultaneously at the tail, except for the case that there is no circulation around the section – in this case, there is no lift on it. }} | |||
::::::</ref> | |||
::::::Regarding whether most flows around solid objects exhibit ETT, if that were true than ] and ] would not pose problems for engineers to overcome. | |||
::::::{{Reflist-talk}} | |||
::So I feel strongly that before we dive into the qualitative explanations, we owe the reader a heads-up on where such explanations stand in the overall scheme of things, and why. "The understanding of lift..." attempts to do this, but it may not be entirely satisfactory as it stands. It should perhaps be beefed up to make it clear that the difficulty of the problem dooms the qualitative explanations to fall short of being completely satisfying, not just that they don't produce numbers and that there's been disagreement on what to include in them. In my sandbox ] I've added a sentence to try to do that. | |||
] (]) 16:20, 15 June 2024 (UTC) | |||
:::Edits finished. Hopefully that addresses the concerns above. ] (]) 16:36, 14 June 2024 (UTC) | |||
::There are times when some meta-analysis up front makes things better for the reader, and I think this is one of those times. | |||
::::Your recent edit to the article is an acceptable alternative to my edits. Thank you for making those changes. | |||
::::The article now avoids giving readers the impression that ETT is inherently false. Hopefully readers can now see that the only falsehood is suggesting ETT exists in the flow around a ''lifting body''. ] ''(])'' 14:46, 15 June 2024 (UTC) | |||
:Thanks for the reference to “Flight Physics:Essentials ...” I was not aware of that publication. It looks like it might be essential! | |||
:Vortex induced vibrations are an oscillatory phenomenon. They become a problem in structures that have inadequate stiffness or inadequate damping. In our article on lift we are talking about steady flows with zero viscous effects, or only minor viscous effects. We use a reference frame attached to the airfoil or solid body so the consequences of oscillations of a solid body are way beyond the level of analysis we are using in this article, and related articles. | |||
:Could it be that after half a lifetime of believing that ETT is false, the work of the devil, it will take a major change of direction to accept that there is nothing false or distasteful about ETT? Could that be why you are finding reasons to deny the inevitability of flows in which circulation is zero, ETT prevails and lift is zero? ] ''(])'' 03:46, 16 June 2024 (UTC) | |||
::It's not that I don't believe lift can be zero (and that implies ETT). I just don't think it occurs as often as you seem to think it does i.e. 99% of the time a solid body is immersed in a moving fluid. That's because almost all real world objects are not perfectly symmetrical and that implies an asymmetrical air flow hence non-zero circulation. | |||
::Stated another way, ETT is not a valid assumption in general. If you assume ETT, you will get zero lift. I don't have a cite for this and I am willing to consider evidence to the contrary, but real-world airflows around solid objects with zero circulation are the exception rather than the rule. For instance, consider a symmetrical airfoil in a steady flow - it is well established that the lift varies by the angle of attack. For the special case of zero AOA, the lift is zero and ETT occurs (in this simple 2-d model). For all the other values there is lift, circulation is non-zero, and ETT is false. In mathematical terms, the set of values for which ETT holds has ]. That's about as rare as you can get without it being ''never''. | |||
::Perhaps there is some area of aerodynamic research that assumes ETT or decides that lift is small enough that lift is negligible - many treatments ignore viscosity, or compressibility for example - I'm not aware of any that assume zero lift, but maybe there are. Let me know if you know of any. ] (]) 13:00, 16 June 2024 (UTC) | |||
:::There are several elements of your edit on which I can comment but at present I only have time for one. I will comment on others later. | |||
:::You write about “real-world solid objects with zero circulation ...” Then you make a sneaky gear change and write about “a symmetrical airfoil ...” The two are very, very different in aerodynamics so your gear change doesn’t go unnoticed. Yes, a well-designed airfoil will produce lift (and lift coefficient and circulation) that varies approximately linearly with angle of attack. The feature of a well-designed airfoil that yields this desirable property is the sharp trailing edge. Clancy’s book ''Aerodynamics'' addresses the role of the sharp trailing edge and the way it causes vortex shedding to adjust the strength of the bound vortex to maintain the ]. I don’t have Clancy with me but I think it is Section 4.5 and/or 4.8 that contains good explanatory diagrams. | |||
:::In the absence of a sharp trailing edge, any change in orientation of a body is not accompanied by a change in lift (or lift coefficient or circulation.) For example, a cylinder with elliptical cross section, immersed in a flow produces little or no lift; altering the orientation of the cylinder doesn’t produce much change. What lift might be produced is due to asymmetric boundary layers and separated flow, rather than due to the primary flow predicted using an inviscid fluid. If a body doesn’t have a sharp trailing edge, and the orientation of that body is changed, the fluid flow adjusts itself so that circulation remains zero. Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge. Airfoils have sharp trailing edges, but real-world solid objects don’t. That is why the only circulation and lift that are observed on bodies without sharp trailing edges is the small amount caused by asymmetric boundary layers on the two sides of the body, separated flow and possibly other minor viscous effects. | |||
:::Scientists and engineers have to work hard to generate circulation and lift. Typically they use airfoils with thin, sharp trailing edges even though this feature is structurally weak and vulnerable. Flowing fluids are uncooperative - as they flow around bodies their natural state is doing so with zero circulation. Any change in orientation of a real-world solid body causes the fluid to change its flow pattern to avoid circulation developing. If it were not so, aircraft designers would use wings with thick, generously rounded trailing edges so they could get more fuel into the wings, use deeper and lighter spars, and have more room into which to retract the undercarriage. ] ''(])'' 16:18, 16 June 2024 (UTC) | |||
::::On the matter of the sharp trailing edge there is a very useful quotation by George Batchelor in the short article ]. | |||
::And the section heading should remain "The understanding of lift as a physical phenomenon", not "Understanding lift as a physical phenomenon". The former implies we're talking about the understanding held by the community at large (which is what this section is doing), while the latter implies a concentration on changing the understanding held by the reader. I think the difference is significant. | |||
::::There is also a useful quotation by Richard von Mises at ], reference number 4. ] ''(])'' 00:38, 17 June 2024 (UTC) | |||
::Next are a couple more issues with headings: | |||
::::The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation. Picture the wind blowing around such a body, and then the wind changes direction. Imagine that this change causes a circulation to begin in the flow. This circulation causes a lift force to act on the solid body. Newton’s 3rd law tells us that an identical lift force acts on the flowing air. When a fluid that is free to flow or change shape is subjected to a force or pressure it responds in whatever way will cause that force to diminish. Consequently the lift force on the air flowing around the solid body causes the streamlines, velocities and pressures to change to diminish the circulation that has just begun. This process can be expected to continue until all circulation has been eliminated. Only then has equilibrium been achieved within the flow pattern around the body. | |||
::The content in "Description of lift on an airfoil" isn't really description; it's explanation. I think "Simplified physical explanations of lift on an airfoil" is more consistent with the content. | |||
::::Any residual circulation and lift is not related to the primary flow as would exist in a geometrically similar situation but with an inviscid fluid. It is related to the secondary flow caused by viscous effects such as flow separation. Any residual lift is still accompanied by the original drag force. The lift to drag ratio is so small that this solid body doesn’t qualify as an airfoil. I believe this is an explanation for the operation of oddly shaped ] which glide without conventional wings. ] ''(])'' 05:22, 17 June 2024 (UTC) | |||
::I think the heading "Methods to determine lift on an airfoil" promises more than we deliver. To apply either "Lift coefficient" or "Pressure integration" you have to know something a priori that's tantamount to knowing the lift. So these are really just relationships for converting one form of knowledge about lift to another; they don't really "determine" lift. I propose deleting the heading "Methods to determine lift on an airfoil" and promoting "Lift coefficient" and "Pressure integration" to sections in their own right. | |||
::::I'm continuing this discussion since I think I may learn something. I'm not trying to be "sneaky", just trying to understand what evidence there is that zero-circulation/zero-lift/ETT is the usual or normal state of affairs rather than a rare exception. | |||
::::''>Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge.''\ | |||
::::Agree that Kutta condition requires a sharp trailing edge, because without one it's not obvious where the rear stagnation point occurs. And without that it's not clear how much circulation to apply to model the fluid re-joining at the rear stagnation point. But you don't need a sharp trailing edge to have an asymmetrical airflow with non-zero circulation, you just can't apply the Kutta contidion. As Gale Craig states, (paraphrasing) ''you don't need an airfoil shape to get lift, as anyone who has ever handled a sheet of plywood in the wind knows.'' Of course, if you want enough lift to fly a plane of propel a sailboat, you'll want something with ''more'' lift than a non-arifoil can provide. That doesn't mean only airfoils with sharp trailing edges can generate lift. | |||
::::I have sailed boats with rudders that have a rounded trailing edge. Performance is sub-optimal, but the rudder most definitely provides enough lift to steer the boat. When I look at leaves on trees or flags on a flagpole in the wind, they never settle down into an equilibrium of zero lift as you describe above. Spinning balls have lift, as any tennis player understands. Here in the US, there's a baseball pitch called the knuckleball where the ball is thrown with a little spin as possible, with the effect that it's impossible to predict which direction the lift will take the ball making it very hard to hit. So, my experience is quite at odds with your assertions. | |||
::::You say that "The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation." but don't provide anything to back that up. Along with your 99% figure, I would need some more to go on than your assertion. | |||
::::Agree that my examples above are anecdotal or original research. Here's an interesting treatment of bluff bodies which seems to be in conflict with your assertion that ''Circulation greater than zero requires the Kutta condition...'' | |||
:::::For bluff bodies, the interest is usually in the drag on that body, mainly because experiments have found that drag is the dominant force. This observation, however, does not imply that bluff bodies cannot produce lift because many do. Nevertheless, examining just the drag characteristics of such bodies is convenient in the first instance. Furthermore, bluff bodies may also produce pitching moments, which sometimes need to be known for certain types of engineering work, e.g., to determine torsional loads. | |||
::::] (]) 13:56, 17 June 2024 (UTC) | |||
:::::Here's an excerpt from another paper | |||
<blockquote> | |||
::Most of the material in the section "Kutta-Joukowski theorem" is now covered in "Circulation and the Kutta-Joukowski theorem" in the "Mathematical theories of lift" section. I propose integrating some material from "Kutta-Joukowski theorem" into "Circulation and the Kutta-Joukowski theorem", moving the description of the Magnus effect to "Lift forces on bluff bodies", and deleting "Kutta-Joukowski theorem". I've taken a crack at this in my sandbox ]. | |||
:::::Bluff bodies are obviously also subjected to forces in the across-wind direction and to | |||
:::::moments around the various axes due to non-symmetries of the pressure distribution on their | |||
::Then a few technical issues: | |||
:::::surface. Therefore, these loads depend fundamentally both of the body shape and on the | |||
:::::orientation of the incoming freestream. Particularly in the two-dimensional case, the force | |||
:::::component in the across-wind direction is often called lift force, in analogy to the | |||
:::::corresponding force acting on an aeronautical wing section (airfoil). | |||
:::::(elision of details about the starting vortex and consequential circulation around an arifoil) | |||
:::::Coming back to bluff bodies, the above described mechanism does not apply in all its | |||
:::::details, particularly because the boundary layer cannot remain attached to their surface even | |||
:::::after the end of the initial transient. However, if the body is sufficiently elongated (like an | |||
:::::ellipse), a starting vortex is shed anyway (even if not as strong as that of an airfoil), and the | |||
:::::asymmetry of the final flow configuration for non-symmetrical wind orientations may be | |||
:::::sufficient for producing significant lateral forces. | |||
</blockquote> | |||
::Under "Flow deflection and Newton's laws", the statement "The resulting force upwards is equal to the time rate of change of momentum of the air downwards" is problematic on two counts, in spite of the fact that it has a citable source. | |||
:::::Seems to me that if it were the case that almost all bluff bodies experience zero lift the paper would say that at some point. ] (]) 14:32, 17 June 2024 (UTC) | |||
:::::One of the frustrating aspects of discussing this subject is the variation in meaning given to the word “airfoil”. On these Talk pages I see the word used with three different meanings: | |||
::The first problem with the statement is that for it to be true, the downward force exerted by the airfoil on the air surrounding it would have to be the only force being exerted on "the air". There are many possibilities for how we can define the body of air we're considering, and this condition (no other force but the lift) isn't met in general. The airfoil exerts a downward force on the inner boundary of the body of air surrounding it (at the airfoil surface), but the surrounding environment exerts unbalanced pressure forces on the outer boundary of the body of air. This problem cannot be eliminated just by increasing all the dimensions of the "box" of air we consider, even to the limit of infinity. As the box is made larger, the pressure disturbances at the outer boundary get weaker, but the area over which they act gets larger, and the integrated force remains comparable to the lift. How much of the lift is accounted for by this pressure force rather than by momentum change depends on the proportions of the box. For example, for a box that is very large horizontally compared to its vertical dimension, practically all of the lift is accounted for by pressure at the outer boundary, and practically none by momentum changes. Only in the limit as the vertical dimension of the box becomes large relative to the horizontal is it true that lift is accounted for by momentum changes. | |||
:::::#A two-dimensional shape that can be employed in three-dimensional bodies to generate lift. For example, the shape known as NACA 2412 is an airfoil section commonly used for the wings of low-speed aircraft. | |||
:::::#A three-dimensional body that generates at least a little lift. Some Users point to an irregular body or a sheet of plywood or a sycamore seed and, noting that it experiences a small lift force, say “see, it is an airfoil!” | |||
::The other problem is that most such analysis in fluid mechanics deals with boxes whose boundaries are fixed in space. The time rate of change of momentum in such a box is zero in steady flow, and momentum changes must be assessed in terms of fluxes in and out, not the time rate of change. | |||
:::::#A three-dimensional body that, over a usable range of angle of attack, is capable of generating significantly more lift than drag. With this meaning, airfoils are manmade structures that have the generation of lift as their primary purpose. Airfoils are carefully designed and manufactured structures to ensure the lift-to-drag ratio is high enough to achieve its intended purpose. | |||
:::::Misplaced Pages’s current definition of airfoil closely matches No 3 above. ] says: | |||
::Thus the simple explanation in terms of flow deflection is correct only if it's couched in vague terms such as "for the airfoil to deflect the flow downward, it must exert a downward force on the air". The more specific statement "lift is equal to the time rate of change of momentum of the air" is not correct in general. I recommend deleting this sentence. | |||
:::::{{tq|When the wind is obstructed by an object such as a flat plate, a building, or the deck of a bridge, the object will experience drag and also an aerodynamic force perpendicular to the wind. This does not mean the object qualifies as an airfoil. Airfoils are highly-efficient lifting shapes, able to generate more lift than similarly sized flat plates of the same area, and able to generate lift with significantly less drag. Airfoils are used in the design of aircraft, propellers, rotor blades, wind turbines and other applications of aeronautical engineering}} | |||
:::::The layman imagines that the essential feature of an airfoil (meaning No 3) is its generously rounded leading edge, or its curved surface. In fact it is the trailing edge. That is partly the explanation of why a flat sheet of plywood will experience lift in a flow of air - it has a sharp trailing edge. | |||
::Under "Limitations of deflection/turning", the only limitation mentioned is that this explanation doesn't produce numbers. This limitation is a characteristic of all of the qualitative explanations and is now included in "The understanding of lift as a physical phenomenon". I recommend substituting the paragraph under "Limitations of the flow-deflection explanation" in my sandbox version ], which discusses some limitations specific to deflection. | |||
:::::Since the days of Joukowski and Kutta, mathematicians and physicists have been able to model the flow of an inviscid fluid around suitable geometric shapes. With a sharp trailing edge it is possible to determine the lift and pitching moment on the shapes. Tests on real models of wings in wind tunnels show there is close agreement between the math and the real world for these shapes with sharp trailing edges. For bodies without a sharp trailing edge, the math shows that an inviscid fluid imparts no lift or pitching moment to the body. | |||
:::::Wind tunnel tests on bodies without sharp trailing edges, and anecdotal evidence, show that these bodies can experience a little lift. This does not mean they qualify as airfoils under meaning No 3 above. Engineering, and most science, have little interest in these bodies. What lift they develop is not due to ''airfoil action'' - exploiting the Kutta condition to generate lift. It is due solely to viscous effects such as flow separation. These bodies, at best, have a very low lift-to-drag ratio. Little is written about them in mainstream science or engineering publications. This type of lift has little or no engineering application. | |||
::Under "Increased flow speed and Bernoulli's principle", the first paragraph needs to stipulate that Bernoulli's principle requires steady flow. | |||
:::::We know that eating a tablespoon of salt a day won’t cure cancer, but it is probably impossible to find a reliable published source that confirms eating a tablespoon of salt a day won’t cure cancer! Similarly it is probably impossible to find a reliable published source that confirms that no bluff body has ever been found that is capable of a high lift-to-drag ratio. | |||
:::::We use the Kutta condition to determine, mathematically, the circulation around a 2-D shape with a sharp trailing edge edge. There is no similar model, theory or equation to determine circulation around a 2-D shape with no sharp trailing edge. I suspect that wind tunnel tests would not show a usable relationship because, being reliant entirely on viscous effects, the results would be strongly influenced by the surface conditions of each model being used - roughness, smoothness, manufacturing imperfections etc. | |||
::In that same section, I recommend deleting the second paragraph. The statement "Bernoulli's principle does not explain why the air flows faster over the top of the wing" isn't true. On the contrary, Bernoulli's principle tells us that if the air flows faster, it is because of the lower pressure. It's just that that didn't help the originators of the Bernoulli explanations in boot-strapping their way toward an explanation of where the low pressure comes from, and they had to find other reasons for the faster flow. | |||
:::::When I say that bodies without sharp trailing edges do not generate circulation in fluid flows around them, I am speaking as an aerodynamicist applying the model of the inviscid fluid. There is no doubt that my statement is true for inviscid flows, which admittedly are fictitious, but this is usually a good, simple guide to the reality of high Reynolds number flows. When you say that all bodies in a fluid flow experience viscous forces and these forces will provide at least a very small amount of circulation that cannot be eliminated by the flow pattern adjusting itself you are possibly speaking as a scientist focussed on observing the complex realities of the real world. You aren’t able to determine how much circulation there will be, or say exactly how that circulation is sustained. What circulation exists is small and I say it is zero. You possibly describe the same situation by saying circulation is not zero. That might be as close to consensus as we can hope to reach. ] ''(])'' 15:39, 17 June 2024 (UTC) | |||
::::::Agree that I am sometimes a bit loose with the terminology re: airfoil. One other possible avenue of miscommunication here is that when I see the word "lift" in this context I think of the definition used in the first sentence of the article: | |||
::We're getting close, but I'd appreciate it if you'd consider the above changes. Thank you for your patience. | |||
:::::::When a ] flows around an object, the fluid exerts a ] on the object. '''Lift''' is the ] of this force that is perpendicular to the oncoming flow direction. | |||
::::::and as a mathematician rather than an aerodynamic engineer ''lift=0'' means actually zero, as opposed to "too small to be useful or significant." One of the arts of engineering is to figure out what things can be ignored, and for most non-airfoil applications the fact that there is some component of the aerodynamic force perpendicular to the airflow is negligible. I'm sure that there are many situations where we would agree that whatever small amount of lift might be present, it's too small to matter so let's assume it is zero. This would imply ETT in that situation. | |||
::] (]) 01:58, 27 July 2014 (UTC) | |||
::::::Other situations I wouldn't agree that it's too small to matter, for instance, a leaf on a tree in a breeze - the leaf repeatedly flutters back and forth in a direction perpendicular to the airflow and this implies to me that there is some force making it move that way and the obvious one is that there is some non-zero component of force transverse to the airflow. I would call that "lift" according to the definition above. But since I doubt either of us will be hired as an engineer to design tree leaves any time soon we can leave it there. ] (]) 17:56, 17 June 2024 (UTC) | |||
:::::::Thanks. I agree with most, if not all, of what you have written. I now realise that the concepts of streamlines, time slices, circulation and ETT are all concepts that rely on steady flow. When we are talking about a turbulent wake, separated flow, oscillatory flow, the erratic dancing of the leaves and branches of a tree, we can’t claim the protection offered by retreating to steady flow. Debating about streamlines, time slices and ETT in a non-steady flow is deeply flawed. | |||
:::A lot to respond to at once, so I'll break it up into bullet points; | |||
:::::::The dancing of leaves on a tree is definitely caused by the interaction of aerodynamic forces and elastic forces within the highly flexible structures of a tree. This kind of motion could be caused entirely by drag, so I’m not persuaded that the dancing motion of a leaf necessarily shows the presence of lift. | |||
:::::::The concepts of lift and drag rely on knowing the direction of the local velocity of the fluid. The air moving through the branches and leaves of a tree is highly disorganised and the velocity at each point is changing rapidly so it is probably true to say that while we can possibly identify aerodynamic forces acting on branches and leaves, the concepts of a drag component and a lift component are not applicable. The distinction between a lift component and a drag component seems to be reliant on steady flow, and flow in which the speed and direction at one point is almost identical to the speed and direction at all nearby points. | |||
:::*Placement of the "The understanding of lift as a physical phenomenon" section - As I've stated before I think it s a good addition to the article, but leading with it seems off-putting to the general audience. And really, fundamentally I think our disagreement here stems from a different idea of who the intended audience is. For the layperson who knows little about the subject (i.e. the vast majority of wikipedia readers) the section would make little sense without first providing some context. I am open to moving it up in the article, say, between "Basic attributes of lift" and "A more comprehensive physical explanation." | |||
:::::::The Kutta-Joukowski theorem is remarkably similar to Newton’s 1st and 2nd laws. Scientists and engineers say Newton’s laws are valid. Perhaps a mathematician and philosopher might say Newton’s 1st law is redundant because there is no such thing as a body whose acceleration is truly zero; and no such thing as a body experiencing a net force that is truly zero. ] ''(])'' 00:30, 18 June 2024 (UTC) | |||
::::::::In my edit dated 15 June 2024 (14:30) I wrote “I can supply a quotation from Anderson’s ''Fundamentals of Aerodynamics'' that will help on this topic.” See the . In section 3.16 Anderson writes about the Kutta-Joukowski theorem: <blockquote>"Although the result given by the equation <math>L^\prime = \rho_\infty V_\infty\Gamma</math> was derived for a circular cylinder, it applies in general to cylindrical bodies of arbitrary cross section."</blockquote> | |||
:::*Section heading - I don't see a big difference in meaning between "The understanding of lift as a physical phenomenon" and "Understanding lift as a physical phenomenon" to my eyes, the former merely has two extraneous words. But I can see how you would parse it differently than I, so I've reverted the heading to your original. | |||
:::::::: | |||
::::::::This confirms that the Kutta-Joukowski theorem is not confined to airfoils. It applies to all cylindrical bodies regardless of their cross sectional shape. If a cylinder of arbitrary cross section causes no circulation in the flow in which it is immersed the cylinder will experience no lift. | |||
:::*Section heading - "Simplified physical explanations of lift on an airfoil" is fine by me, I'll implement that change too. | |||
:::::::: | |||
::::::::It is not too great a leap to say that, just as airfoils are associated with the Kutta condition to explain when they will generate lift, and when they won’t, cylindrical bodies of arbitrary cross section also rely on a feature resembling a sharp edge to obtain a well-defined lift. If these bodies of arbitrary cross section experience lift in the absence of a sharp edge, it is due to viscous effects such as flow separation and asymmetric boundary layers, rather than due to airfoil action. | |||
:::*Section heading - ''propose deleting the heading "Methods to determine lift on an airfoil" and promoting "Lift coefficient" and "Pressure integration" to sections in their own right.'' that sounds reasonable. I'll do it and see how it looks. | |||
::::::::My mention of a well-defined lift is from "sharp trailing edge to obtain a well-defined lift" as written by ]. See citation No. 4 in ]. ] ''(])'' 12:44, 30 June 2024 (UTC) | |||
:::*''"The resulting force upwards is equal to the time rate of change of momentum of the air downwards" is problematic'' - I'm gong to punt on this one for now. Let me give it some thought and attention and I'll get back to you. | |||
:::* "Limitations of deflection/turning" - I think you make a reasonable criticism, but I also think there's a bit of strawman there - the basic deflection explanation does not refer only to forces "exchanged at the airfoil surface, where the air and the airfoil are actually in contact". The diagrams clearly show air being deflected at some distance from the foil, not just at the surface. <br><br>Agree that it doesn't explain why the air is deflected a distance away from the foil, or how the force manifests itself as a pressure difference, but my take is that it doesn't have to. For instance, it also doesn't explain why the air moves faster over the top or any of a hundred other related phenomena. It ''does'' explain where the lift force comes from and that's the point of the exercise.<br><br>We have to be careful that we don't give the misleading impression that deflection is ''wrong'' or ''incorrect'' and I think the typical wikipedia user could get that impression from what you have written. I'll take a stab at addressing your concerns by adding some of these issues to the list of limitations. | |||
:::*Redundancies in K-J theory section. Your proposal sounds fine. I'll take a look at integrating your changes into my version. | |||
:::* ''Under "Increased flow speed and Bernoulli's principle", the first paragraph needs to stipulate that Bernoulli's principle requires steady flow.'' Ok, I'll add something to that effect. | |||
:::*''"Bernoulli's principle does not explain why the air flows faster over the top of the wing" isn't true. '' Yeah, that sentence has always bothered me too. Once you know that the pressure is reduced, BP tells you that the speed is faster. So it does explain why. ''Equal transit time'' doesn't explain why the air goes faster, and most explanations based on BP do not explain (correctly anyway) why the air goes faster. I'll look at changing that sentence. | |||
:::It's now Friday, August first, and I think we are close enough that we can go live with the revision as-is. We can continue to discuss outstanding issues afterwards. I'll make the changes outlined above and unless I hear objections I'll replace the current article with the draft early next week.] (]) 15:19, 1 August 2014 (UTC) | |||
:::UPDATE: I've now completed the above edits. One issue I see is in response to ''I propose deleting the heading "Methods to determine lift on an airfoil" and promoting "Lift coefficient" and "Pressure integration" to sections in their own righ... I propose integrating some material from "Kutta-Joukowski theorem" into "Circulation and the Kutta-Joukowski theorem", moving the description of the Magnus effect to "Lift forces on bluff bodies", and deleting "Kutta-Joukowski theorem".'' | |||
:::I've done this in my draft (with the exception of the treatment of the Magnus effect - will take a look at that next) A question: does it make sense for Lift Coefficient and Pressure Integration to have their own sections, or does it make more sense for them to be sub-sections under "Mathematical theories of lift"? I'm in favor of the latter, but could be convinced otherwise. I'm going to move them under the math section pending further discussion. ] (]) 18:29, 1 August 2014 (UTC) | |||
Doug McLean wrote: ''...the statement "The resulting force upwards is equal to the time rate of change of momentum of the air downwards" is problematic... '' | |||
I have to say that I was surprised by this, so much so that I needed to take a few days to think about it before responding. And the reason for the surprise is that the statement is merely a combination of Newton's 2nd and 3rd laws with dp/dt replacing ma. This should be about as uncontroversial as it gets. In the simple model where all we consider is the air flow and the foil, it follows directly from Newton's laws. Of course, if the air is being accelerated by something other than its interaction with the foil then that additional acceleration will not contribute to the lift force, but it seems clear to me from the context that we're not talking about that scenario. I've added some language to clarify: | |||
:The resulting force upwards is equal to the time rate of change of momentum of the air deflected downwards by the foil. | |||
Agree that this total momentum change is difficult to calculate or measure. But in theory at least it must be equal to the lift force. | |||
BTW, there's not just one cite for it, three others are included elsewhere: | |||
https://en.wikipedia.org/User:Mr_swordfish/Lift#cite_note-7 | |||
https://en.wikipedia.org/User:Mr_swordfish/Lift#cite_note-23 | |||
https://en.wikipedia.org/User:Mr_swordfish/Lift#cite_note-32 | |||
] (]) 18:33, 4 August 2014 (UTC) | |||
:I'm also surprised by Doug's comment. Perhaps he is alluding to the idea that the time rate of change of momentum is equal to the aerodynamic force and not just its vertical component, lift. ] ''(])'' 22:28, 4 August 2014 (UTC) | |||
::No. The problem has nothing to do with whether we consider the total force exerted by the foil or only the lift component. See my response to Mr. Swordfish above. ] (]) 00:19, 7 August 2014 (UTC) | |||
:Your reasoning regarding placement of "The understanding of lift as a physical phenomenon" puzzles me. You argue that leading with it would be "off-putting to the general audience" and that it would "make little sense without first providing some context". But providing context is what this section is intended to do. It seems to me that launching directly into the deflection explanation without the context provided by "The understanding of lift as a physical phenomenon" gives a mistaken impression to the reader, to be remedied only later in the article: "Oh, by the way, those explanations we gave you early on aren't the real story on how lift is understood." | |||
:As for making "little sense" to an audience without prior knowledge, I don't see it that way. The section is brief and to the point, and, I think, easy to understand. I assume the target audience of an article in a general encyclopedia is literate adults, not children. If I were the reader, I'd welcome the context-setting up front. This is an encyclopedia article, not a mystery story. | |||
:So how do we decide this? Let's try a little meta-analysis of the arguments pro and con. I've argued that logical exposition of the subject matter favors having "The understanding of lift as a physical phenomenon" precede the simplified explanations, so as to put them in context with general understanding of lift. You haven't offered a counter-argument to this but have instead brought up other issues: "It's -meta." "It's potentially difficult for an audience without prior knowledge to understand." I think I've offered effective rebuttals to these arguments. | |||
:Regarding my proposed passage in "Limitations of deflection/turning", I think your argument that there's a strawman there is unjustified. I do say that the only forces referred to are those "exchanged at the airfoil surface, where the air and the airfoil are actually in contact", which is true. I don't say that those forces are all that the explanation refers to. I think the passage should be included. It doesn't imply that deflection is incorrect, just that it leaves a gap in that it doesn't explain how a deeper swath of flow is deflected than is touched by the airfoil. | |||
:Regarding "The resulting force upwards is equal to the time rate of change of momentum of the air downwards", I thought I made it clear in my previous posting what the problem with this statement is, but your response indicates that you don't agree that the force exerted by the airfoil is not generally the only force exerted on "the air" as a result of the lift. Let's look at this further. | |||
:A crucial question raised by the statement is what is meant by "the air". Again, any body of air that you choose to define as "the air" surrounding the airfoil must have both an inner boundary where the airfoil contacts it and an outer boundary where the surrounding environment contacts it. As a result of the lift there is generally an unbalanced pressure force on the outer boundary, so that the force exerted by the airfoil on the inner boundary isn't the only force resulting from the lift. With some detailed bookkeeping this pressure force can be quantified. If we put the outer boundary far enough from the foil, the idealized model of a uniform flow plus a vortex suffices, and we can draw general conclusions. Please read my previous comments where I explain how the percentage of the airfoil's force that is offset by the pressure force on the outer boundary depends on the proportions of the outer-boundary box. | |||
:Anyway, for most ways of defining what is meant by "the air", the statement is untrue. For example, the reader might reasonably assume that "the air" refers to the whole atmosphere. Given this definition of "the air", the downward force exerted on the air by the airfoil is completely offset by a distribution of over-pressure on the ground (see the famous figure 150 in Prandtl and Tietjens for what this pressure footprint looks like in 3D), so that the net force exerted on the air as a result of the lift is zero. Then the time rate of change of the integrated vertical momentum of the air must be zero as well. It's just Newton's second law, as you say. So again, the problem with the statement in the current draft is that it's not generally true, because it doesn't account for all the forces. | |||
:Your proposed clarification, i.e. limiting the statement to "the air deflected downwards by the foil", doesn't fix the problem. The subset of the air that's actually experiencing downward acceleration is still a body of air that an outer boundary can be drawn around. That body will still in general have a net pressure force on its outer boundary, so that the downward force exerted by the foil will not be the only force acting on that body of air. Thus even your clarified version of the statement isn't generally true. | |||
:There is one way to define "the air" so that the statement is true, but I think it's too specialized and complicated to be appropriate for this article. Draw the outer boundary of the box so that the vertical dimension is much larger than the horizontal dimension. In the limit as the vertical dimension goes to infinity relative to the horizontal dimension, the net vertical pressure force on the outer boundary vanishes. Then all of the lift is accounted for by the momentum transfer and none by the outer-boundary pressure force. But we're not done yet. To observe the momentum transfer as a time rate of change, we have to take another special step. The outer boundaries of the box must be assumed to be moving with the flow so that the box is not gaining or losing fluid anywhere along the boundary (This is different from the usual approach to control-volume analysis, in which box boundaries are fixed in the reference frame of the body). Only for this very special definition of "the air" can we make the statement that the lift is equal to the time rate of change of the integrated downward momentum of "the air". Unless we're willing to add these specialized qualifications to the statement (along with an appropriate citation), I think we should delete it. | |||
:This isn't just a quibble about rigor. The statement L = dp/dt is actually untrue for many reasonable ways of defining what is meant by "the air", i.e. it's untrue for anything other than an infinitely tall vertical sliver with boundaries that move with the flow. | |||
:The three sources you mention all make an error that's easy to make, i.e. applying the second law to a body of air, but without adequately defining what is meant by "the air" and without identifying all the relevant forces. The idea that "the air" generally has lift-related forces acting on it other than that exerted by the foil seemingly didn't occur to them. ] (]) 00:19, 7 August 2014 (UTC) | |||
::There seem to be three remaining areas of disagreement; | |||
::*'''Placement of the "The understanding of lift as a physical phenomenon" section.''' At this point, I don't think either of us are going to be swayed by the others opinion. My sense is that we have a disagreement over the intended audience and how best to serve that audience. My view is that the section makes a lot of sense to those who are already familiar with the material, but that it's "inside baseball" for 99% of the audience. My editorial sense is that we shouldn't lead with it.<br>This will have to be resolved by seeing what the other editors think or getting a third opinion.<br> I do take exception to your characterization "Oh, by the way, those explanations we gave you early on aren't the real story on how lift is understood." The simplified explanations are every bit as "real" as the more thorough explanations. Replace ''real'' with ''full'' and I'll agree with you. But the article is quite upfront about the fact that the simplified explanations are not the "full story". | |||
::*'''"Limitations of deflection/turning"''' I've added a few lines reflecting the issues you bring up. Please take a look. | |||
::*'''"The resulting force upwards is equal to the time rate of change of momentum of the air downwards"''' I have to say that I am not able to follow your line of argumentation. And even if I could and agreed with it, it wouldn't matter for our purposes here as editors. Discussions on this page are not citable. Our job as editors is to reflect what is published in reliable sources. In reading literally hundreds of articles on this subject, I have never run across a single one refuting this assertion. Meanwhile, there are several reliable sources that support the statement. Perhaps if there was some disagreement in the literature we could present it as a controversy. But unless we have some reliable published source we are bound to present what's been published. See ] for more details. | |||
::] (]) 18:33, 7 August 2014 (UTC) | |||
:::My arguments on the "rate of change of momentum" statement are all supported by citable sources. A minimal but sufficient set of them will be quoted below. I didn't bring them up before because I was advocating for deleting the statement, and I didn't think that would require citations. | |||
:::Because the statement doesn't specify what it means by "the air", a reader would and should expect it to be true for any reasonable assumption as to what "the air" encompasses. However, it is well established in the aerodynamics literature that the statement is false for most of the assumptions the reader might make, i.e. it is false if "the air" refers to the whole atmosphere or to any subset of it that isn't very tall compared to its width. If the statement failed only in exceptional circumstances I wouldn't press the issue. But it fails for the most obvious assumption the reader is likely to make, i.e. that "the air" refers to the whole atmosphere. So the problem is serious. | |||
:::Because the statement has been shown by reliable sources to be contradicted in relevant situations, it has been effectively refuted, and letting it stand "as is" would be inaccurate and inconsistent with "what's been published". I think that leaves us two options: | |||
::::1) Delete the statement and the citation. It isn't crucial to the deflection explanation, which is most often stated without the quantitative assertion " is equal to...." anyway. We have ample evidence from the mainstream aerodynamics literature that the statement is faulty, justifying our deleting it. | |||
::::2) Keep the statement but add the clarification that's needed to make it clear when it's true and when it's not. Here's a rough draft of what I think that would have to look like: | |||
::::In the text of the deflection explanation: | |||
:::::The resulting force upwards is equal to the time rate of change of momentum of the air downwards. This statement assumes that all of the lift can be accounted for by a momentum change in "the air", which is true only if "the air" refers to a region that is very tall relative to its width. For the atmosphere as a whole, or for a subset of it that is not tall compared to its width, part or all of the lift is accounted for by pressure differences on the top and bottom of the body of air in question, reducing the proportion accounted for by the momentum change. | |||
::::In the notes section: | |||
:::::For the atmosphere as a whole, the integrated time rate of change of vertical momentum due to the lift on a wing is zero , and the lift is reacted entirely by a pattern of overpressure on the ground. For regions that are subsets of the atmosphere, the proportions of the lift that are accounted for by momentum change and by pressure differences depend on the size and shape (vertical dimension compared to horizontal dimension) of the region. Only if the vertical dimension is very large relative to the horizontal dimension are the pressure differences negligible, leaving the lift entirely accounted for by the change in momentum. (Section numbers and quotes would be added to these citations, and other citations could be added. I mention only the ones that come immediately to mind, but I think even just these would be sufficient.) | |||
:::I expect you'll agree that the second option is too complicated and technical to be appropriate for this article. I'd argue that deleting the statement and the citation is the better option. | |||
:::I wouldn't advocate presenting this as a "controversy" because I don't think it amounts to one. The "con" arguments are from the mainstream aerodynamics literature, where they are supported by rigorous math. The "pro" statements you've cited are not supported by rigorous analysis and are all from "The Physics Teacher", which is not a mainstream source of information on aerodynamics. The error made by the statement isn't something esoteric about which experts might disagree; it's basic: It is wrong to apply Newton's second law to just a subset of the forces exerted on a body. In addition to the force exerted by the foil, the air around an airfoil generally has unbalanced pressure forces acting on it. Not being aware of these pressure forces is understandable in this case. Authors of articles in "The Physics Teacher" are not typically mainstream experts on aerodynamics. | |||
:::A relevant quote from ]: "To know where we have a dispute and where a simple mistake, consider whenever the author is really an expert on the topic (and not an expert on another topic, making a brief reference to something beyond his area of expertise)...." So we editors are not just cyphers. We are expected to exercise judgment as to the relative authoritativeness of our sources. Weighing what's been published in the mainstream aerodynamics literature against the statement in question, I think we'd be on firm ground deleting the statement and the citation. | |||
:::Your proposed changes to "Limitations of deflection/turning move in the right direction, but not far enough, in my opinion. And the first and second sentences have a jarring relationship. The first sentence deals with the failure to produce quantitative results. The second begins with "In particular," implying it is about to home in on a particular aspect of that issue, but then deals only with the incompleteness of deflection as a qualitative explanation, which is a separate issue. I'd replace "In particular" with "Furthermore". The third sentence deals with issues that are treated further later in the article, so some tie-in would be good. Here's a shot at fixing the whole paragraph, with some rearranging to keep the quantitative and qualitative issues separate: | |||
::::This simple explanation, while correct in as far as it goes, is not sufficiently detailed to support the precise calculations required for engineering. Quantitative predictions require a mathematical theory as described below under "Mathematical theories of lift." | |||
::::Furthermore, this explanation does not explain pressure and velocity variations in the vicinity of the airfoil or how the airfoil can impart downward turning to a much deeper swath of the flow than it actually touches. "A more comprehensive physical explanation" given below attempts to address these issues in a qualitative way. | |||
:::On an earlier question, I don't see "Pressure integration" and "Lift coefficient" as belonging in the mathematical-theory section. I think they would fit well in "Basic attributes of lift", with the material in "Pressure integration" merged into the current "Pressure differences", and the material in "Lift coefficient" merged into the current "Air speed and air density". I've tried this out in my sandbox ], and I think it works well. | |||
:::] (]) 06:44, 10 August 2014 (UTC) | |||
::::This discussion on change of momentum raises some interesting questions. It seems there's no controversy over the physics, but you disagree with the way some authors have concisely described the fulfilment of Newton's second and third laws. I appreciate that a quantitative integration of momentum change would require bounds to be defined carefully to avoid incorrect results, but our reader is not asked to do so. I agree this level of detail would be unnecessary for the article. | |||
::::Does the reader need any concept of packets of air which are subject to changes in either momentum or pressure? Isn't all fluid pressure ultimately caused by the change in momentum of particles of fluid as they strike their container? | |||
::::If the ''change of momentum of the air deflected downwards by the foil'' is understood to refer only to air which has its momentum changed downwards because of the movement of the foil, what other subset of 'the air' is included in the description which shouldn't be? ] (]) 11:21, 10 August 2014 (UTC) | |||
::::It's not just that I disagree with the concise statement. It's that the statement, taken at face value, has been refuted by authoritative sources. But you raise interesting questions. | |||
::::Yes, all pressure in gases is caused by changes in momentum of molecules striking and rebounding from the surface. In liquids, it's more complicated because molecules are in constant contact with their neighbors and can transmit force and exert pressure on the surface without changes in momentum. So the answer to your question is yes, but only for gases, not fluids in general. | |||
::::The molecular momentum change involved in gas pressure must be assessed very close to the surface. The only molecules that can be included are those between the last collision with another molecule before striking the surface and the first collision after rebounding. At sea level the region of interest would be about a micron (several mean free paths) thick, and only a fraction of the molecules in that region would qualify. That's a very limited subset of the air surrounding the airfoil. | |||
::::We could make the AAPT statement true by limiting it to that small subset of the molecules surrounding the foil. But I see several serious drawbacks to casting the statement in that form: | |||
:::::1. Aerodynamics generally deals with fluid motion as if the fluid were a continuum rather than individual molecules because it is very difficult to gain understanding or make predictions at the flowfield level with the molecular approach. | |||
:::::2. The continuum description is more generally applicable. Gases and liquids behave very differently at the molecular level but practically identically at the continuum level (for low Mach number in the gas). | |||
:::::3. Lift is an aerodynamic (and hydrodynamic) phenomenon. In the continuum approach to aerodynamics, "momentum" refers to the bulk momentum of the flowing fluid. The explanation of pressure in terms of molecular momentum, as you're proposing, refers to the thermal momentum of the molecules, not the bulk momentum of the fluid. This kind of explanation doesn't distinguish between aerodynamic and aero-static situations. Even in still air we could say that the pressure force on a portion of a surface is equal to the time rate of change of thermal momentum of the air molecules near the surface (the right subset of them). But this is a situation in which the air has no bulk momentum in the conventional aerodynamic sense. | |||
:::::4. The statement in the AAPT article refers to bulk momentum in the conventional continuum aerodynamic sense and deals with momentum changes taking place over distances measured in airfoil chords, not molecular mean free paths. If we were to recast it in the limited molecular sense, we'd need a different citation. | |||
::::The upshot: I don't think that interpreting the AAPT statement in terms of molecular momentum is a good solution to the questions it raises. I still think we should just delete it. ] (]) 20:34, 10 August 2014 (UTC) | |||
{{Outdent|::::}} | |||
Thank you for your detailed reply. I now understand the texts refer to momentum at the continuum level rather than the molecular level. | |||
No doubt your argument is well supported by sources, but I don't see a refutation of the statement. On the contrary, I see a description of how to prove mathematically that the statement is true; identifying which subset of the air is subject to downwards momentum changes and avoiding errors such as applying Newton's second law to a subset of forces, or summing action and reaction in the calculation of a single force. We agree that that calculation is beyond the scope of the article. | |||
I'm still not convinced that the cited non-specialist authors have made a mistake. I should point out that Chris Waltham's article does mention that, ''"to do this more correctly, we would box in the wing with a control volume of infinite vertical thickness"''. It happens all the time in science that a problem needs to be described and understood at the basic level before more rigorous treatement is attempted. ] makes a good point that there's a risk of losing the reader by expecting too much knowledge too early in the article. ] (]) 08:07, 12 August 2014 (UTC) | |||
Also, Eastlake says: | |||
{{quote| | |||
In the interest of generalization, it is appropriate to | |||
recognize that the isolated wing is not the only type of | |||
flow-field geometry. When there are other surfaces | |||
nearby, such as walls in flow through ducts or the | |||
ground, those other surfaces can and do change the | |||
momentum of the flow as well. | |||
}} | |||
Would it help the article to clarify that it refers to an isolated wing/foil? ] (]) 16:33, 12 August 2014 (UTC) | |||
:My preference is to keep the section under discussion as brief and to the point as possible, without adding a lot of qualifying language that obscures the simple meaning. It's an introductory section aimed at the lay reader after all. I'd rather remove the sentence than replace it with a multi-paragraph treatment of how to compute the infinite integrals to make the statement true. I don't think the statement is ''essential'' to the presentation and if there is consensus to delete I will reluctantly go along. | |||
:That said, I still think its a fairly straghtforward re-statement of Newtons' 2nd and 3rd laws and should be uncontroversial. Granted, when attempting to precisely elaborate on it, what one means by "the air" can be thorny. In a very simple model where all that is present is a uniform infinite fluid flow and a single airfoil, it has to be true. Add other things to the model such as gravity or the ground or other phenomena that affect the air and one has to be much more careful to obtain that result via the calculations. But it seems clear to me from the context that we're talking about a simple model rather than a more complex one. | |||
:Adding the word "isolated" probably won't make the sentence any clearer to the lay reader, but I'll go along with that if necessary. I really don't want to add a paragraph of introductory language to set up the simple statement of F = dp/dt. ] (]) 15:52, 13 August 2014 (UTC) | |||
::I agree. The section describes a principle of physics, not how to model a real-world example. I suppose the article wouldn't suffer greatly from the removal of that sentence, but I don't agree that it is false at face value. ] (]) 17:33, 13 August 2014 (UTC) | |||
::On that note, I think the context was clearer and flowed more naturally from, "Whenever airflow changes direction", before "by the foil" was ]. As Doug McLean said, it didn't help. ] (]) 07:13, 14 August 2014 (UTC) | |||
:::Agreed. I'll remove "by the foil" ] (]) 11:38, 14 August 2014 (UTC) | |||
:>Doug wrote:''Here's a shot at fixing the whole paragraph , with some rearranging to keep the quantitative and qualitative issues separate:'' | |||
:I adopted this language in the draft. I will look at moving the "Pressure integration" and "Lift coefficient" as per your suggestions. I think we are closing in on a releasable article. ] (]) 15:57, 13 August 2014 (UTC) | |||
::I think the draft is an improvement and look forward to the release. ] (]) 17:33, 13 August 2014 (UTC) | |||
::I've now moved the "Pressure integration" and "Lift coefficient" sections from the "Mathematical theories of lift" to "Basic attributes of lift". However I kept them as their own sub-sections - my take is that they are important enough on their own to merit their own sub-section. However, I did retain most of Doug's edits to the material. ] (]) 20:22, 13 August 2014 (UTC) | |||
:::I'd like to take one more try at easing your reluctance to delete the L = dp/dt statement. The statement's problems really are more serious than either of you have given them credit for. | |||
:::The conclusion that "In a very simple model where all that is present is a uniform infinite fluid flow and a single airfoil, it has to be true" isn't supported by the math unless you make stipulations about the shape of the region you're talking about. To evaluate either the pressure forces or the momentum fluxes in an infinite atmosphere, you have to evaluate the integrals over some finite box and then take the limit as the dimensions of the box go to infinity. Even in the case without a ground plane or any other surface, the L = dp/dt statement is true only if the ratio of the vertical height of the box to the horizontal width is infinite, a very specialized condition. It is untrue for any other shape of box. Thus simply adding "isolated" wouldn't by itself make the statement true in general. | |||
:::I'll mention two examples with an infinite atmosphere, in which the statement fails, both from the mainstream literature. In both cases the results hold as the size of the box goes to infinity. | |||
::::1. For a "pancake" box (infinite ratio of width to height) all of the lift shows up as integrated pressure differences between the top and bottom, whether there is a ground plane or not. The only difference is that with a ground plane all of the integrated force comes from the pressure excess on the bottom (the ground), while without a ground plane the force is equally divided between the pressure excess on the bottom of the box and a pressure deficit on the top. | |||
::::2. For a square box centered on the foil, once the sides of the box are longer than about ten airfoil chords, effectively half the lift is accounted for by the pressure differences between the top and bottom of the box, and half by the change in momentum. As the dimensions go to infinity, "effectively half" converges to "exactly half". The same goes for a circular box. | |||
:::I realize that this is counterintuitive. How can the pressure differences infinitely far from the foil account for half the lift? Well, for the small disturbances far from the foil the pressure perturbations are proportional to the velocity perturbations associated with the circulation, which die off as 1/r. The area over which these must be integrated is proportional to r. The upshot is that in the limit as the box size goes to infinity the integrated pressure force on the outer boundary of the box goes to a constant value equal to half the lift. So the force exerted by the foil is not the only force exerted on the air in the box. No matter how large the box is made, the air outside it exerts an unbalanced pressure force on the air inside. | |||
:::So I still maintain that reliable sources have shown that the L = dp/dt statement is false at face value. There is a wide range of reasonable interpretations of what is meant by "the air" for which it fails, even in the simple "isolated" case. It isn't a "fairly straightforward re-statement of Newtons' 2nd and 3rd laws" because meeting the requirements for applying Newton's second law (the force used in the equation must be the resultant of all the forces, not just a subset) still requires a very special shape for the box. | |||
:::I disagree with the statement "It happens all the time in science that a problem needs to be described and understood at the basic level before more rigorous treatment is attempted", at least when it comes to aerodynamics. Trying to understand aerodynamics at the basic level without support of rigorous analysis is too error-prone. ] (]) 19:29, 14 August 2014 (UTC) | |||
::::Thank you for your time and patience in explaining your point. It's been an interesting discussion and I've learned a lot: | |||
::::* In an infinite (square) universe, the forces between the airfoil, the air, and the environment can all be calculated by integration. Changing the bounds of integration changes the results, although the facts and forces in the situation remain the same. | |||
::::* It can be shown that the airfoil exerts a force on the air which is equal to the time rate of change of momentum of the air downwards. | |||
::::* It can also be shown that the environment exerts a force on the air which is equal to the time rate of change of momentum of the air upwards. | |||
::::* In accordance with Newton's third law, the upwards and downwards forces on the air are equal and opposite. As a result, the net change in momentum of the air as a whole is zero. | |||
::::* It is not correct to say, "half the lift is accounted for by the pressure differences between the top and bottom of the box, and half by the change in momentum." The lift is reacted entirely by a pattern of overpressure on the ground . If you had it both as an overpressure on the ground and as momentum in the air, that would be double bookkeeping ] ]. | |||
::::I still see no reason to remove the disputed statement but if I've misunderstood any of the above, I am happy to be corrected. ] (]) 07:00, 15 August 2014 (UTC) | |||
::::My take is that if the integration results are dependent on the relative dimensions of the box as the limit goes to infinity, then the results are not physical but rather an artifact of the model. We've seen this before: a well known rule of thumb for real world air foils is that the downwash angle is approximately equal to one half the angle of attack. This can be measured without recourse to taking integrals over an infinite area. But when you model it as 2-D airflow, in the limit as the span -> infinity the downwash angle becomes zero. This is an artifact of the model, not a reflection of the physics. I think that's what's going on here. | |||
::::I agree with both Doug and ] that it's incorrect to say that half the lift comes from momentum change and half comes from pressure differences. Granted, it may be possible to integrate in such a way that two terms appear that can be interpreted as momentum change and pressure difference, and depending on the relative dimensions of the box it can be 50-50, 0-100, or 100-0. My understanding of the physics is that ''all'' of the lift force can be ascribed to momentum change, and that ''all'' of the lift force can be ascribed to pressure differences. This half-and-half nonsense appears in some popularizations (one variant says "the foil generates lift on the bottom by Newtons law and on the top by Bernoulli's principle"). | |||
::::I'm with ] in seeing no reason to remove the statement. ] (]) 19:43, 15 August 2014 (UTC) | |||
::::Both of you ( ] and ]) seem still to think that my arguments against the L = dp/dt statement don't really apply to an infinite atmosphere and can be dismissed. The counterarguments you offer, however, aren't supported by the math or by reliable sources, only intuition. Intuition is not a reliable guide on this issue, as I'll try to show. You're probably tired of my arguments on this issue, but I intend to persist as long as the arguments you present for dismissing them are erroneous. | |||
::::The "artifact of the model" argument doesn't hold water for either example. | |||
::::The example of the airfoil "rule of thumb" is comparing apples and oranges, I think. The downwash angle behind "real world airfoils" equals roughly half the angle of attack (relative to the zero-lift line), when evaluated at a location about a quarter chord behind the trailing edge. That close to the airfoil, the downwash isn't affected much by aspect ratio, even as it goes to infinity, so the rule of thumb should apply regardless of aspect ratio. In 2D airfoil theory, the predicted near-field flow agrees with the rule of thumb, and the predicted downwash angle goes to zero only far behind the airfoil. So I think you're comparing the rule of thumb for the downwash angle near the foil with what 2D theory predicts for the downwash angle far away, and unjustly blaming the discrepancy on the 2D theory. And on the centerline far behind a 3D wing, the downwash angle goes to zero as aspect ratio goes to infinity, both in theory and in the real world. | |||
::::In the example of the integration of pressures and momentum changes in boxes surrounding an airfoil, the results are indeed "dependent on the relative dimensions of the box", even as the box size goes to infinity. But this is not because the flow model used is "not physical". It is because an infinite atmosphere is an artificiality. For boxes of finite size, no matter now large, the different results for different relative box dimensions reflect physical reality. The fact that the differences persist as the dimensions go to infinity isn't an "artifact" of the math. It reflects the fact that the momentum aspect of the physics is actually ill posed on an infinite domain. See comments below on ]'s first bullet item. | |||
::::The fact is that the partition of the force into pressure differences and momentum changes actually does depend on the shape of the box, no matter how large. So you haven't refuted my objections to the L = dp/dt statement. | |||
::::To repeat and address the bullet points: | |||
:::::] wrote * In an infinite (square) universe, the forces between the airfoil, the air, and the environment can all be calculated by integration. Changing the bounds of integration changes the results, although the facts and forces in the situation remain the same. | |||
:::::::It's true that what's going on physically doesn't change depending on how we choose to model it. But to quantify the forces and momentum changes, we have no choice but to calculate them by integration, and to do that you have to specify a domain. Then if the integration is done correctly, the results reflect the "facts and forces in the situation" in that domain. As I've pointed out, how much of the lift is accounted for by pressure differences and how much by momentum changes depends on the shape of the domain, even as the dimensions of the domain go to infinity. | |||
:::::::Our intuitions resist this, and we tend to assume that there must be a single correct answer for the entire infinite domain. But our intuitions about infinite domains are often wrong, and they're wrong in this case. The double (2D) or triple (3D) integral for the net vertical momentum due to a lifting airfoil or wing in an infinite atmosphere is non-convergent, which means that the vertical momentum is indeterminate. And you can't make quantitative statements about an indeterminate quantity. Still, one thing these integrals tell us about the "facts and forces in the situation" is true: The balance between pressure differences and momentum changes is different in domains of different shapes, no matter how large the domains are. | |||
:::::::This non-convergence doesn't matter in the real world because there is always a ground plane. Even for a semi-infinite space above a ground plane, the integrals converge, and the integrated vertical momentum in the whole atmosphere is zero. For finite subsets of the atmosphere, the shape of the box has strong effects on the results, as I've argued all along. See comment on fourth bullet below for what happens when the height above the ground is large compared to the box size. | |||
:::::::The non-convergence of the momentum integral in an infinite domain and convergence in a semi-infinite domain is not reported in the aerodynamics literature, other than in my book, as far as I know. It's based on a careful analysis of the far-field behavior of the integral by a colleague, a qualified mathematician. | |||
:::::::Back to the infinite-atmosphere case: What you say about the effects of "Changing the bounds of integration" could benefit from some clarification. The results of the integration change drastically with the shape of the domain, but if the shape is held constant, the results cease to change with the size of the domain once it is large enough. | |||
::::::] wrote * It can be shown that the airfoil exerts a force on the air which is equal to the time rate of change of momentum of the air downwards. | |||
:::::::No, not in general. It can be shown only for a domain with an infinite ratio of height to width. | |||
::::::] wrote * It can also be shown that the environment exerts a force on the air which is equal to the time rate of change of momentum of the air upwards. | |||
::::::::This is not true for any domain that contains a lifting airfoil. Remember, a force is equal to a time rate of change in momentum only if it's the only force (or the vector sum of all the forces) acting on the object in question. When there's a lifting airfoil, the force exerted by the environment isn't the only force acting on the air in the domain. | |||
::::::] wrote * In accordance with Newton's third law, the upwards and downwards forces on the air are equal and opposite. As a result, the net change in momentum of the air as a whole is zero. | |||
:::::::Are you referring to the forces exerted on the air by the foil and by the surrounding environment? If so, what you're saying isn't a correct application of Newton's third law. The third law refers to the forces exchanged between two objects, not to the forces exerted by two objects (the foil and the environment) on a third (the air). There is no reason two separate forces acting on a third object must be equal and opposite. | |||
:::::::With this bullet and the two previous, you've argued yourself into a contradiction: The net change of momentum of the air is zero. Thus according to the first of the three bullets, the lift is zero, which I don't think is what you were assuming. | |||
::::::] wrote * It is not correct to say, "half the lift is accounted for by the pressure differences between the top and bottom of the box, and half by the change in momentum." The lift is reacted entirely by a pattern of overpressure on the ground . If you had it both as an overpressure on the ground and as momentum in the air, that would be double bookkeeping. | |||
:::::::I think I made it clear that the statement you quote applies to the case of a square or circular box without a ground plane. And it is correct for that case. It's also correct if there is a ground plane, provided the distance to the ground plane is large compared to the dimensions of the box, so that the box and it's environs are effectively in free air. Of course it's not true if the box gets close to the ground plane, and especially if the bottom of the box is the ground plane. You're right to say that would be double bookkeeping. | |||
::::No reason "to remove the disputed statement"? As I've said, the statement is inaccurate, to say the least, unless we add clarification. It's been shown to be false for the most obvious interpretation the reader is likely to make of what "the air" means. This is from reliable sources, and no one here has effectively rebutted it. We all agree that the required clarification would be inappropriate for the article. To me, this adds up to a compelling reason to delete it. | |||
::::] (]) 05:19, 16 August 2014 (UTC) | |||
:::::To my mind, if you calculate something twice using two different methods, you should get the same answer, otherwise there is a problem with the calculation. If a physical fact is mathematically proven as true, then it is a fact. The conclusion I draw from argument you have made on this page is that the statement is true. I have not seen any reliable source, nor any reference to one, which says it is not. | |||
:::::I think the physics between the three bodies is pretty simple. The air is given some momentum by the wing. That momentum reverses direction as it rebounds from the surface, causing an overpressure. ] is a vector quantity. Equal and opposite vectors add up to zero. ] (]) 17:15, 16 August 2014 (UTC) | |||
::::::Most of the time you'd be right in saying that if you calculate something by two different methods you should get the same answer. But that's true only if the "something" you're trying to calculate has a definite value. A non-convergent integral, which is what we have in the case of the vertical-momentum integral in an infinite domain, doesn't have a definite value. A classic symptom of non-convergence (also called non-existence) in a double or triple integral on an infinite domain is that when you try to calculate it you get different values depending on the order or the relative rates with which you take the dimensions of the box to infinity. In a case like this, there is indeed a "problem with the calculation", but it's not what you're thinking. The problem is that no correct way to do the calculation exists when the thing you're trying to calculate doesn't have a definite value. This isn't just math. What it says about the physics is true. The vertical momentum due to a lifting foil in an infinite atmosphere is indeterminate. So I stand by my statement that the vertical-momentum aspect of the physics is ill-posed on an infinite domain. And this means that The Statement is problematic if the atmosphere is assumed to be infinite. | |||
::::::Your conclusion that The Statement is "true" is unfounded. You can't make a blanket statement that something is true if there are common situations in which it is untrue. The situations for which The Statement is untrue are well documented in the literature. In my entry of 10 August I cited a sufficient set of reliable sources. Do you disagree with these sources? If so, what are your specific objections? | |||
:::::::I think it's clear from this discussion that my understanding of the quote you gave from Prandtl and Tietjens is quite different to yours. ] (]) 09:50, 17 August 2014 (UTC) | |||
::::::I see a couple of problems with your discussion of the physics of three bodies. First, if the momentum imparted by the foil actually "reverses direction" in its interaction with the ground, the downward force on the ground would be twice the lift (Say the lift has a value of +1, for which the foil imparts downward momentum to the air with a value of -1. If the ground reversed the direction of that, it would go to +1, and the imparted change in momentum would be +2). Second, it's true that equal and opposite vectors add to zero, but in this case the vectors are equal and opposite only because you supposed them to be so. It isn't required by Newton's third law as you implied in the fourth bullet of your previous posting. ] (]) 05:31, 17 August 2014 (UTC) | |||
:::::::I'm saying the air presses down on the ground with a total force equal to lift. The ground presses back with an equal and opposite force. That is Newton's Third law. It may be true that Newton's Third law alone is not sufficient to prove conservation of momentum, but that's besides the point. ] (]) 08:34, 17 August 2014 (UTC) | |||
::::A further thought: Even if I agreed with you that The Statement was true for an infinite atmosphere, I'd argue that the right decision would still be to delete it. We have an explanation (deflection) that works fine without it and is usually stated without it. Why add a statement that's true only in a fictional abstract situation (an infinite atmosphere) and not in the real world where lift actually takes place (the real atmosphere with a ground plane)? The infinite-atmosphere case plays a role in the mathematical theories, but that's no reason to add something that's true only in that case to an explanation for the general reader. | |||
::::] (]) 16:10, 16 August 2014 (UTC) | |||
:::::The onus is on you to obtain ] for your proposal. ] (]) 18:46, 16 August 2014 (UTC) | |||
::::::That's what I've been trying to do. But I'd say the onus isn't just on me. The Statement: "The resulting force upwards is equal to the time rate of change of momentum of the air deflected downwards" is a paraphrase of a quote from a cited source in one of the notes in the current article. It doesn't appear in the body of the current article. Putting it in the body of the article, as ] proposes in his draft replacement is a change relative to the current article. Technically speaking, ] may be more obliged to obtain consensus to add The Statement to the body of the article than I am to obtain consensus to omit it. But this shouldn't be a legalistic game. It's supposed to be a cooperative effort. | |||
::::::I've put some effort into trying to convince you and ] that The Statement is technically sloppy and that without proper clarification it raises more problems than it's worth. I've offered detailed technical arguments backed by citable sources, and detailed rebuttals to your counterarguments. Neither of you has really attempted to rebut my arguments in any detail. Instead, you offer general observations on how you think the physics ought to work. When I've rebutted these, you've either tried another tack or simply restated your previous general assertion, but you haven't pointed out specific faults in my arguments. I'm open to being corrected, but I feel like one of the reasons this discussion is at a stalemate is that you're not really engaging with me on the technical details. | |||
::::::I've just argued that even if The Statement were true in a fictional abstract situation, it is still untrue in the real world, and that's enough to justify omitting it. What, specifically, do you disagree with in that argument? If this is to be a cooperative effort, the onus is on you as well. ] (]) 05:31, 17 August 2014 (UTC) | |||
:::::::I now understand the statement can be proven true even in a square flowfield, and <del>at least to a good approximation in most</del> real-world situations. You argue that in a square atmosphere, the ground reaction only supports half the lift. This cannot be true; if it were, the sky would fall. That is more than a sufficient rebuttal of your argument, in addition to the others I've given. Personally I don't have a strong opinion on the inclusion of the sentence, but I am quite satisfied from this discussion that it is true. Please ] to Mr. Swordfish. ] (]) 08:34, 17 August 2014 (UTC); edited 11:51, 20 August 2014 (UTC) | |||
Having had some more time to consider, I begin to understand how some of the misconceptions in this discussion relate to the citations provided. | |||
'''For the atmosphere as a whole, the integrated time rate of change of vertical momentum due to the lift on a wing is zero.''' | |||
When the momentum of a parcel changes from ''mv'' to ''-mv'', the change in momentum is ''mv - -mv'' = 2. | |||
The total momentum is ''mv + -mv'' = 0. There is no change. | |||
Therefore, there is no contradiction between, "For the atmosphere as a whole, the integrated time rate of change of vertical momentum due to the lift on a wing is zero", and, "The resulting force upwards is equal to the time rate of change of momentum of the air downwards". | |||
This citation does not imply that changes in momentum do not happen in the atmosphere, or that the AAPT statement can sometimes be false. | |||
'''the lift is reacted entirely by a pattern of overpressure on the ground''' | |||
''Reacted'' does not mean ''produced''. The airfoil is fully supported by the air. The air is fully supported by the ground. Therefore the air's reaction to the airfoil and the ground's reaction to the air are both equal to lift. | |||
The overpressure is caused by the ground's reaction to the momentum imparted to the air by the airfoil. It cannot exist in isolation, that would breach Newton's Third law. | |||
'''For regions that are subsets of the atmosphere, the proportions of the lift that are accounted for by momentum change and by pressure differences depend on the size and shape (vertical dimension compared to horizontal dimension) of the region. Only if the vertical dimension is very large relative to the horizontal dimension are the pressure differences negligible, leaving the lift entirely accounted for by the change in momentum''' | |||
I can see why calculating this would create challenges, although I have not seen the details. As agreed, it is wrong to apply Newton's second law to a subset of forces, which is why any calculation would have to account only for the force relevant to that calculation. | |||
It makes sense that a region with large vertical dimensions relative to the horizontal would account mainly for momentum changes due to the airfoil because that region contains the entire airfoil and a relatively small proportion of the ground. For similar reasons, a horizontal box would account mainly for ground reaction. | |||
Enlarging the region to a square box would not achieve the isolation described above. As a result, the downwards forces on the air will enter the calculation as well as the upwards forces. This is incorrect. I would expect such a calculation to give a result of zero, since the net change of momentum in the atmosphere as a whole is zero. | |||
This citation does not imply that changing the bounds of a calculation has any effect on forces in the physical world. | |||
I understand the objection that external pressure differences will slow down the air as it travels downwards and prevent it from keeping all of the momentum it has been given by the wing. However, a slowing down of the air is still a negative change of momentum. It is not correct to say that the statement does not apply when there are other forces involved. It does apply, it's just more difficult to quantify. | |||
By the way, I have found an additional ] which is more specifically related to aerodynamics. Hope this helps. ] (]) 11:51, 20 August 2014 (UTC) | |||
As ] says, there is not yet a clear consensus on this issue. Unfortunately I am not able to engage in all the technical details since I am not a subject expert. My ideas may be naïve but you are of course welcome to discuss them. I am sorry if I have created the impression otherwise. ] (]) 07:42, 26 August 2014 (UTC) | |||
I am disappointed to see another week of embarrassing silence. The issue should be ], not as an ''exercise in schadenfreude'', but in order to progress the volume of knowledge which we have all worked towards. | |||
I just found the following quote: '''lift is accounted for either by pressure or by momentum flux, depending on the proportions of the control volume. ''' | |||
This seems clearer than the final citation given above, confirming that the control volume can account entirely for the force exerted on the air by the airfoil or for the reaction from the environment, not 'proportions of the lift'. I hope this settles any remaining doubt or confusion. | |||
I don't think anyone disputes that it is possible to define a region of 'the air' which only accounts for the downward change in momentum caused by the foil, and also a different region which only accounts for overpressure caused by the reaction from the environment. The fact remains that the environment only touches the outer boundary of the air, it does not contact the foil and cannot contribute to the lift force. | |||
The question is whether the wording, "The resulting force upwards is equal to the time rate of change of momentum of the air downwards" is sufficient to identify the region of air referred to, without necessarily describing it in detail. I say it does, because there is only one correct way to calculate 'rate of change of momentum of the air downwards'. | |||
Do we now have consensus for the proposed addition? ] (]) 09:03, 4 September 2014 (UTC); edited 10:56, 4 September 2014 (UTC) | |||
:I don't see any evidence that anyone has changed their mind. And I have little expectation that further discussion will alter that fact. A couple of weeks have gone by without hearing from the lone dissenter, so the answer is a qualified "maybe". I'm not going to add the sentence, but I won't object if someone else does. ] (]) 16:16, 4 September 2014 (UTC) | |||
::It does shake your confidence a little to be told you're wrong, repeatedly by someone who is in a position to know, doesn't it? On the other hand, we know that an ] is fallacious. Even experts can make mistakes, sometimes very ] ones. | |||
::I think what would help us most now would be the considered opinion of an aerodynamics expert. ] (]) 16:41, 4 September 2014 (UTC) | |||
] wrote: ''if there is consensus to delete I will reluctantly go along... In the interest of moving forward, I have removed it'' | |||
Thank you for demonstrating your willingness to compromise by removing it, and for your patience awaiting further discussion. I agree that now looks unlikely to happen. I was going to wait until after my holiday to post this, but I think we've waited long enough for a resolution to this dispute. | |||
I see a ] that the statement is in keeping with guidance from the AAPT. I see no legitimate concern in opposition, so I am re-adding it. ] (]) 05:10, 7 September 2014 (UTC) | |||
== L=-dp/dt == | |||
In the discussion above we have failed to reach consensus (yet) about the inclusion of the sentence "The resulting force upwards is equal to the time rate of change of momentum of the air deflected downwards." | |||
In the interest of moving forward, I have removed it from the draft and would like to proceed with publishing the draft in it's current state. We can continue to discuss the issue, but I don't want to hold up publication pending the resolution of what I think is a fairly minor issue in the greater scheme of things. Have we reached consensus on publishing the article as-is? If so, I'll make the switch. ] (]) 19:56, 19 August 2014 (UTC) | |||
:I agree. I'm in favor of you making the switch. Well done! ] ''(])'' 06:12, 20 August 2014 (UTC) | |||
::It is clear how much time and effort you (] and ]) have both put into improving the clarity, coverage, and accuracy of the article. Thank you. I haven't been able to review the draft in as much detail as you, but I think it would be a shame to let it go stale because of a disagreement over one or two sentences. It makes sense to move into the article space and iron out any remaining details in the normal course of Misplaced Pages editing. ] (]) 08:28, 20 August 2014 (UTC) | |||
:::It's now been a week, and seeing no opposition I'm making the draft live. We can continue to discuss and improve that article moving forward. ] (]) 14:49, 26 August 2014 (UTC) | |||
== Lift does NOT only apply to airfoils - they are a special case == | |||
This is my first ever contribution to Misplaced Pages - so I apologise in advance if I breach any guidelines. | |||
My concern is that this whole article suffers from a major distortion in its emphasis. Lift is defined as being the force perpendicular to the motion of an object relative to a fluid. The object does not need to be an airfoil (wing shape). But this whole article is utterly preoccupied with airfoils. And as a consequence with Bernoulli's principle (and its various possible explanations). Therefore the article largely duplicates the existing Bernoulli Principle article. They should be merged together. | |||
The article also - as a consequence of the above - completely ignores other mechanisms whereby Lift is generated, and all the real-world examples. EG the rudder of a boat; a kite; the tail of a fish or dolphin, a scuba diver's fins, a weathervane etc etc. There are plenty of examples of flat objects generating lift purely because of their angle of attack, nothing to do with Bernoulli and airfoils. These should be the first topic in an article on Lift. Airfoils should be mentioned as a special case with a link to the existing articles on Airfoil and Bernoulli. To ignore the most simple and straightforward source of Lift is bizarre. <span style="font-size: smaller;" class="autosigned">— Preceding ] comment added by ] (]) 00:39, 4 September 2014 (UTC)</span><!-- Template:Unsigned IP --> <!--Autosigned by SineBot--> | |||
:Welcome to Misplaced Pages, and thanks for your contribution. The only deficiency with your first edit is that you forgot to sign your "name" by typing four tildes - see ]. This should be done at the end of all contributions to a Talk page. (You will notice a Bot has signed your "name" for you.) | |||
:*''But this whole article is utterly preoccupied with airfoils.'' I disagree. The word "airfoil" is not used until the seventeenth sentence. Many textbooks concede that even a flat plate can experience lift when it is behaving '''like an airfoil.''' This article is about lift and how it is generated. It is reasonable to clarify the meaning of lift by describing it as a force experienced by airfoils and other objects when they are behaving like airfoils. | |||
:*''The article also completely ignores other mechanisms whereby lift is generated, ...'' I disagree. The seventh sentence in this article states "Lift is also exploited in the animal world, and even in the plant world by the seeds of certain trees." (Or are you alluding to the ]?) | |||
:*''To ignore the most simple and straightforward source of lift is bizarre.'' You forgot to state what it is you believe is the "most simple and straightforward source of lift." Please clarify. | |||
:Please read the article carefully and if you find a sentence or paragraph that states or implies lift is produced only by airfoils, or predominantly by airfoils, please let us know by replying here on this Talk page. ] ''(])'' 06:38, 4 September 2014 (UTC) | |||
==The Statement (L = -dp/dt) should be deleted== | |||
I've been away from internet access for several weeks and thus not able to participate in the discussion. I see that in the interim ] installed the revised article, which I support, and that ] has added to it The Statement, "The resulting force upwards is equal to the time rate of change of momentum of the air deflected downwards", which I don't support. | |||
Two general lines of argument have been put forward in support of The Statement, an earlier one by ] and a more recent one by ]. Both of these lines of argument are contradicted by what actually happens in lifting flows, as I'll show below. ] has put forward several rebuttals of my arguments against The Statement, but none of these rebuttals is consistent with the physics, as I'll also show. | |||
Thus in the interests of technical accuracy and consistency with the published specialist sources The Statement should either be deleted, or the required clarification should be added, as I've discussed in earlier posts. I may be the "lone dissenter", but my "con" position is supported by the physics as described in the mainstream aerodynamics literature, while the "pro" position is supported only by the statement itself in an article in a journal for physics teachers, and by intuitive and insufficiently rigorous arguments on this page, which I believe to be erroneous and for which I know of no citable source. | |||
Let's look at the failings of the "pro" arguments. | |||
===Limiting integration to "the air deflected downwards"=== | |||
Some time ago ] argued, and ] later agreed, that The Statement must be true if the rate of change of momentum is integrated only over the air that is being "deflected downwards", i.e. that is undergoing downward acceleration. But this idea has no support in the physics or in the literature. | |||
In a steady flowfield around a lifting airfoil, consider the air that is currently undergoing downward acceleration and thus contributing to the integrated rate of change. This is a body of air around which a boundary can be drawn and for which we could in principle calculate the integrated rate of change of vertical momentum. But we can arrive at a qualitative assessment of ]'s idea more easily by looking at the forces exerted on this body of air. For The Statement to be true, the total force exerted on "the air deflected downwards" would have to be equal to the force exerted on it by the airfoil, and the net force exerted on it by its other surroundings would have to be zero. | |||
For simplicity, assume the inner boundary of this body of air is everywhere in contact with the airfoil surface, though that may not always be true. Assume further that at this inner boundary the airfoil exerts a downward force on the air equal to the lift. What we need to evaluate now is whether the force exerted on the air by its surroundings at the outer boundaries is zero as required if The Statement is to be true. What do these outer boundaries look like? In general they will take the form of two curves fanning forward from near the leading edge, one upward and one downward, and two curves spreading aft from the trailing edge, one upward and one downward. In the far field, these curves will approach +-45-degree lines configured like a letter X (see fig 7.3.23 in my book). The air being accelerated downward is thus contained within two generally fan-shaped regions, one above the airfoil, and one below, with the combined regions forming a general hourglass shape with the airfoil spanning the waist. For our purposes, the key characteristic of these regions is that the boundaries have extensive projected horizontal area on which the pressure differences in the field will act and thus exert an integrated vertical pressure force. The theory gives us no reason to expect that the integrated vertical pressure force on this entire outer boundary is zero, and in fact it isn't. The boundaries of the upper region are immersed in lower-than-ambient pressure, and the boundaries of the lower region are immersed in higher-than-ambient pressure, resulting in an unbalanced pressure force. Thus the total force exerted on "the air deflected downwards" is not equal just to the downward force exerted by the airfoil. | |||
So I stand by my earlier argument that The Statement is true only for a box that is very tall compared to its width, and is not generally true for "the air deflected downwards". | |||
:I accept your point that 'the air deflected downwards' includes more air than just a slim column. However, for the reasons you have given, there is only one correct way to calculate 'the rate of change of momentum of the air deflected downwards'. The resulting force is always equal to lift, regardless of what other incorrect calculations could be made. ] (]) 15:18, 17 September 2014 (UTC) | |||
::If we take 'the air deflected downwards' to be a small box, then the assumption that its surroundings exert no force on it is false: in accelerating downwards, it experiences an increase in lift from the box above, which in turn experiences an increase in downforce. The assumption is only true for an arbitrarily tall volume. The counterargument to "The Statement" is likewise false. — Cheers, ] (]) 13:28, 22 September 2014 (UTC) | |||
===Lift manifested as a rate of change of momentum in the neighborhood of the airfoil, with that momentum being removed elsewhere by interaction with the ground=== | |||
] has argued that the airfoil imparts downward momentum to air in some region surrounding it at a rate equal to the lift and that that momentum is then canceled in the far field in its interaction with the ground, resulting in the overpressure on the ground. This idea is intuitively appealing, but it isn't consistent with the detailed physics of the flow around an airfoil. See, for example, my argument above regarding the fan-shaped regions of "the air deflected downwards", and the fact that even in the near field that body of air will generally have unbalanced pressure forces acting on it in addition to the force exerted on it by the airfoil. | |||
Or consider the air in a square box surrounding the airfoil, where the box is at least several chords in size but small compared to the distance from the ground, so that the flow in the box is as if the airfoil were in free air. In this case only half the lift is manifested as a rate of change of momentum, and the other half as pressure differences on the top and bottom of the box (] took issue with this result for a square box, but that was the result of a misunderstanding on his part, as I discuss below). | |||
A further counterargument: Removing downward momentum from the air requires upward acceleration. If the overpressure on the ground were a result of downward momentum being removed from the air in the neighborhood of the ground, there should be a region of upward acceleration of the air overlying the area of overpressure on the ground. But this isn't what we see. For an airfoil many chords above the ground, the overpressure on the ground is centered directly under the airfoil (The 2D version of the overpressure distribution is qualitatively just a 2D version of the 3D drawing in Prandtl and Tietjens). The dominant central portion of this region of overpressure, where the overpressure is strongest, is overlain by air that is accelerating downward, not upward. Only the weaker parts of the overpressure distribution, well ahead of the airfoil and behind, are overlain by air that is accelerating upward (This can be shown based on the model of the flow as a uniform flow with a lifting vortex and the image of the lifting vortex under the ground superimposed, which would be valid for large height compared to the chord. For smaller heights, some details would differ, but not the overall conclusion). Thus ]'s simple momentum explanation for the overpressure is not consistent with the real pressure and velocity fields. | |||
:I never specified the nature of the region of air accelerating upwards. I simply inferred its existence from the facts that the airfoil accelerates air downwards and the net rate of change of momentum of the atmosphere as a whole is zero. I see no evidence that the momentum explanation I gave is inconsistent with yours. ] (]) 15:18, 17 September 2014 (UTC) | |||
::What happens in the far field is wholly irrelevant to the way in which forces are generated and momentum is changed locally. This sub-topic is equally irrelevant to the main discussion. — Cheers, ] (]) 13:36, 22 September 2014 (UTC) | |||
===Rebutting the rebuttals of the "con" arguments=== | |||
] has put forward several rebuttals of the "con" arguments, but none of these rebuttals is consistent with the physics. I'll address some of the main points here. | |||
] wrote: *I now understand the statement can be proven true even in a square flowfield, and at least to a good approximation in most real-world situations. | |||
:It can't be proven for a square box because it isn't true for a square box. You haven't proven it, and you haven't offered a citable source that proves it. | |||
::If it's possible to perform a calculation on a subset of the atmosphere, it is likewise possible to perform a calculation on a subset of a square box. That is my interpretation of the citations you have given. Let's not forget as well that The Statement itself is already cited. ] (]) 15:18, 17 September 2014 (UTC) | |||
] wrote: *You argue that in a square atmosphere, the ground reaction only supports half the lift. This cannot be true; if it were, the sky would fall. | |||
:This is a misinterpretation of my argument. As I wrote originally and later reiterated, for a square box, equal partition of the effect of lift between momentum changes and pressure differences is the result for the case where there is no ground plane, or the ground plane is far away compared to the size of the box. With equal partition, the half of the lift accounted for by pressure differences is equally split between the pressure excess at the bottom of the box and the pressure deficit at the top, i.e. one quarter each. | |||
:I never said that the partition is equal when the bottom of the box is the ground plane. If the airfoil is centered in a square box that is large compared to the airfoil chord, and the bottom of the box is the ground plane, it can be shown that half the lift is accounted for by the pressure excess on the part of the ground plane that forms the bottom of the box, about 14% is accounted for by the pressure deficit on the top, and about 36% is accounted for by the change in momentum. To find all of the lift accounted for by the overpressure on the ground, you must integrate over the entire ground plane, not just the part inside the square box. | |||
::So, we agree that this calculation does not fully account for either of the two forces on the air. ] (]) 15:18, 17 September 2014 (UTC) | |||
] wrote: *Therefore, there is no contradiction between, "For the atmosphere as a whole, the integrated time rate of change of vertical momentum due to the lift on a wing is zero", and, "The resulting force upwards is equal to the time rate of change of momentum of the air downwards". | |||
:If you simply assume, as you did, that the airfoil imparts downward momentum at a rate equal to the lift, and that the ground takes it away at the same rate, then the total rate adds up to zero as it should, and there is no contradiction. But the fact that the assumed rates add up to the right sum doesn't prove that the assumed rates were correct to start with. In a real airfoil flow, the rate of momentum change is equal to the lift only for a very restricted definition of "the air" (a tall "sliver" of a box). For any other definition of "the air", including for "the air deflected downwards", the rate of momentum change is not equal to the lift, and there is a contradiction. See my arguments above. | |||
::As I said, the environment only touches the outer boundary of the air, it does not contact the foil. You seem to be implying that the rigidity of the ground actually contributes to the lift, rather than simply reacting to it. That is not what is said in the citation you gave from Prandtl and Tietjens. If the ground reaction cannot contribute to lift, the foil must be entirely supported by momentum changes. <ins>So I believe it is absolutely true that 'the airfoil imparts downward momentum to the air at a rate equal to the lift.' I disagree with your opinion that it would be 'reasonable' for anyone attempting a calculation of the rate to assume that air subject to other forces should be included.</ins> ] (]) 15:18, 17 September 2014 (UTC); edited 07:13, 20 September 2014 (UTC) | |||
] wrote: *I don't think anyone disputes that it is possible to define a region of 'the air' which only accounts for the downward change in momentum caused by the foil, and also a different region which only accounts for overpressure caused by the reaction from the environment. | |||
:If you mean one region surrounding the airfoil in which the force exerted by the airfoil is reflected only in momentum changes, and another region farther away in which the environmental pressures act on the imparted momentum, then I dispute it. In general, there is no support in the physics or in the literature for the idea that these effects can be separated into different regions in that way. You haven't shown us any example of a region that meets your requirement that it "only accounts for the downward change in momentum caused by the foil". | |||
::You have already given an example: "Only in the limit as the vertical dimension of the box becomes large relative to the horizontal is it true that lift is accounted for by momentum changes." ] (]) 15:18, 17 September 2014 (UTC) | |||
:I've shown that any rectangular box that isn't very tall compared to its width doesn't satisfy the requirement, and that the body of "the air deflected downwards" doesn't either, because unbalanced pressure forces on the outer boundaries of "the air deflected downwards" are acting even in the near-field of the airfoil. Again, the only way to see lift manifested only as a change in vertical momentum is to confine your view to a box that is very tall compared to its width. | |||
===The bottom line=== | |||
Those are the technical issues as I see them. I think it's clear from what's written in the mainstream literature that The Statement isn't true unless it is explicitly stated that "the air" refers to a region of air in the form of a very tall "sliver". And because this level of detail isn't appropriate for the article, it would be better just to delete The Statement. As for restricting it to the air undergoing downward acceleration (i.e. by changing "momentum of the air downwards" to "momentum of the air deflected downwards"), that doesn't fix the problem either. | |||
However, in one way the "air deflected downwards" issue is beside the point. Even if adding "deflected" did fix the problem, it would be an unwarranted extrapolation from the source material and thus constitute original research. The AAPT article says nothing about integration at all, let alone about the idea of restricting the integration to the air undergoing downward acceleration. | |||
But the bottom line is that no viable defense of either version of The Statement has been given. The Statement in either form is inconsistent with what's known from the mainstream literature, and it should be deleted. | |||
If you still disagree with me, I'd suggest you seek a second specialist opinion. I'm not going to recommend a particular expert to you because I'd be open to the accusation of seeking a friendly witness. The arguments I've made here are pretty basic aerodynamics, based on the standard control-volume framework for analyzing momentum balance in fluid flows, and using a well-accepted model for 2D lifting flow (uniform flow plus a vortex, plus an image vortex if there is a ground plane). If another aerodynamics specialist agrees to look at this, I'd expect him/her to look at the same sources, apply the same models, and reach the same conclusions that I have. | |||
] (]) 01:19, 17 September 2014 (UTC) | |||
:I appreciate a reply with some clarification. However, I see no significant new material or progress towards resolving the issues raised. | |||
:I see no response to the problem I pointed out, with a fresh citation which clarifies that the proportion of momentum and pressure accounted for by the control volume is dependent on its aspect ratio. My understanding is that the force on the foil is caused entirely by momentum changes, and the force on the ground is caused entirely by pressure, and both forces are always equal in magnitude to lift. A control volume which accounts for a mixture of these effects will therefore account for a mixture of the equal and opposite forces on the air. This would not be a calculation of the lift force. As you say in your book, "You can apply the standard procedures for evaluating integrals and, without making any procedural error, obtain a wrong answer." | |||
:You are now requesting a 'specialist opinion', knowing I am not a specialist. I would welcome an opinion from an alternative specialist, but unfortunately I don't know how, or whether, that can be arranged. More importantly, I agree with your earlier statement, that it "isn't something esoteric about which experts might disagree; it's basic: It is wrong to apply Newton's second law to just a subset of the forces exerted on a body." I have studied physics at degree level and consider myself qualified to comment on the Newtonian mechanics between three bodies. You have described in detail how it is possible to choose a region which mathematically eliminates the reaction force in order to prove that the force on the airfoil is equal to the rate of change of momentum, yet you claim this statement is not generally true. The sources you have offered do not appear to support your assertion. ] (]) 15:18, 17 September 2014 (UTC) | |||
::I prefer to understand lift as a reaction to the force accelerating the air downwards: ''F''=''ma''. This is dimensionally equivalent to the rate of momentum change over time, ''dp''/''dt'', with both expressions having dimension MLT<sup>-2</sup> (Mass x Length / Time squared). The statement given in the article is perfectly valid - no amount of sophistry is going to overcome such basic physics. — Cheers, ] (]) 13:50, 22 September 2014 (UTC) | |||
22 Sept 2014 - I've remained silent for the past week to give others a chance to express their opinions. Welcome back, Doug. I am pleased to see that your absence was only temporary. My take on the current situation: | |||
*We still haven't reached consensus on the inclusion of The Statement. I do not think a temporary absence by one of the main editors should be interpreted as achieving consensus, so in the interest of fairness and following the wikipedia protocols I am (reluctantly) removing The Statement until we reach consensus to add it. Whether this is temporary or permanent remains to be seen. | |||
*I have posted requests for assistance at the parent project pages to solicit wider opinion. I see that ] has already responded. (welcome!) Hopefully, we'll get some other views. The next step would be filing an RFC, but let's see what the folks from the project pages have to say. | |||
] (]) 14:30, 22 September 2014 (UTC) | |||
:*I have only looked at the extensive walls of text here in a very cursory way, but my initial impression is that this wording is actually a bit confusing, independent of the question of whether it is rigorously true. Why is it being described as a rate of change in momentum rather than a force? The more intuitive wording would be something like, "The force applied upward is equal to the ". The current wording requires that you convert "change in momentum over time" to "mass times acceleration" in your head just to get the units correct.] ]</sup>/<sub>]</sub>] 16:49, 22 September 2014 (UTC) | |||
::Yeah, it's quite a wall, isn't it? Anyway, The American Association of Physics Teachers has this pedagogical recommendation: | |||
:::"...lift on an airfoil should be explained simply in terms of Newton’s Third Law, with the thrust up being equal to the time rate of change of momentum of the air downwards." (https://en.wikipedia.org/Lift_%28force%29#cite_note-7) | |||
::So, that's where the language comes from. It seems pretty clear to me, but maybe I'm too close to the issue. ] (]) 17:17, 22 September 2014 (UTC) | |||
:::I suppose that a strict derivation from Newton's Third Law would require one to identify the net force on the air as, say, ''F''. One then points out that by said law, ''F'' and ''L'' are equal and opposite. Both ''F'' = ''ma'' and ''F'' = ''dp''/''dt'' are then valid derivations of ''F''. I guess which of them one uses will depend on whether momentum or acceleration is more to the fore in the subsequent treatment. Here, I did not notice any subsequent treatment, so I'd suggest that we describe both relationships, making it clear that they are equivalent. — Cheers, ] (]) 17:57, 22 September 2014 (UTC) | |||
::::Yes, I would agree with this - I am seeing this entirely out of context, and it's not obvious to me why we're comparing a force to a change in momentum over time. I guess it's because the statement is conveying two ideas simultaneously - the fact that the two forces (the force downward on the air and the force upward on the wing) are equal, and the fact that forces are changes in momentum over time. I think it would work fine if it were broken out more clearly: "The force applied upward is equal to the - or, equivalently, the change in momentum over time - ." Of course, the question is still open, in my opinion, as to ''why'' we're bringing momentum into this at all. If there was some reasoning for this particular choice in the original source, does it still apply here if, {{u|Steelpillow}} says, we're not actually discussing the ''momentum'' specifically? ] ]</sup>/<sub>]</sub>] 18:40, 22 September 2014 (UTC) | |||
:* I came here from the physics project. Walls of text and sometimes missing signatures and/or inconsistent indents mean that I've only skimmed the controversy. To help resolve the problem of whether the statement, or something like it, should be in the article, we should appeal one of the pillars of Misplaced Pages, ]. If mainstream reliable sources assert that the statement is true, then the statement is verified and with ] that explanation deserves a place in the article, along with citations to said sources. If there are reliable source that claim the statement isn't true, then that controversy should be reported with due weight and cited sources. It doesn't matter whether I or any other editor ''think'' the statement is true or false or incomplete, only the reliable sources matter. Indeed, our personal takes on the subject could become ] if we stray too far from the sources. | |||
:: Given the pillar of verifiability, perhaps we can resolve this controversy by giving an accounting of the reliable sources for and against. Then inclusion of the statement would be based on judging the quality and weight of the sources, not our personal takes on the subject. I confess to not parsing all the verbiage to extract those sources. Could they be summarized here? --] (]) 18:38, 22 September 2014 (UTC) | |||
:::Yes, I would also appreciate a summary of the sources, and if someone who understands it better could clarify in a ''succinct'' way the particular nature of the conflict, that would be appreciated. I'm starting to parse out the particular objections, but it'd be much easier if this were done RfC style, with a simple summary of the conflict.] ]</sup>/<sub>]</sub>] 18:49, 22 September 2014 (UTC) |
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Lift force: New Theory of Flight
The following information to the reader is being removed by Dolphin51
1. There is no commonly accepted explanation of the generation of large lift at small drag of a wing as expressed as late as 2020 in Scientific American as “No one knows what keeps planes in the air”.
2. Any reference to the peer reviewed published work New Theory of Flight, Journal of Mathematical Fluid Mechanics, 2017, by Hoffman and Johnson, which offers a new explanation, is being removed.
What is the motivation to hiding 1 and 2 from the public? SecretofFlight (talk) 07:00, 31 July 2021 (UTC)
- 1. The Scientific American article titled “No-one can explain why planes stay in the air” is an article that has been seen here before, and has been analysed in some detail. We weren’t much impressed. See Humility in the face of the unknown.
- If you want to initiate a discussion about this Scientific American article you are welcome to do so on this Talk page, but you can see how it has been regarded in the past. Dolphin (t) 07:44, 31 July 2021 (UTC)
- 2. I reverted the following text: A New Theory of Flight first presented in Computational Turbulent Incompressible Flow as a new explanation of the generation of large lift at small drag of a wing based on computing turbulent solutions of Euler's equations supported by mathematical analysis, has been developed by J. Hoffman, J. Jansson and C. Johnson. See my diff.
- This text said almost nothing about the new theory of flight, but it gave prominence to the authors. On Misplaced Pages, the authors of cited sources are not identified in the article, but they should be identified in an in-line citation.
- If you are one of Hoffman, Jansson or Johnson, or you have a close association with them, there may be a Conflict of Interest.
- There may be a case for adding this information to the article but it should be added in accordance with encyclopaedic standards. I recommend you have a look at some or all of the following:
- Regards, Dolphin (t) 08:57, 31 July 2021 (UTC)
The book Understanding Aerodynamics by Doug McLean gives hard evidence that a common agreement on a scientific explanation of the generation of large lift at small drag of an airplane wing is missing, as just one piece of evidence to this very remarkable fact expressed in the Scientific American article. Why should Misplaced Pages hide this state affairs from the public?
Why is any reference to the New Theory of Flight, which gives the first full scientific explanation backed by solid math and computation, , removed?
Are you open to a section explaining the essence of the New Theory of Flight? Yes I am one of the authors (Johnson). — Preceding unsigned comment added by SecretofFlight (talk • contribs) 08:59, 31 July 2021 (UTC)
- You have written about a "common agreement on a scientific explanation of ... lift ..." You have also referred to "this very remarkable fact". In the past decades we have seen many examples of people who believe there can only be one truly correct explanation of aerodynamic lift. These people seem to think "my explanation is correct so all other attempts at explanation must be incorrect." Similarly, there is no reason to expect that scientists will reach agreement on one truly correct way to explain aerodynamic lift. The majority of Users who work regularly on the topic of lift reject as nonsense these suggestions that there is only one truly correct explanation of lift. We also reject as nonsense the suggestion that scientists should reach agreement on one explanation of lift, or that there is something mysterious or sinister in the fact that different scientists display expertise in different ways to explain lift.
- The reason your edits have been erased has nothing to do with wishing to hide your theory from public view - it has everything to do with the way it is written and presented in the article. To see how a theory should be written and presented, look closely at the various theories already firmly entrenched in the article - see Sections 2, 4 and 6 in the list of Contents. Also look at the 5 guidance articles I linked in my previous edit. Of course we are open to a section covering a new theory of flight - but it needs to be written in a way that is compatible with the encyclopaedic standards applied across Misplaced Pages. I recommend you draft the section and present it on this Talk page, or on your own personal sandbox, and then use the Talk page to invite interested Users to peruse it and make their comments.
- Please remember to sign your Talk page edits with four tildes. Dolphin (t) 13:06, 31 July 2021 (UTC)
- Your latest addition to the article (see the diff) looks like an advertisement for a book or a public lecture, rather than a scholarly entry in an encyclopaedia. It contains no in-line citation of the kind required on Misplaced Pages. You have written "The new theory reveals the true physics of generation of large lift ..." The true physics - wow, that is a bold claim indeed! It is not an appropriate claim to make on an encyclopaedia, especially when you have correctly revealed that you have a potential conflict of interest in all matters of the New Theory of Lift.
- I suggest you look carefully at the existing content of this article and revise your additions so they look consistent with the rest of the content. Dolphin (t) 13:19, 31 July 2021 (UTC)
- It also only cites one primary source and a self-published source. According to the manual of style's guidance for reliable sources:
- Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.
- It also only cites one primary source and a self-published source. According to the manual of style's guidance for reliable sources:
- So, the latest edit fails to meet basic inclusion criteria. Mr. Swordfish (talk) 23:06, 31 July 2021 (UTC)
I appreciate that I can have a discussion with Misplaced Pages on the important scientific question about "what keeps planes on the air" citing Scientific American 2020 reporting that "nobody knows". The fact that this question does not have a proper answer more than 100 years after the take off of powered human flight in 1903 is very remarkable, impossible to understand for the general general public, and kept as a secret kept within the scientific community of fluid dynamics hidden from the public. Yet it is true, and the evidence is massive. There is no convincing theory of flight in the standard scientific literature, and this is clearly evidenced by the Misplaced Pages article on Lift presenting lots of material but no theory claimed to be correct, because there is none. If there was a correct theory, known to be correct, then Misplaced Pages would present this theory and all incorrect theories now being presented would serve no role. The New Theory of Flight is a new scientific theory for the generation of lift at small drag of a wing with massive support from computation and mathematical evidence developed by leading academicians and published in leading peer reviewed journals opening a new window in the AIAA HiLift Workshops. Misplaced Pages can here serve an important role to expose this new theory to the scientific community for scrutiny and the general public for information. Can we agree on this mission?SecretofFlight (talk) 18:39, 31 July 2021 (UTC)
Regarding the Scientific American article, it's a pretty clear case of journalistic malpractice. John D. Anderson said "There is no simple one-liner answer to this...” The author misrepresented his statement as "What Anderson said, however, is that there is actually no agreement on what generates the aerodynamic force known as lift." which is a completely different statement.
This was further compounded by the headline writer (often headlines are written by someone other than the author of the article, so I don't know precisely who to blame here) who turned that into the sensationalist click-bait headline "No One Can Explain Why Planes Stay in the Air" It's utter crap. That said, if the author had turned down the hyperbole there's a decent article there.
Regarding Hoffman et. al. to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. As such it's WP:FRINGE. Perhaps that will change, but until it does, their work doesn't belong in the article. Maybe Doug can add some perspective here.
While it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic, from internal combustion engines to cheese making. There's nothing mysterious going on here - there are very well established models of lift that are quite well understood, at least by practicing aerodynamic professionals. What has happened is that for the better part of the 20th century the most common simple explanation turned out to be just plain wrong, and when that was pointed out, people being human held tightly on to it because nobody ever wants to admit that they were wrong. Much debate and argument followed, with disagreement on how best to take a complex subject and explain it simply. That's very different than "nobody knows" or even "there is no agreement on the (mathematical) theory." Were we to propagate the "nobody knows" shibbolleth we'd be remiss in our duties as wikipedia editors. Mr. Swordfish (talk) 21:46, 31 July 2021 (UTC)
Yes, it is a good idea to call in Doug McLean who has written an excellent book on flight theory with an attempt to come up with something better than the standard theories all know to be incorrect. I have written a post on my blog which I ask you to read and answer the questions posed at the end. Will you do that?SecretofFlight (talk) 11:00, 1 August 2021 (UTC)
- Yes, I have read your blog as you requested. I deplore the fact that you have named @Mr swordfish: in your blog in the way you have done, presumably without their consent or prior knowledge. This is immature behavior that is unlikely to find any support in the scientific community.
- At the end of your blog you ask several questions. All your questions are rhetorical. I'm sure you don't know what a rhetorical question is, so I will explain. A rhetorical question is one that is asked without any genuine expectation of an answer; usually because no answer exists or because no answer is wanted. For example, "Why do we have to endure this horrible Covid pandemic?" is a rhetorical question. In a genuine scientific or philosophical dialogue people say what they mean; they don't ask rhetorical questions.
- I am building a picture of User:SecretofFlight as a somewhat immature and petulant person; someone more interested in advertising his theory than promoting the best quality article on Misplaced Pages. Please grow up or I will stop communicating with you. Dolphin (t) 12:51, 1 August 2021 (UTC)
You say regarding Hoffman et. al to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. You are not well informed. The New Theory is now through Jansson an important discussion point at the HiLift Workshops collecting world leading competence.
You say that while it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic. This is a misconception about what science is. The main objective of science is to give correct explanations of natural phenomena and it is crucial to distinguish correct theory from false theory. The fact that there is no theory of flight accepted as a correct theory is truly remarkable and efforts to cover up this fact is not science and not in the interest of the public. SecretofFlight (talk) 11:20, 1 August 2021 (UTC)
I did not get any answer on my question posed on my blog so I repeat it here: Why does Misplaced Pages censor any reference to the well documented New Theory of Flight in a Misplaced Pages article on Lift (force), which is only an account of old theories all known to be incorrect? I guess the reason is that the Wikipedians exercising the censorship (Dolphin51 and Mr swordfish) do not themselves carry the scientific expertise required to properly evaluate the merits of the New Theory of Flight and so take the simple way out to dismiss it without any scrutiny. But if so, this is not in the interest of the public. If there is a correct theory of flight, it should not be hidden to the people, in particular not to all people relying on safe air transportation. So I add the following question: Which experts are Misplaced Pages relying on, when dismissing/censoring the New Theory of Flight? SecretofFlight (talk) 18:58, 1 August 2021 (UTC)
- The very simple answer as to why the material was removed is that it does not conform to the various wikipedia policies regarding notability, sourcing, and possibly conflict of interest. Dolphin and I have provided links to the help pages that clearly explain the policies and the reasoning behind them. I would suggest you read them, especially WP:ORIGINAL, WP:NPOV, WP:VERIFY, and WP:AGF I'd also suggest you drop the allegations of censorship - they just make your case look weak.
- I'm sorry that your theory has apparently not attracted the attention you feel it deserves, but wikipedia is not the place to drum up notoriety. In fact it works exactly the opposite way - first the material must become notable, and only then does it warrant inclusion here. In other words, you need to do your PR work elsewhere first; come back when you have the requisite citations. I'll repeat myself, in case you missed it above:
- From reliable sources:
- Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.
- One very clear problem with your edits is that you haven't established notability. Feel free to come back when you can. Mr. Swordfish (talk) 21:30, 1 August 2021 (UTC)
The only reasonable thing to do is to subject New Theory of Flight to scrutiny by some expert such as Doug McLean. My case is strong because I have hard evidence published in leading journals, while the Misplaced Pages article on Lift (force) is very weak as made very clear in the Talk statement above by Doug. The Misplaced Pages article starts out with (see also blog post):
"There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift".
This is very serious disinformation Mr Swordfish. Very serious. You apparently agree with the statement above by Anderson: "There is actually no agreement on what generates the aerodynamic force known as lift". You thus know very well that there is no scientific explanation of lift agreed to be correct (only incorrect ones agreed to be incorrect), yet you let Misplaced Pages inform the people of the World that there is one, or even better that there are many although most (all?) of them are incorrect. You must understand that this against the most basic of all Misplaced Pages principles your refer to: Misplaced Pages should not mislead the people. Who is telling you to do that? To cover up what is a fact reported by experts in serious media.
I want to bring this case to highest level at Misplaced Pages. It is very serious and of great concern to the people. How do I proceed?SecretofFlight (talk) 06:54, 2 August 2021 (UTC)
- User:SecretofFlight: To bring this case to the highest level of knowledge of physics at Misplaced Pages you should take it to the Physics Project team (see Misplaced Pages:WikiProject Physics). You can do this by posting your case at Misplaced Pages talk:WikiProject Physics. Dolphin (t) 12:31, 2 August 2021 (UTC)
- Another course of action, which will more likely bring it to the attention of the "highest level", is to raise the issue on one of the various noticeboards. There is a process for resolving disputes that cannot be resolved on the talk page, and I think this one qualifies. See https://en.wikipedia.org/Wikipedia:Noticeboards#List_of_Wikipedia's_noticeboards Mr. Swordfish (talk) 13:47, 2 August 2021 (UTC)
Thanks for this information. I will now prepare material to take the case New Theory of Flight vs Misplaced Pages Lift (force) to the Physics Project Team and also to Noticeboards.SecretofFlight (talk) 16:02, 2 August 2021 (UTC)
- Please post a link here when you have filed your case(s). Thanks. Mr. Swordfish (talk) 19:11, 2 August 2021 (UTC)
- @SecretofFlight: When a dispute exists a User will sometimes post their case in two different places on Misplaced Pages. When this is realised one of the posts gets deleted promptly so Misplaced Pages’s effort is not divided into two places, potentially producing an ambiguous outcome. I suggest you post first on the Project Physics Talk page and see what happens. If you don’t see a suitable outcome after, say a week, then take it to a Dispute Resolution site. If you post at the Dispute site first it is highly likely that you will be asked to raise the matter first with the subject specialists at Project Physics so they have the opportunity to contribute their views, and their views will be highly valued by others who are trying to arbitrate on any dispute. Dolphin (t) 22:26, 2 August 2021 (UTC)
- Seems to me that @SecretofFlight: has larger issues with how wikipedia makes these kinds of editorial decisions than what is within the normal set of issues that Misplaced Pages:WikiProject Physics deals with. I'm not sure which noticeboard is the best venue to adjudicate this dispute, but my sense is that he will receive a more thorough response at the noticeboards than at Misplaced Pages:WikiProject Physics. But I'll leave it up to him to choose the venue. Mr. Swordfish (talk) 02:14, 3 August 2021 (UTC)
- @SecretofFlight: When a dispute exists a User will sometimes post their case in two different places on Misplaced Pages. When this is realised one of the posts gets deleted promptly so Misplaced Pages’s effort is not divided into two places, potentially producing an ambiguous outcome. I suggest you post first on the Project Physics Talk page and see what happens. If you don’t see a suitable outcome after, say a week, then take it to a Dispute Resolution site. If you post at the Dispute site first it is highly likely that you will be asked to raise the matter first with the subject specialists at Project Physics so they have the opportunity to contribute their views, and their views will be highly valued by others who are trying to arbitrate on any dispute. Dolphin (t) 22:26, 2 August 2021 (UTC)
@Mr. swordfish,Dolphin51: Before I take the case further I pose the following basic questions connecting to e.g the Scientific American article with headline "No One Can Explain Why Planes Stay in the Air. Do recent explanations solve the mysteries of aerodynamic lift?" (i) Is this a correct description of the state of the science of lift according to Misplaced Pages? If not, what is incorrect? (ii) Is there an accepted scientific theory/explanation of the generation of lift at small drag of an airplane wing? If yes, which is this theory/explanation? (iii) Mr. Swordfish states above "It is true that there is no simple, correct, and complete theory of lift". Does this mean that there is a non-simple, correct and complete theory, if so which, or no such thing? (iv) The Misplaced Pages article starts out: "There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift". There seems to be a contradiction between (i)+(ii)+(iii) and (iv), that is a contradiction between the statements (a) There is a commonly accepted scientific explanation of lift, and (b) There is no commonly accepted scientific explanation of lift. Which of (a) and (b) is the view of Misplaced Pages? I want a clear answer, not handwaving that (c) they are both correct since there are many theories carrying different elements, some true some false. It is against this background the New Theory of Flight stands out as the first explanation in both mathematical and physical terms of the generation of lift at small drag of a wing with solid documentation in the scientific literature, which you remove from visibility on Misplaced Pages. The matter is serious. The role of Wikepedia is to give correct information to the people, not double messages that there both is and is not a scientific explanation of lift. Ok?SecretofFlight (talk) 06:57, 3 August 2021 (UTC)
- My views on this matter, and my answers to your questions, are all evident in the posts I have made to this thread. I suggest you take your case further. I will respond there. Dolphin (t) 12:40, 3 August 2021 (UTC)
- I agree. We've both already responded to most of this upthread. I fail to see the utility in discussing it further here. Mr. Swordfish (talk) 13:43, 3 August 2021 (UTC)
@Mr. swordfish,Dolphin51: No, you have not answered my questions in your posts! To take the case further it is necessary to make the present standpoint of Misplaced Pages clear on the matter of scientific explanation of lift. You say you will respond in the next instance. I ask you to do this right away, so that we will not have to start all over again. You have a responsibility to all the readers of Misplaced Pages and to the scientific community you are representing to answer my questions. What are your answers? SecretofFlight (talk) 13:59, 3 August 2021 (UTC)
@Mr. swordfish,Dolphin51: If you are unable/unwilling to answer the most basic question concerning the article Lift (force) for which you have responsibility, a question of utter scientific importance, then you are not, as I can see, filling the role of a true Wikipedian, which I think will not be appreciated by Misplaced Pages when made clear in the next instance. Do you see my point? You say that answers are to be found in your posts on this thread. Then point me to them! The world expects clear answers. What are your answers?SecretofFlight (talk) 14:34, 3 August 2021 (UTC)
@Mr. swordfish,Dolphin51: You can choose between two roles as Wikipedians: (i) You can go to history by opening to a much needed scientific discussion on theory of flight with in particular new input from New Theory of Flight, in a situation where there is no commonly accepted correct scientific theory of flight and all current theories basically dating back more than 100 years, are known to both experts and people through popular science press, to be incorrect/incomplete. (ii) You can act as gate keepers with a cover up that for sure there are (many) theories of flight, that science is settled and that New Theory of Flight has no place on Misplaced Pages. Which role do you prefer? For help to come to a decision I invite you to Secret of Flight with in particular the videos The Secret of Flight and Incorrect Theories of Flight. SecretofFlight (talk) 15:26, 3 August 2021 (UTC)
Here is state of art of standard fluid mechanics as expressed by Doug McLean in his book Understanding Aerodynamics concerning scientific understanding of lift:
"So in one sense, the physics of lift is perfectly understood: Lift happens because the flow obeys the NS equations with a no-slip condition on solid surfaces. On the other hand, physical explanations of lift, without math, pose a more difficult problem. Practically everyone, the nontechnical person included, has heard at least one nonmathematical explanation of how an airfoil produces lift when air flows past it. Such explanations fall into several general categories, with many variations. Unfortunately, most of them are either incomplete or wrong in one way or another. And some give up at one point or another and resort to math. This situation is a consequence of the general difficulty of explaining things physically in fluid mechanics, a problem we’ve touched on several times in the preceding chapters."
We read that generation of lift of a wing is a secret deeply hidden in the Navier-Stokes equations with no slip (but uncomputable because of very thin boundary layer), while scientific understanding in physical terms is a difficult problem, apparently unresolved (as expressed in Proposed revision of simplified explanations of lift below).
The New Theory of Flight reveals the secret of lift hidden in the Euler/Navier-Stokes equations with slip (without boundary layer and thus computable) in a description of slightly viscous incompressible flow around a long wing as potential flow modified by 3d rotational slip separation at the trailing edge into a turbulent wake, with potential flow generating large lift by attaching to the upper surface while gliding with very small friction as expressed by slip combined with 3d rotational slip separation at the trailing edge without the pressure rise of full potential flow destroying lift.
In short: Standard CFD as Navier-Stokes with no-slip is uncomputable and hides the secret of lift, while Euler/Navier-Stokes with slip is computable and opens to reveal the true secret in a New Theory of Flight in the form of potential flow modified by 3d rotational slip separation. It is as simple as that. Details on Secret of FlightSecretofFlight (talk) 07:48, 2 August 2021 (UTC).
@SecretofFlight: @Mr swordfish: @Dolphin51: I read "The Secret of Flight" paper and found the description to be compelling but somewhat hyperbolic in its claims. Although this material is not yet covered in secondary sources, it is not fringe, and it is recent and I think sufficiently strong to be included here in the article on lift. I've included a short description towards the end of the article, in Three Dimensional Flow, where it seems to fit best. Please consider keeping it, making changes, or delete it if you think this is not a valuable addition to the article, as I believe it is. Dilaton (talk) 21:52, 15 August 2021 (UTC)
- @Dilaton: Thanks for your thoughts on this one. I concede that this new theory might be regarded as sound in some quarters, and might one day be widely accepted among mathematicians as a theory of flight. At present I see nothing to suggest that it is sufficiently mature to warrant mention in Misplaced Pages or any other encyclopaedia aimed at a general audience. We have seen two attempts at describing what this new theory of flight looks like, but I am none the wiser. For example, expressions like:
- 3D vortices. There appears to be nothing on Misplaced Pages to explain 3D vortices so this expression cannot be linked to any existing article to enable the reader to find something about these vortices. (Is this just an alternative to line vortex or vortex filament? Or is it somehow different?)
- potential flow modified by 3D rotational slip separation at the trailing edge into a turbulent wake. This is inaccessible to a general audience. It looks like something from a PhD thesis. Misplaced Pages is not the place for such a thesis.
- the potential flow generates large lift by attaching to the upper surface while allowing a wing to glide with very small drag from turbulent vortex attachment at the trailing edge. Potential flow attached to the upper surface? Surely every application of potential flow around an airfoil since the time of d’Alembert has assumed the flow is attached to the upper surface, and to the lower surface as well? Sentences like this serve more to confuse than to explain.
- If it is to earn a place in this article, it must be described in a way that a general audience might comprehend. Despite your best efforts, your recent addition to the article is unlikely to be comprehended by a specialist audience of fluid-dynamic-literate users, much less by a general audience.
- My view is that your recent addition should be removed. I will wait to see what Mr swordfish and other Users think. Dolphin (t) 07:35, 16 August 2021 (UTC)
- @Dolphin51: Thanks for considering an addition. "3D vortices" is an attempt to convey that these are a collection of vortex filaments of unequal alternating vorticity, with ends attached to the trailing edge. It is essentially a more accurate refinement of the Kutta condition, in which the sheet of shear leaving the trailing edge is now understood as a sheet of turbulent vortices. The improvement of understanding comes in now seeing that this is where the majority of the drag originates on an airfoil. Perhaps the paragraph I attempted to add could be improved with this or other language? Dilaton (talk) 15:38, 16 August 2021 (UTC)
- Misplaced Pages policy is abundantly clear that there must be secondary sources to include material. So far, there has been none for the "new theory of flight" despite a decades long PR campaign that often spills over into Misplaced Pages. The academic article itself has been accessed about 720 times and has garnered a total of 6 citations in the literature. Now, it may be that as Dolphin says it "...might one day be widely accepted among mathematicians as a theory of flight." but for now it's not. I've removed it since it clearly does not meet the standards for reliably sourced material. Mr. Swordfish (talk) 14:48, 16 August 2021 (UTC)
- @Mr swordfish: I understand your concern and respect your adherence to secondary sources; however, WP:NOR does state that primary sources published in reliable places can be used with care, and I think this published article may thus qualify and be used carefully. Or we can do as you wish and wait for someone else to write about it. I do think that would be a bit of a loss, as the improvement of understanding of drag from attached vortices seems significant. Dilaton (talk) 15:38, 16 August 2021 (UTC)
- @Dilaton:While you are correct that primary sources may be used with care, there must be some secondary sources to support notability. At the risk or repeating what I posted upthread, Misplaced Pages policy on reliable sources says:
- Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.
- @Dilaton:While you are correct that primary sources may be used with care, there must be some secondary sources to support notability. At the risk or repeating what I posted upthread, Misplaced Pages policy on reliable sources says:
- @Mr swordfish: I understand your concern and respect your adherence to secondary sources; however, WP:NOR does state that primary sources published in reliable places can be used with care, and I think this published article may thus qualify and be used carefully. Or we can do as you wish and wait for someone else to write about it. I do think that would be a bit of a loss, as the improvement of understanding of drag from attached vortices seems significant. Dilaton (talk) 15:38, 16 August 2021 (UTC)
- Here, we have a paper that was published five years ago and in response the world has shrugged. Now, perhaps it is truly the major scientific breakthrough that the authors claim it to be. Perhaps even you agree that it is and think that the world needs to be told about it. Fine. Go do that. But do it somewhere else. Come back when there are sufficient secondary sources to support the notion that it merits inclusion here. Mr. Swordfish (talk) 23:39, 16 August 2021 (UTC)
I have to say that the sheer volume of debate on these talk pages leads me to believe that the Scientific American article was right after all. --Westwind273 (talk) 05:43, 1 September 2021 (UTC)
- The Scientific American article comprises two distinct elements: firstly there is the title “No-one can explain why planes stay in the air.” and secondly there is the body of the article.
- My impression of the body of the article is that it contains little to support the title. If you believe the body of the article contains some text addressing what the title says, please let us know what you see - please return to this Talk page and quote the wording you are looking at. Many thanks. Dolphin (t) 05:59, 1 September 2021 (UTC)
Proposed revision of simplified explanations of lift
There is a proposal for a revised treatment of simplified explanations of lift available at
https://en.wikipedia.org/User:J_Doug_McLean/sandbox
I think in general it is very good. I think it could be improved by addressing the following issues:
- The current article states "The downward turning of the flow is not produced solely by the lower surface of the airfoil, and the air flow above the airfoil accounts for much of the downward-turning action." This has been removed in the draft. I think it needs to be stated somewhere in the article, otherwise readers may come away with "skipping stone theory"; I'm not seeing a better place than its current location, but I could be persuaded otherwise.
- it doesn't adequately present the streamtube pinching explanation. Probably most of us reading this are already familiar with this "explanation" which can be found in Anderson and Clancy, but the typical reader will probably have no idea what we're talking about. The current article does present it, and I think if we're going to include this material we should explain it more fully than the draft does.
- it asserts :
That's not my understanding of the argument. In the current version of the article (the "streamtube pinching" explanation also starts by arguing that the flow over the upper surface is faster than the flow over the lower surface
which I believe accurately reflects the reliable sources) the streamtube pinching explanation starts with the fact that theory predicts and experiments confirm that the streamtubes narrow on the top of the wing, and proceeds from there. - it lumps streamtube pinching into an "incorrect" subheading, but I'm unconvinced that streamtube pinching is actually incorrect. My view,
which I think is born out by the reliable sources, is that it is a correct description of the physical phenomena, but with the logical problem that it begs the question of why the streamtubes change size. - it claims that speed/Bernoulli explanations come in two basic versions, but there is a third: the half-venturi tube "explanation". There are probably others. I think this can be easily written around, assuming we don't want to drag half-venturi into the article, by replacing "These explanations come in two basic versions" with "There are two common versions of this explanation"
- The final subsection "Alternative explanations, misconceptions, and controversies" is reduced to only one explanation, misconception, or controversy after moving previously contained material upwards. It might be appropriate to address half-venturi, skipping stone, "squeeze the soap" and others here. Or just remove this subsection.
There are probably some other minor edits to avoid repetition and improve readability, but I think if the issues above are addressed the revised material will be ready for publication. Thanks for your efforts on this. Mr. Swordfish (talk) 00:42, 1 August 2021 (UTC)
- Thanks for the feedback. To respond to the issues raised above:
- 1. Yes, let's put this back. And let's find a source to cite for it.
- 2-3. I think the whole paragraph taken together describes the arguments correctly, but I see how it can be confusing if you look at the first sentence by itself. I'll try a rewrite. I don't support retaining the current article's opening statement on what experiments and analyses show. It's a true statement, but no reliable source I know of uses it in the context of a streamtube-pinching explanation of lift, and the current article cites no source for it. My objective is still to stick with the classical sources that propose a reason for the pinching, even if we end up pointing out that the reason doesn't make sense.
- 4. I agree with your comment on "versions". But I still think streamtube pinching belongs under the "incorrect" heading because its two main steps (streamtube pinching causes higher flow speed, and higher flow speed causes lower pressure) run opposite to actual physical cause-and-effect. In addition to not providing a good reason for the pinching, it has the flaw that conservation of mass isn't a satisfying physical reason why the flow would speed up. Really explaining why something speeds up requires identifying the force that makes it accelerate. I'll add the second "flaw".
- 5. The upper-surface-as-an-obstacle and the upper-surface-as-a-half-Venturi are really the same argument. Your rewording is OK with me.
- 6. I'm going to try removing the "Alternative explanations..." subhead and move the "Controversy regarding Coanda effect" sub-subhead up with the flow-deflection explanation, as that's the explanation to which it relates.
I've implemented these changes in my sandbox. Thank you for the suggestions. J Doug McLean (talk) 17:23, 4 August 2021 (UTC)
- I have gone through the proposed text and I find it excellent, and an improvement over the current state of the article. I have a few minor language/typographic fixes in mind, which I think will be better carried out once the text is integrated in the article. -- Ariadacapo (talk) 07:09, 5 August 2021 (UTC)
- Thanks for your consideration of my suggestions.
- 1. I have added a citation for the assertion that the upper surface produces "much" of the lift. I'd like to find a better one, but I think this will do for now.
- 2. My working hypothesis is that the vast majority of our readers will not be familiar with the streamtube pinching explanation. It can be found in Anderson's Introduction to Flight, Eighth Edition, but not in earlier editions (or at least I couldn't find it there), in Clancy's Aerodynamics, and in Eastlake's article for The Physics Teacher. I have been unable to find it elsewhere. A year or so ago I was of the opinion that it was sufficiently obscure that it didn't merit attention in the article, but after acquiring Clancy and seeing it there, my opinion has changed. My best guess is that most people who have taken a college level class in aeronautical engineering have seen it, but it remains mostly unknown to the general population.
- Since we can't expect the reader to already be familiar with it, we should provide a more detailed description - the current draft states "When streamtubes become narrower, conservation of mass requires that flow speed must increase." This is certainly true, but a sentence or two along with a picture will help many readers to understant why narrow streamtubes imply faster flow.
- 3. I think you are correct that the current article's treatment is at variance with the sources. Re-reading Anderson, he starts with "obstruction theory" to explain streamtube pinching, not "Starting with the flow pattern observed in both theory and experiments..." so we should present it his way. Eastlake doesn't explicitly explain why the streamtubes change size, but he alludes to the flow passing "the thickest part of the airfoil" and putting your thumb over the end of a hose, so I'll place him in the "obstruction theory" camp. I don't have my copy of Clancy with me and won't for several weeks, so someone else will need to check that reference.
- 4. The authors of the current section must have been engaging in an act of charity to re-factor the streamtube pinching explanation so that it is not actually incorrect. Seems that we both agree that the current version is not actually incorrect, but it is different than what is to be found in the cited sources. Since the sources present the explanation as a result of obstruction, we should too. And when we do, I think it is appropriate to lump it under the "Incorrect" heading.
- One thing I'd like to see carried over from the current article is
- Sometimes a geometrical argument is offered to demonstrate why the streamtubes change size: it is asserted that the top "obstructs" or "constricts" the air more than the bottom, hence narrower streamtubes. For conventional wings that are flat on the bottom and curved on top this makes some intuitive sense. But it does not explain how flat plates, symmetric airfoils, sailboat sails, or conventional airfoils flying upside down can generate lift, and attempts to calculate lift based on the amount of constriction do not predict experimental results.
- The material expressed in the first sentence has been carried over, but the rest has not. Since the third sentence above is one of the better (best?) arguments why obstruction theory is lacking I think it makes sense to continue to include it.
- 5. Seems to have been taken care of. Thanks.
- 6. Moving the Coanda material up and removing the depleted section on "Alternative theories" makes logical sense. My issue with this version of the draft is that the article now spends more time discussing what is essentially a semantic issue than it does treating the much more central idea of lift as a consequence of conservation of momentum. Moving the Coanda material down in the article would be an acceptable solution, but I'm not sure where to move it. Like the streamtube pinching explanation, I think the "Coanda controversy" is limited to folks who have done some formal study or aerodynamics and not widespread in the general population, so perhaps we don't really need to address it. Or perhaps find a more concise way to present it.
- Thanks for considering my suggestions. I think we're making real progress here. Mr. Swordfish (talk) 14:28, 5 August 2021 (UTC)
- @Mr Swordfish: If at 3. you are alluding to the citation of Clancy p.76 “This lift force ... ... downward momentum of the air” I can confirm that this is an accurate quotation from Section 5.15 Lift and Downwash (which is on p.76 in my copy.) Dolphin (t) 00:19, 6 August 2021 (UTC)
- @Dolphin: My recollection is that Clancy presents the streamtube pinching explanation, but I don't recall whether he starts with "obstruction theory" or proceeds from some other premise (e.g. the "theory & experiment" approach the article uses). We don't cite Clancy in this subsection, so you'll have to look beyond our citations. If you have your copy handy, I'd appreciate if you could take a look at Clancy's approach and report back. Thanks. Mr. Swordfish (talk) 18:18, 6 August 2021 (UTC)
- @Mr Swordfish: If at 3. you are alluding to the citation of Clancy p.76 “This lift force ... ... downward momentum of the air” I can confirm that this is an accurate quotation from Section 5.15 Lift and Downwash (which is on p.76 in my copy.) Dolphin (t) 00:19, 6 August 2021 (UTC)
- @Mr Swordfish: I have had a quick look through Clancy. He explains lift using the Circulation Theory and the Kutta-Joukowsky theorem. The book appears to contain no linking of lift on an airfoil and stream tube pinching. There are several diagrams that show streamlines of varying spacing around a circular cylinder with circulation, and around an airfoil-shaped cylinder with different amounts of circulation. In the explanatory text adjacent to the diagram of the circular cylinder with circulation Clancy draws attention to the varying spacing of streamlines and links this to pressure variation using Bernoulli (Section 4.5 Circular Cylinder with Circulation on p.38) In the text adjacent to diagrams of airfoils Clancy makes no attempt to draw attention to streamline spacing and its implication for pressure.
- In para 4.5(b) Clancy writes “The effect of the circulation is generally to increase the speed over the upper surface of the cylinder and to reduce the speed over the lower surface. This effect is shown by the spacing of the streamlines in Fig 4.4”
- In para 4.5(c) he writes “From Bernoulli’s Theorem, therefore, it follows that the pressure is generally reduced on the upper surface and increased on the lower surface. As a result, there is a net force vertically upwards. This is lift.” Dolphin (t) 13:49, 7 August 2021 (UTC)
- I stand corrected about streamtube pinching appearing as an explanation of lift in Clancy. I'm now back to wondering if presenting this explanation here is giving it undue weight. Mr. Swordfish (talk) 14:17, 7 August 2021 (UTC)
I've been re-reading the Help article on undue weight, first in the context of the streamtube pinching "explanation", but then in the context of the apparent controversy over the Scientific American article that claims "nobody understands lift". The article on weight states
- Neutrality requires that mainspace articles and pages fairly represent all significant viewpoints that have been published by reliable sources, in proportion to the prominence of each viewpoint in the published, reliable sources. Giving due weight and avoiding giving undue weight means articles should not give minority views or aspects as much of or as detailed a description as more widely held views or widely supported aspects.
The current version of the article states succinctly "...there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift." The proposed revision does an about face and states "...neither approach, by itself, is a completely satisfactory explanation." (And then there's the SA article, which I'm going to ignore as WP:FRINGE.)
Both of these are valid opinions that are supported by reliable sources. I tend to agree with the latter as my own opinion, but when I put on my editing hat I find it problematical to clearly come down on one side or the other. If we're going to present this controversy, we're supposed to present both sides and "teach the controversy". That said, I don't want to waste our readers' time by rehashing the great Bernoulli v Newton debate that raged back in the late nineties. My preferred solution is to sidestep the issue and avoid sweeping statement about whether both are right, or neither is right, (or whether nobody really knows). The proposed revision clearly explains each approach and its limitations or shortcomings. I think the readers can draw their own conclusions without us having to make sweeping statements like the above examples.
I'll copy the present proposal over to my sandbox and make the proposed changes there so we retain an easy to access "clean" copy of Doug's proposal.
Regarding the streamtube pinching, or "obstruction theory", I'm in agreement that it's essentially the same argument as the "half venturi tube" approach, which seems to be more prevalent in the sources so we should give more prominence to it. I'll take a whack at that, along with an attempt to provide a more concise treatment of the Coanda material. Mr. Swordfish (talk) 13:44, 10 August 2021 (UTC)
- My view is that there are multiple explanations of lift, each derived from one or more of the various conservation laws and other laws of physics that are applicable to a solid object immersed in the flow of a fluid. We make use of multiple explanations of lift to serve the needs of the multiple audiences that have an interest in the subject. Even within one audience there are multiple purposes and objectives that cannot be satisfied by just one explanation. For example:
- An explanation of lift that can be presented to 19-year olds will be unsuitable for 13-year olds. An explanation that is both satisfying and satisfactory for student pilots will be unsuitable for students of physics and engineering.
- An explanation that helps explain lift in 2-dimensional flow will not be satisfactory if the objective is to help explain lift-induced drag.
- I support the sentiment in the present article: “Either can be used to explain lift.” I don’t support the sentiment that "...neither approach, by itself, is a completely satisfactory explanation." It will be unhelpful, unnecessary and unsound to apologise for certain explanations of lift, or to suggest that no satisfactory explanation exists, or that no-one knows what it is. Misplaced Pages is able to demonstrate its maturity and soundness by not engaging in a search for a "completely satisfactory explanation". Nor should Misplaced Pages support a notion that every incomplete explanation must be incorrect.
- When we search for the most appropriate explanation of lift for our purposes we are engaging in applied science or applied math or engineering but we aren’t engaging in pure or fundamental science. Bernoulli’s principle and Newton’s laws of motion have universal application and so qualify as fundamental science, but an explanation of lift on an airfoil is simply one of many examples of Bernoulli and Newton in action. There will never be a Committee of eminent scientists whose task is to determine by arbitration the one true explanation of lift.
- When we talk about the explanation of lift based on Bernoulli’s principle, it would really be more accurate to say we are using lift as an example of Bernoulli’s principle in action. Similarly, when we talk about the explanation of lift based on Newton’s laws, it would really be more accurate to say we are using lift as an example of Newton’s laws in action. The pure science is always more fundamental than the application of that science to one of a multitude of everyday observations.
- I look forward to seeing your latest proposal on your sandbox. Dolphin (t) 12:10, 11 August 2021 (UTC)
- Dolphin, Agree that different audiences require different explanations, and it is appropriate for us to present several, starting with the easier to understand and proceeding to the more rigorous. I think we need to be careful about using words like "satisfying" and "satisfactory" because they beg the question of "satisfying to whom?" My hunch is that most people are completely satisfied to know nothing about this topic. Those who bother to read the article may come away satisfied after a section or two, or they may read further until they are "satisfied".
- Moving on....
- The opinion “Either can be used to explain lift.” is just that - an opinion. So is the opinion "...neither approach, by itself, is a completely satisfactory explanation." If we're going to include either one, we need to present the other, present both as opinion, and provide some context for how widespread each is in the reliable sources. I'd rather not do that, especially early on in the article. Perhaps a later section on the "Bernoulli v Newton Controversy" would be in order, or perhaps a separate article instead. My preference is to just sidestep it as a distraction and present the various approaches, starting from simple and moving to the complex, with some context to address whatever shortcomings or limitations each approach has. And let the material speak for itself without making unnecessary sweeping generalizations.
- To that end, I don't think we need the first section "Understanding lift as a physical phenomenon". The article starts with qualitative physical explanations without math and proceeds to the various mathematical models. That is apparent from the table of contents, so I don't think we need to state it explicitly; readers will get it if they bother to read that far. I'm going to remove it from my draft. Comments appreciated.
- My view is that no version is 100% complete nor is any version 100% correct. When we do physics, we make abstract models, and in order to make the models tractable we make some simplifying assumptions along the way so the model doesn't exactly describe the actual physical phenomena. That doesn't mean that the models are bad, just that they are always limited, and when criticized for that variance the criticism is often warranted. For instance, 2D potential flow doesn't predict stall, drag, or downwash. But it does a surprisingly good job at predicting lift without making the math impossible. IOW, it's a good but limited model.
- Which is to say that every explanation is incomplete to some degree. So, I'm not sure it's "fair" to label the explanation based on flow deflection and Newton's laws that way in the title. I do think it's fair to state that it's incomplete in the body, so I'm removing it from the title but leaving it in the body.
- Regarding "Bernoulli-based" explanations, the two we discuss in that section are clearly incorrect. Correct explanations involving Bernoulli (or more properly, explanations that are based on models that have some predictive power) always include many other physical principles to the extent that it's a misnomer to call them "Bernoulli-based". To put a finer point on it, they always include conservation of momentum at some level. Bernoulli's principle is just one piece of the puzzle.
- That said, I think a serious shortcoming of this draft as it stands is that readers may come away with the notion that Bernoulli's principle is somehow wrong, or that it is always incorrect to use it when explaining lift. I think we need so say something along the lines of "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." But I'm not sure where to put it or how best to phrase. Suggestions appreciated. Mr. Swordfish (talk) 18:32, 14 August 2021 (UTC)
- UPDATE: I've added "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." to the draft. Mr. Swordfish (talk) 18:49, 14 August 2021 (UTC)
I've not gotten much feedback on the draft in my sandbox. I'm not sure if that's because other editors don't like it, or because they think it's fine as is. Assuming the latter, I'll give it a couple of days and if no objections I'll deploy the material in my sandbox. Mr. Swordfish (talk) 22:02, 19 August 2021 (UTC)
- I will be happy to give some feedback in the next day or two. Dolphin (t) 22:42, 19 August 2021 (UTC)
- Thanks. It's more important that we get it right than that we do it fast. But I want to keep the process moving. Mr. Swordfish (talk) 01:41, 20 August 2021 (UTC)
- It looks good to me and I don’t see much to comment on. I have provided my feedback at User talk:Mr swordfish/sandbox. Dolphin (t) 13:31, 20 August 2021 (UTC)
- Thanks. It's more important that we get it right than that we do it fast. But I want to keep the process moving. Mr. Swordfish (talk) 01:41, 20 August 2021 (UTC)
I think the proposed new section "Understanding lift as a physical phenomenon" is important. It clarifies the status of the qualitative explanations relative to the rigorous scientific understanding embodied in the mathematical theories. In so doing, it says a lot more than what a reader could infer from the TOC or what he would be likely to realize even after reading the entire article. I think it makes what follows much easier to understand.
I think we should keep the "Obstruction..." explanation. Anderson is a very prominent author, and this book is a prominent source.
I've put up a new candidate in my sandbox. It avoids the "satisfactory" wording and removes the value judgements from the headings. It also incorporates Swordfish's shortened version of the Coanda section and his separate subheads for "Equal transit time" and "Obstruction...". I added another subhead to separate out the issues common to both explanations that had been swallowed into the "Obstruction..." subsection. I also incorporated his wording on Bernoulli not being incorrect as a principle, with the added qualification that Bernoulli is applicable outside the boundary layer. Comments? J Doug McLean (talk) 19:21, 21 August 2021 (UTC)
- I've copied Doug's latest draft over to my sandbox for the purposes of comparison. The diff is here: https://en.wikipedia.org/search/?title=User%3AMr_swordfish%2Fsandbox&type=revision&diff=1040264566&oldid=1039805588 I'll have more to say in a day or so. Mr. Swordfish (talk) 17:29, 23 August 2021 (UTC)
Comments on the latest drafts (24 Aug 2021):
o The first thing I noticed when looking at the diff was that the latest version from Doug is some 10,000 characters shorter. This is mostly refs that didn't make it over. I don't think it will be controversial to restore the refs, although some may be ripe for pruning. I'll restore all of them in my next draft, and if any are deemed to be unnecessary we can remove them on a case-by-case basis.
o Regarding the first section , it reads to me as an opinion rather than a simple statement of fact. The current version of the article also includes the opinion that "Either can be used to explain lift." I prefer the simple factual statement in my previous draft, which I think adequately foreshadows the qualitative vs mathematical dichotomy to come.
- There are several ways to explain how an airfoil generates lift. Some are more complicated or more mathematically rigorous than others; some have been shown to be incorrect. Most simplified explanations follow one of two basic approaches, based either on Newton's laws of motion or on Bernoulli's principle.
o I looked into other wikipedia articles that link directly to sub-headings, and only found one that would be affected by the current drafts. I added an anchor tag to that section. We should make sure that it makes it into the final version.
o Agree to keeping the obstruction/constriction/streamtube-pinching explanation. While it's not nearly as widespread as the ETT fallacy, it seems to be common enough for us to reference it here (although I'd be open to an argument that it's not if anyone wants to make it). I think it's worth expending a single sentence on NASA's "Venturi tube" version of it since NASA's site may be the most widely read version.
o I don't think labeling the incorrect explanation as "incorrect" is a value judgement. Seems to be simply a statement of fact, so I'd advocate restoring that in the titles.
o I like the additional subhead to address issues common to both - I wanted to do that myself, but couldn't come up with a good title.
o I'm unconvinced that it's necessary to state that "Bernoulli's principle is applicable to the flow outside the boundary layer." at this point in the article. I think simply stating "Bernoulli's principle can be used correctly as part of a more complicated explanation of lift." is sufficient for the intended audience for this portion of the article. If we're going to address when Bernoull's principle applies and when it doesn't, that should wait until later in the article.
o Regarding "This explanation is correct as far as it goes but is incomplete. " I've come to agree with Dolphin's that "as far as it goes" is a colloquial idiomatic expression, that while common in the US may not be understood the way it's meant to by someone unfamiliar with the expression. If we were writing this for a US audience I'd advocate to keep it, but since we're writing for the broader English-speaking world I think the phrase should be excised. We have two candidates for the material at this point:
- This explanation is correct but it is incomplete. It doesn't explain how the airfoil can impart downward turning to a much deeper swath of the flow than it actually touches. Furthermore, it doesn't mention that the lift force is exerted by pressure differences, and doesn't explain how those pressure differences are sustained.
and
- Flow deflection combined with Newton’s laws is a helpful way to explain some aspects of lift. It leaves some questions unanswered; it doesn't explain how the airfoil imparts downward turning to the flow, and it doesn't mention that the lift force is exerted by pressure differences. It doesn't explain how those pressure differences are sustained.
I prefer the concise "correct but incomplete" phrasing, but could be persuaded otherwise.
I'll merge the the latest draft from Doug with mine, incorporating the ideas above. Comments as always welcome. Mr. Swordfish (talk) 16:32, 24 August 2021 (UTC)
Oversimplification
The current version of that section still refers to Bernoulli's Principle as "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." This sounds great, but it isnt correct, as it is a (fairly significant) oversimplification of his work. In the context of aviation and aerodynamic lift, it is only accurate along a streamline where no heat is being transferred between the wing and the air. Does the cited work include this gross oversimplification? As importantly, does the gross oversimplification make the concept clearer to the reader? PrimalBlueWolf (talk) 08:26, 23 August 2021 (UTC)
- @PrimalBlueWolf: Where you have written “but it isn’t correct ...” do you mean Bernoulli’s principle doesn’t correctly represent the reality; or our article doesn’t correctly reflect the principle described by Bernoulli?
- It is well known, and always acknowledged in reliable published sources, that Bernoulli’s principle doesn’t take account of viscous forces within the fluid, nor does it apply to a flow field in which heat is being transferred. Despite these assumptions Bernoulli’s principle is a very powerful tool in analysing the subsonic flows around streamlined bodies. I don’t agree with your characterisation that the Misplaced Pages article represents a “gross oversimplification.” Please explain further. Dolphin (<.,span style="color: blue;">t) 13:57, 23 August 2021 (UTC)
That it doesn't correctly represent the principle as represented in Hydrodynamica. The current version of the article alleges that you can determine velocity and pressure of any other point using Bernoulli's Principle knowing only the velocity and pressure of one point, and the velocity of one other point. That is only valid along a streamline, but the article doesn't acknowledge that. PrimalBlueWolf (talk) 21:25, 23 August 2021 (UTC)
- It is often stated that "Bernoulli's principle is only valid along a streamline" but this is a misconception. Within a flow field that exhibits uniform flow as the initial condition, BP applies throughout the flow field. This assumes that the energy is constant, i.e. it assumes no heat loss (as one would find in the example of an airplane wing) or no net work done (as one would find in the example of a sailboat). If one is going to pick nits, BP is not applicable to any real world airfoil due to these energy considerations, however it is commonly used as a approximation or simplification to make mathematical models tractable. Physics is full of these approximations, e.g. assuming sin(x)=x for sufficiently small x. And if we're not going to assume constant energy, BP doesn't apply along a streamline either.
- The statement "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." is consistent with how BP is used in practice in mathematical analysis of fluid dynamics. Granted, it's a calculational shortcut that does not precisely model the actual physical world. But it's close enough for engineering work. Note that the section is about "simplified explanations" and is not the proper place for a long technical discussion of exactly when BP applies and when it doesn't. Mr. Swordfish (talk) 03:28, 24 August 2021 (UTC)
@PrimalBlueWolf: As you can see, I have moved your posts and the responses from me and @Mr swordfish: to their own thread under this new heading.
You have written “That is only valid along a streamline, …” That is incorrect in the case of a wing generating lift in the atmosphere. Consider the following:
In Fluid Mechanics by V.L. Streeter (1951 McGraw-Hill), section 3.7 The Bernoulli Equation says:
The constant of integration (called the Bernoulli constant) in general varies from one streamline to another but remains constant along a streamline in steady, frictionless, incompressible flow. These four assumptions are needed and must be kept in mind when applying this equation.
Under special conditions each of the four assumptions underlying Bernoulli's equation may be waived.
1. When all streamlines originate from a reservoir, where the energy content is everywhere the same, the constant of integration does not change from one streamline to another and … may be selected arbitrarily, i.e. not necessarily on the same streamline.
In Aerodynamics by L.J. Clancy (1975 Pitman Publishing) section 3.4 Bernoulli's Theorem for Incompressible Flow says:
Further, at some distance upstream of the aircraft, the flow consists of a uniform stream. It follows that on any given streamline in this region the value of p + 1/2 ρ v is the same as it is on any other streamline.
In Fundamentals of Aerodynamics by John D. Anderson (1984 McGraw-Hill) section 3.2 Bernoulli's Equation says:
For a general, rotational flow, the value of the will change from one streamline to the next. However, if the flow is irrotational, then Bernoulli's equation holds between any two points in the flow, not necessarily just on the same streamline.
In the language of fluid dynamics we say Bernoulli's principle applies equally at all points on all streamlines in a region of irrotational flow. A wing operates in a stationary atmosphere so there are no viscous forces or vorticity in the air outside the boundary layers. The flow around a wing is irrotational everywhere except in the boundary layers.
You have also written “… only accurate along a streamline where no heat is being transferred between the wing and the air.” I assume you are referring to transonic and supersonic flow. The Misplaced Pages article presently only refers to lift in subsonic flight. In low-speed flight there is no significant amount of heat being transferred. Dolphin (t) 04:32, 24 August 2021 (UTC)
I'm glad to take the correction and agree with the reasoning. Thanks for the detailed and well sourced explanation. PrimalBlueWolf (talk) 07:19, 24 August 2021 (UTC)
Proposed new version of simplified explanation continued
The last thread had gotten rather long, so starting a new one.
Latest version now available in my sandbox.https://en.wikipedia.org/User:Mr_swordfish/sandbox
I opted to keep the opening section, at least for now, but as it stands now there is substantial repetition between it and the first paragraph of the next section. Not sure what is the best solution, but I'm out of time for the day. Comments and suggestions appreciated. Mr. Swordfish (talk) 15:33, 26 August 2021 (UTC)
- I spent some time today looking at other Misplaced Pages articles on technical, mathematical, or scientific subjects. I came away with two observations:
- The articles discuss the topic at hand, rather than discussing the article and how it covers the topic.
- None of them have language that implies that the topic is difficult to explain or to understand.
- With that in mind, the opening section "Understanding lift as a physical phenomena" would be an outlier in terms of Misplaced Pages style. The more matter-of-fact treatment in the section that follows is in keeping with wider Misplaced Pages standards.
- See Aerodynamics, Wing, Quantum Mechanics, Fluid Mechanics, Fluid Dynamics, Chemistry, Category Theory for a few examples.
- On that basis I'm going to remove the section from the draft while repurposing some of the language into the new first section. At this point, I think we have a release candidate. Comments? Mr. Swordfish (talk) 15:31, 27 August 2021 (UTC)
- I agree. I encourage you to release the latest version. Dolphin (t) 13:35, 28 August 2021 (UTC)
- It's been released. Thanks to everyone who contributed. Mr. Swordfish (talk) 21:06, 28 August 2021 (UTC)
- I agree. I encourage you to release the latest version. Dolphin (t) 13:35, 28 August 2021 (UTC)
Sorry for not weighing in sooner on the latest changes. I've been away for a few days.
I see that the proposed new section has been removed again and that some of the language has been "repurposed" into the following section. It seems to me that these changes have negatively impacted the article's organizational clarity. The first mention of the mathematical theories now comes under the heading "Simplified explanations.....", and with this placement the mathematical theories are now categorized as one of "several ways to explain how an airfoil generates lift". This isn't an accurate reflection of where the mathematical theories fit in the overall picture. The mathematical theories are the basis of the rigorous scientific understanding of lift. They're not "explanations" of lift.
I think the proposed new section reflected the facts of the matter more clearly. Except for the phrase (referring to the simplified explanations) "and most readers will likely already have been exposed to one or more of them", which I propose we delete, everything that remains is a straightforward statement of fact. Even the one bit of "meta" information ("These issues are discussed in connection...") is a factual statement that more detail on the issues just raised is coming later in the article, not a "discussion" of "how the article covers the topic".
I don't think that providing a bit of factual meta information is out of place in a Misplaced Pages article. Nor is it out of place to say that a correct qualitative explanation of lift is difficult, given that it's a statement of fact supported by the checkered history of qualitative explanations and by the sources (my TPT paper, at least).
I've tweaked the proposed new section and removed its heading, which makes it part of the "Overview" section, where I think it fits well. I've also taken a crack at removing the resulting duplication from the intro to "Simplified physical explanations..." in my sandbox. My recommendation is to merge these changes into the article in place of the recently released version. J Doug McLean (talk) 19:27, 2 September 2021 (UTC)
- Thanks for your continued effort on this page. I've made an attempt to merge your latest version with the current article. It's in my sandbox. https://en.wikipedia.org/User:Mr_swordfish/sandbox#Overview Comments appreciated. Mr. Swordfish (talk) 20:12, 4 September 2021 (UTC)
- Mr Swordfish: I have no objection to the current version in your sandbox being released. Dolphin (t) 12:52, 6 September 2021 (UTC)
- Mr Swordfish: Your rendition of the addition to "Background" is more cryptic than my draft, but I'm on board with all of it except the last sentence, which seems to me to be ambiguous. Actually, I think all, not just some, of the simplified explanations we present have the flaw of leaving important things unexplained, even the ones that also have incorrect elements. A possible revision:
- There are also many simplified explanations, but all leave significant parts of the phenomenon unexplained, while some also have elements that are simply incorrect.
- I think we're almost done and on the verge of completing a significant improvement of the article. J Doug McLean (talk) 00:54, 7 September 2021 (UTC)
- I have implemented the suggested change in my sandbox and will deploy that version. However, I failed to start with the latest version from the real article and several changes have been made since I deployed the version from my sandbox so I can't just do a cut and paste or it will override those changes. So, there will be several intermediate versions in my sandbox as I reconcile the two. Mr. Swordfish (talk) 13:46, 8 September 2021 (UTC)
- I think we're almost done and on the verge of completing a significant improvement of the article. J Doug McLean (talk) 00:54, 7 September 2021 (UTC)
Coandă effect criticism
The following sentence was recently added:
- A criticism of the Coandă effect as an explanation for aerodynamic lift is that the Coandă effect itself is not well understood.
With a cite to https://digitalcommons.usu.edu/cgi/viewcontent.cgi?article=1096&context=etd
The relevant part of that paper says:
The Coanda effect has been widely used in the both aeronautics and medical applications , air moving technology, and other fields. Nevertheless, this phenomenon is not completely understood, especially for three-dimensional flow as in the CSM design. The nature of the Coanda effect, with boundary layer separation and entrainment interaction, make for difficulty in solving the flow numerically and analytically.
I'm not seeing where the source criticizes the usage of the Coandă effect to explain lift, so this material appears to be WP:SYNTHESIS. A bigger problem is that saying that "the Coandă effect itself is not well understood" is a very broad statement that would need stronger backing than the carefully worded excerpt from the cited Masters Thesis above. Reading the Coandă effect article I don't see anything supporting the assertion that it is not well understood - were this truly the case I would expect it to be treated in that article.
Of course, that wikipedia article is not dispositive - we're supposed to look at reliable sources, and other wikipedia articles are not reliable sources - but it strikes me that if we're going to publish a broad assertion like that the proper venue for discussing it and presenting the source material would be the talk page for that article, not this one.
I'm removing the material pending the production of better citations. Mr. Swordfish (talk) 20:32, 9 March 2022 (UTC)
- I agree with Mr. Swordfish that better citations are necessary. However, as far as I have been able to determine, there are no sources that offer a well thought out explanation for why or how the Coandă effect applies to aerodynamic lift. The popular references quoted in the main article (references 33 and 34) certainly do not offer that explanation. This lack of a source making a detailed argument for applying the Coandă effect to aerodynamic lift is not apparent in the main article. I tried to make this deficit of a source argument, not vey well I must agree, but one that should be made. It is difficult to make this argument since there are no referenceable sources that point out this deficit of a source offering a valid explanation. David Weyburne (talk) 16:51, 10 March 2022 (UTC)
- Were I writing this article for myself, I'd include something like:
- People often try to explain why the air is deflected on the top of the wing by saying it's because of the Coandă effect, but this doesn't actually explain anything, it just gives it a fancy European name.
- But I'm not allowed to just make stuff up on my own and I haven't seen this idea expressed elsewhere so I don't have a source for it. And that means I can't add it to the article. That said, I agree with the sentiment that it's poor pedagogy to explain something via material that the reader doesn't understand either. And I think the article would be improved with a short statement like the one above or something similar to what you added, but unless we can find reliable sources to cite we can't add it. If you find a good source for this I'm all ears. Mr. Swordfish (talk) 23:23, 10 March 2022 (UTC)
- Were I writing this article for myself, I'd include something like:
Anderson and Eberhardt's "Understanding Flight" (McGraw-Hill, 1st ed. 2001) is the one source I know of that appeals to the Coanda effect in a lift explanation and also tries to explain how Coanda works in physical terms. They attribute the Coanda effect entirely to viscous "shear forces." On p. 23, after explaining no-slip at the surface and the resulting formation of a boundary layer, they say:
- "The differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer. This causes the fluid to try to wrap around the object."
This explanation of Coanda is easy to rebut. However, my own book ("Understanding Aerodynamics", Wiley, 2012) is the only citable source I know of that does so explicitly. With reference to using Coanda in lift explanations, I say in sec 7.3.1.7:
- "The Coanda effect is erroneously seen as implying that viscosity plays a direct role in the ability of a flow to follow a curved surface. Anderson and Eberhardt assert that viscous forces in the boundary layer tend to make the flow turn toward the surface, specifically, as they put it, that the 'differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer.' Actually, there is no basis in the physics for any direct relationship between shear forces and the tendency of the flow to follow a curved path."
In the paragraphs following the above, I explain in detail my reasons supporting the statement in that last sentence. The gist of it is that the curving of the flow is a result of the interaction between the pressure field and the velocity field, as we explain in the article under "A more comprehensive explanation." It has practically nothing to do with viscous or turbulent shear stresses. As long as the boundary-layer doesn't separate, the curving of the flow to follow the curved surface is an essentially inviscid effect.
Mr. Swordfish has invited us to identify a citable source for his naming-isn't-explaining objection to relying on Coanda. Again, the only one I know of is my own book. In sec 7.3.2 I list things to avoid in an explanation of lift. Item 5 is:
- "'Naming' as a substitute for explaining, as, for example, in saying that a jet flow follows a curved surface because of the Coanda effect, where 'Coanda effect' is just a name for the tendency of jet flows to follow curved surfaces."
So we have citable sources for a couple of possible additions to the Coanda subsection that would be of interest to some readers. I'm not enthusiastic about doing it, however, because I think we may already be giving Coanda more prominence than it deserves. On the other hand, I could argue that the article as it stands doesn't present enough of the case against Coanda, and that the additions we're considering here would balance things better and help justify the word "Controversy" in the article's section heading.J Doug McLean (talk) 20:20, 3 April 2022 (UTC)
- Thanks very much Doug. Mr swordfish and I will ensure your book is cited as a source where it is appropriate to do so in relation to Coanda effect. Dolphin (t) 23:49, 3 April 2022 (UTC)
- Now that we have a cite I've been trying to craft language along these lines, but so far haven't come up with anything that doesn't seem out of place or unencyclopedic. I'll keep trying. Suggestions cheerfully considered. Mr. Swordfish (talk) 23:56, 11 April 2022 (UTC)
- Mr swordfish and J Doug McLean I have inserted a paragraph that, hopefully, begins to capture some of Doug's wisdom from above. See my diff. Dolphin (t) 04:41, 27 September 2022 (UTC)
- I have also added a sentence on "naming is not explaining". Mr. Swordfish (talk) 18:55, 28 September 2022 (UTC)
- Mr swordfish and J Doug McLean I have inserted a paragraph that, hopefully, begins to capture some of Doug's wisdom from above. See my diff. Dolphin (t) 04:41, 27 September 2022 (UTC)
- Now that we have a cite I've been trying to craft language along these lines, but so far haven't come up with anything that doesn't seem out of place or unencyclopedic. I'll keep trying. Suggestions cheerfully considered. Mr. Swordfish (talk) 23:56, 11 April 2022 (UTC)
A new simplified lift explanation
As if things weren't complicated enough, I have developed a new simplified explanation for aerodynamic lift that I would propose as a add-on to the present version. I am looking for comments and recommendations at this point.
The proposed text is available in my sandbox at https://en.wikipedia.org/User:David_Weyburne/sandbox
The proposed explanation is based on a graphical interpretation of the mathematical equations governing fluid flow. The key to the approach is the graphical plots of the velocity profiles and the pressure gradient profiles taken at a bunch of locations along the airfoil surface. This permits a one-to-one correspondence between the flow governing equations and the plotted profiles. By invoking the momentum conservation equation in this way, the explanation provides the connection between the velocity and pressure fields that is missing in the other simple explanations. David Weyburne (talk) 13:38, 17 September 2022 (UTC)
- Where a Misplaced Pages User develops a new explanation for something it is called Original Research. Such an explanation is not published in Misplaced Pages - see WP:NOR.
- Your explanation cannot be described as simplified. I find it mystifying. Some of your sentences are statements of the obvious and therefore unnecessary in your description; and others are either incorrect or misleading. If you wish to continue with your work on this subject in order to publish it in an appropriate place, it needs a lot of refinement.
- You are relying on four sources but three have been published by yourself. This is usually unwise and I have commented at User talk:David Weyburne/sandbox. Dolphin (t) 23:20, 17 September 2022 (UTC)
- Thanks for the feedback. As to original research comment: I do not think any of the explanations presented in the Simplified Explanations section would constitute original research that would be appropriate for a journal article. The explanation may be original but it is not something that can be tested and verified by other research groups. As to the rest of the comment: I am sorry you find it mystifying but I am hoping that is not the case for the majority of readers. You claim there are obvious statements that are unnecessary: I have tried to make the explanation readable for the non-expert and would hope that the expert reader would allow for that. You also claim there are misleading and incorrect statements: It is hard to comment on this claim since you did not bother to outline which statements are false or misleading. David Weyburne (talk) 12:54, 21 September 2022 (UTC)
- David Weyburne Thanks David. On 18 September I made some introductory comments about statements I regard as superfluous, and others I regard as misleading. Those comments are on one of your Talk pages - see User talk:David Weyburne/sandbox. Dolphin (t) 23:05, 21 September 2022 (UTC)
- Sorry, I initially missed your comments in my sandbox. I appreciate your detailed comments and I have replied to the comments in the Talk section. At this point I will leave the explanation as is and would add that a more detailed explanation is available in the supplied references. David Weyburne (talk) 12:40, 22 September 2022 (UTC)
- One further note as to the observation that three of the sources were published by myself and is therefore inappropriate. I would point out that one is a YouTube video, another is an Air Force Technical Report, and the third is an e-book collection of my Air Force Tech Reports. All of them lay out a more detailed version of the condensed simplified explanation provided in my Sandbox. The reason the references are all mine is that I believe that my simplified explanation is original. However, as I stated before, this type of simplified explanation is not something that would be appropriate to be published in a standard journal. It is appropriate for providing a simplified explanation in an encyclopedia-style format. David Weyburne (talk) 12:45, 23 September 2022 (UTC)
- As the author of the proposed cited articles you may be subject to Wikipeda's conflict of interest policy. I would suggest familiarizing yourself with that policy. I appreciate the fact that you have disclosed that you are the author of those articles, but that fact remains and is germane and therefore not inappropriate.
- That said, the fact that the proposed additional material uses your articles as their source doesn't mean that the material can't be added to the article, or that your articles can't be cited. We've encountered this issue before with a prominent author, who provided some very valuable insights into this topic and helped improve the article. But he made very few edits himself, instead working with the other editors to reach consensus about any proposed revision to the article. I think we are on solid grounds if we follow that model. Mr. Swordfish (talk) 19:38, 23 September 2022 (UTC)
- Sorry, been busy. I understand that referencing my own work is problematic. To explain the reason for doing this, I need to give a little background. My simplified explanation for aerodynamic lift is based on showing "graphically" how the conservation of mass, momentum, and energy occurs for a flow around an airfoil. To do this, I start using a simple word-based argument to say that mass diversion results in velocity changes while being diverted around an airfoil. These velocity changes result in a speed up for the flow on the airfoil. How do you graphically show this speed-up? It is possible to use streamline, contour, or vector plots of the velocity but because of the large spatial variations, this approach is not very effective. Hence, most simplified explanations for lift regress to simply stating that "the velocity speeds up". For my simplified explanation I switched to a series of "velocity profile plots" along the airfoil. The profiles show the velocity behavior from a point on the airfoil to a point deep in the free stream above the airfoil. What you see are velocity peaks near the airfoil surface that slowly return to the free stream over distances of ~two chords. These peaks are important in that it gives a visual confirmation of velocity changes and give a one-to-one comparison to the momentum equation du/dy term. The momentum equation says these velocity changes must be conserved which is done, in part, by pressure changes. I then can show a plot of the pressure gradient profiles above and below the wing at the same location as the velocity profiles. The difference in the pressure profile areas, the pressure difference, shows graphically how mass and momentum conservation results in lift.
- So what is the problem, why do I only reference my own work? The reason is there is no one doing anything similar using velocity profiles. This velocity profile "peaking" behavior is not discussed or plotted anywhere in the literature that I could find (other than the simple text saying "the velocity speeds up"). Many textbooks show schematics of boundary layer profiles but not ones that show the peaks, the velocity speedup behavior. I observe it my airfoil simulations and in raw mesh data provided by other researchers, but nowhere in the literature. If I had references showing that these velocity and pressure profile peaks exist, I would be less dependent on referencing my own work. For the record, I think for the non-expert, my 15 min. graphics-based YouTube video does a better job of explaining this aerodynamic lift argument than my e-book version.
- I would be willing to work with any editor to resolve this issue. David Weyburne (talk) 15:03, 23 March 2023 (UTC)
Recent changes to equal transit time section
The diff is here: https://en.wikipedia.org/search/?title=Lift_%28force%29&diff=1228641725&oldid=1227711027
I don't read the previous version as claiming that equal transit time never happens, only that it cannot be assumed. The "offending" passage is:
- This is because the assumption of equal transit time is wrong. There is no physical principle that requires equal transit time and experimental results show that this assumption is false.
By way of analogy, regarding flipping a coin we could write:
- This is because the assumption of it always landing heads-up is wrong. There is no physical principle that requires a coin to always land heads-up and experimental results show that this assumption is false.
I don't think that anyone would read that as claiming that coins never land heads-up, only that they don't always land heads-up. Likewise, ETT is not a general physical principle, but that doesn't imply that it never happens. I don't think we need this level of clarification and the recently added/changed language seems to me to make the section more difficult to read. Perhaps we could simply add a sentence to the effect of "ETT does occur in some situations, but when it does there is no lift." But I don't know that it's really necessary. I'll wait for other editors to weigh in before reverting the edit. Mr. Swordfish (talk) 14:24, 12 June 2024 (UTC)
- Prior to my recent edit, Misplaced Pages’s emphasis was that equal transit time (ETT) is wrong, false, incorrect, misleading etc. In fact, the opposite is true. ETT represents the flow past most solid bodies. Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT. It is only lifting flows that don’t exhibit ETT. Let’s say 99% of flows around solid objects can be described as exhibiting ETT; and only 1% of flows cannot be described in this way. Saying “the assumption of equal transit time is wrong” is a statement that can be soundly challenged unless it is clear that it is confined to lifting flows.
- ETT is a very simple 3-word expression. Doug McLean describes it as “an argument that is widespread in explanations aimed at the layman.” (See Understanding Aerodynamics, section 7.3.1.4) A more sophisticated way of saying ETT is “the circulation is equal to zero”. There are many reliable sources that talk about flows where circulation is equal to zero.
- Prior to my recent edit, Misplaced Pages said
there is no physical principle that requires equal transit time ...
This statement can be soundly challenged unless it is clear that it is confined to lifting flows. The Kutta–Joukowski theorem is a fundamental theorem in the field of aerodynamics and it clearly implies that a non-lifting flow around a body must have a circulation of zero! Similarly it implies that if the circulation is zero, the lift will also be zero. For circulation equal to zero, the layman may read ETT. - Misplaced Pages needs to say that ETT does not exist around a lifting body or around an airfoil experiencing lift but we need to be careful to avoid versions of this statement that are so universal in their applicability that they can be readily challenged. It can be challenged if Misplaced Pages implies that ETT is inherently false, or universally inapplicable. ETT is the usual state of affairs, and it is only in the very narrow field of lifting flows that it does not prevail and cannot be assumed. Dolphin (t) 06:15, 13 June 2024 (UTC)
- > Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT.
- Is this true? Usually power lines, wires in fences, and flagpoles sway and move in the wind. What force is causing that movement? Do raindrops always fall straight down, or is there sometimes asymmetrical airflow that causes a horizontal force?
- Flows with zero circulation are nice simple models so there are lots of textbook examples of that idealized condition. I'm highly skeptical that they occur in nature as the rule rather than the as a first order model in theory; for it to occur, I think you'd need to have the solid object be perfectly symmetrical, not rotating, and the airflow non-turbulent. Perhaps you can provide a reference for your 99% claim? Regardless, this tangent distracts from the main thrust of the section i.e. ETT is not a physical law like conservation of momentum, energy, or mass so it can't be assumed.
- The previous version states that "the assumption of ETT is wrong". That's correct. And "There is no physical principle that requires ETT" That is also correct. We should stick by that. Mr. Swordfish (talk) 12:56, 13 June 2024 (UTC)
- Interesting article that addresses the history of ETT. It's not peer reviewed so we can't cite it as a reliable source, but worth a read.
- https://arxiv.org/pdf/2110.00690
- On the Origins and Relevance of the Equal Transit Time Fallacy to Explain Lift
- Graham Wild
- School of Engineering and Information Technology, UNSW ADFA, Canberra, Australia
- G.Wild@ADFA.edu.au
- 1st of October 2021
- Preprint
- Not Peer Reviewed
- Abstract
- Recently, aerodynamics syllabi have changed in high schools, pilot ground training, and even
- undergraduate physics. In contrast, there has been no change in the basic theory taught to
- aeronautical or aerospace engineers. What has changed is technology, both experimentally and
- computationally. The internet and social media have also empowered citizen science such that
- the deficiencies in the legacy physics education around flight and lift are well known. The long-
- standing equal transit time (ETT) theory to explain lift has been proven false. If incorrect, why
- was it ever taught? Through a historical analysis of relevant fluid and aerodynamics literature,
- this study attempts to explain why ETT theory is part of our collectively lower-level cognitive
- understanding of lift and flight. It was found that in 1744 D’Alembert himself assumed this to
- be a feature of moving fluids, and while this initial intuition (ETT 1.0) was incorrect, the
- property of ETT (ETT 2.0) was derived in 1752 when applying Newton’s laws of motion to
- fluids. This incorrect result was independently confirmed in 1757 by Euler! The conclusion is
- that an over simplified treatment of fluids predicts ETT, along with no lift and drag. This then
- leads to the open question, can ETT be taught at an appropriately low level as an explanation
- for lift? Mr. Swordfish (talk) 12:51, 14 June 2024 (UTC)
- I don’t accept your arguments. I explained my arguments in significant detail but you haven’t engaged with that detail or responded to it adequately. For example, I have written about non-lifting flows and you have responded with a little original research suggesting that flows with zero circulation are non-existent or rare.
- If you wish, you could make a reasonable defence of the sentence I amended by arguing that the surrounding context makes it clear to all readers that the entire section, and the article, apply exclusively to lifting flows so if Misplaced Pages says
the assumption of ETT is wrong
it is not referring to non-lifting flows. I won’t automatically buy that argument but perhaps I will eventually if it is explained persuasively. It is an argument that has much greater potential than the arguments you put forward in your previous edit. - You have written “the assumption of ETT is wrong. That’s correct.” No, it’s not correct in the case of non-lifting flows. I have explained that in detail.
- You have written “There is no physical principle that requires ETT. That is also correct.” No, it isn’t correct. The Kutta–Joukowski theorem is a physical principle and it requires ETT in non-lifting flows. I have explained that in detail. Dolphin (t) 13:13, 14 June 2024 (UTC)
- I think we both agree that ETT is not a valid assumption for an airfoil with lift. I think we also both agree that there is a body of scholarship that does make the simplifying assumption of ETT in some specific examples. That doesn't imply to me that ETT is the usual state of affairs any more than the assumption of a spherical cow implies anything about the shape or real-world cows.
- You assert that "ETT represents the flow past most solid bodies". But you have not provided a citation for that. I'm highly skeptical that this is true since just about everything moves and flutters in the wind. As Norman Smith's paper states:
- ...the claim that the air must traverse the curved top surface in the same time as it does the flat bottom surface...is fictional. We can quote no physical law that tells us this.
- That is, in general there is no physical law that requires ETT. That's not to say it never happens, or that no physical models ever make that simplifying assumption (and when they do, the result is zero lift). Whether "most solid bodies" exhibit ETT is somewhat orthogonal to this section, so perhaps we don't need to settle that here. I do think that the recent additions and changes are a distraction and make the section less readable. I'll take a look at improving the readability while keeping your concerns about overstating the invalidity of ETT. Mr. Swordfish (talk) 16:04, 14 June 2024 (UTC)
- You and I both have a thorough understanding of the Kutta–Joukowski theorem. I believe the expression “equal transit time” may be a layman’s way of saying the circulation is equal to zero; I hope we agree on that.
- A small part of the problem is that ETT is not a well-defined or rigorously defined expression. To the best of my knowledge this expression is only used by authors who are repudiating this attempt at an explanation of aerodynamic lift. To the best of my knowledge none of the authors and institutions that resort to this naïve explanation of lift actually use the expression “equal transit time“; no-one actually asserts that “ETT” is true or correct. There are only people like us who assert that ETT is not correct (when applied to a body generating lift.)
- Your quote from Norman Smith describes a body with “the curved top surface” and “the flat bottom surface.” He is not referring to “most solid bodies” - he is describing an airfoil!
- I can supply a quotation from Anderson’s “Fundamentals of Aerodynamics” that will help on this topic. I expect to get access to my copy of Anderson within 7 days. Dolphin (t) 14:30, 15 June 2024 (UTC)
- Agree that ETT is not well defined, and that it doesn't appear to be used other than by those repudiating it. Searching for the phrase (or even the word "equal") on my user page collection of works presenting ETT as correct only finds that in the references, not the actual works themselves. Similarly, the obstruction explanation is sometimes derisively referred to as "hump theory" but it's proponents don't use that phrase.
- A typical turn of phrase is "The air moving on the top has to travel a greater distance in the same amount of time." or "Air flowing over the top has a greater distance to travel in the same time; that's why it flows faster."
- I don't know that the expression “equal transit time” is a layman’s way of saying the circulation is equal to zero, since I would surmize that those advancing the idea probably don't know what circulation is. That said, here's a source basically confirming that ETT and Γ=0 are the same idea.
- Regarding whether most flows around solid objects exhibit ETT, if that were true than vortex shedding and Vortex-induced vibration would not pose problems for engineers to overcome.
References
- Flight Physics: Essentials of Aeronautical Disciplines and Technology, with Historical Notes (1st ed.). Springer. 2009. p. 144. ISBN 1-4020-8663-6.
In conclusion, there is no possibility that the particles passing above and below the aerofoil would arrive simultaneously at the tail, except for the case that there is no circulation around the section – in this case, there is no lift on it.
Mr. Swordfish (talk) 16:20, 15 June 2024 (UTC)
- Edits finished. Hopefully that addresses the concerns above. Mr. Swordfish (talk) 16:36, 14 June 2024 (UTC)
- Your recent edit to the article is an acceptable alternative to my edits. Thank you for making those changes.
- The article now avoids giving readers the impression that ETT is inherently false. Hopefully readers can now see that the only falsehood is suggesting ETT exists in the flow around a lifting body. Dolphin (t) 14:46, 15 June 2024 (UTC)
- Edits finished. Hopefully that addresses the concerns above. Mr. Swordfish (talk) 16:36, 14 June 2024 (UTC)
- Thanks for the reference to “Flight Physics:Essentials ...” I was not aware of that publication. It looks like it might be essential!
- Vortex induced vibrations are an oscillatory phenomenon. They become a problem in structures that have inadequate stiffness or inadequate damping. In our article on lift we are talking about steady flows with zero viscous effects, or only minor viscous effects. We use a reference frame attached to the airfoil or solid body so the consequences of oscillations of a solid body are way beyond the level of analysis we are using in this article, and related articles.
- Could it be that after half a lifetime of believing that ETT is false, the work of the devil, it will take a major change of direction to accept that there is nothing false or distasteful about ETT? Could that be why you are finding reasons to deny the inevitability of flows in which circulation is zero, ETT prevails and lift is zero? Dolphin (t) 03:46, 16 June 2024 (UTC)
- It's not that I don't believe lift can be zero (and that implies ETT). I just don't think it occurs as often as you seem to think it does i.e. 99% of the time a solid body is immersed in a moving fluid. That's because almost all real world objects are not perfectly symmetrical and that implies an asymmetrical air flow hence non-zero circulation.
- Stated another way, ETT is not a valid assumption in general. If you assume ETT, you will get zero lift. I don't have a cite for this and I am willing to consider evidence to the contrary, but real-world airflows around solid objects with zero circulation are the exception rather than the rule. For instance, consider a symmetrical airfoil in a steady flow - it is well established that the lift varies by the angle of attack. For the special case of zero AOA, the lift is zero and ETT occurs (in this simple 2-d model). For all the other values there is lift, circulation is non-zero, and ETT is false. In mathematical terms, the set of values for which ETT holds has measure zero. That's about as rare as you can get without it being never.
- Perhaps there is some area of aerodynamic research that assumes ETT or decides that lift is small enough that lift is negligible - many treatments ignore viscosity, or compressibility for example - I'm not aware of any that assume zero lift, but maybe there are. Let me know if you know of any. Mr. Swordfish (talk) 13:00, 16 June 2024 (UTC)
- There are several elements of your edit on which I can comment but at present I only have time for one. I will comment on others later.
- You write about “real-world solid objects with zero circulation ...” Then you make a sneaky gear change and write about “a symmetrical airfoil ...” The two are very, very different in aerodynamics so your gear change doesn’t go unnoticed. Yes, a well-designed airfoil will produce lift (and lift coefficient and circulation) that varies approximately linearly with angle of attack. The feature of a well-designed airfoil that yields this desirable property is the sharp trailing edge. Clancy’s book Aerodynamics addresses the role of the sharp trailing edge and the way it causes vortex shedding to adjust the strength of the bound vortex to maintain the Kutta condition. I don’t have Clancy with me but I think it is Section 4.5 and/or 4.8 that contains good explanatory diagrams.
- In the absence of a sharp trailing edge, any change in orientation of a body is not accompanied by a change in lift (or lift coefficient or circulation.) For example, a cylinder with elliptical cross section, immersed in a flow produces little or no lift; altering the orientation of the cylinder doesn’t produce much change. What lift might be produced is due to asymmetric boundary layers and separated flow, rather than due to the primary flow predicted using an inviscid fluid. If a body doesn’t have a sharp trailing edge, and the orientation of that body is changed, the fluid flow adjusts itself so that circulation remains zero. Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge. Airfoils have sharp trailing edges, but real-world solid objects don’t. That is why the only circulation and lift that are observed on bodies without sharp trailing edges is the small amount caused by asymmetric boundary layers on the two sides of the body, separated flow and possibly other minor viscous effects.
- Scientists and engineers have to work hard to generate circulation and lift. Typically they use airfoils with thin, sharp trailing edges even though this feature is structurally weak and vulnerable. Flowing fluids are uncooperative - as they flow around bodies their natural state is doing so with zero circulation. Any change in orientation of a real-world solid body causes the fluid to change its flow pattern to avoid circulation developing. If it were not so, aircraft designers would use wings with thick, generously rounded trailing edges so they could get more fuel into the wings, use deeper and lighter spars, and have more room into which to retract the undercarriage. Dolphin (t) 16:18, 16 June 2024 (UTC)
- On the matter of the sharp trailing edge there is a very useful quotation by George Batchelor in the short article Trailing edge.
- There is also a useful quotation by Richard von Mises at Airfoil, reference number 4. Dolphin (t) 00:38, 17 June 2024 (UTC)
- The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation. Picture the wind blowing around such a body, and then the wind changes direction. Imagine that this change causes a circulation to begin in the flow. This circulation causes a lift force to act on the solid body. Newton’s 3rd law tells us that an identical lift force acts on the flowing air. When a fluid that is free to flow or change shape is subjected to a force or pressure it responds in whatever way will cause that force to diminish. Consequently the lift force on the air flowing around the solid body causes the streamlines, velocities and pressures to change to diminish the circulation that has just begun. This process can be expected to continue until all circulation has been eliminated. Only then has equilibrium been achieved within the flow pattern around the body.
- Any residual circulation and lift is not related to the primary flow as would exist in a geometrically similar situation but with an inviscid fluid. It is related to the secondary flow caused by viscous effects such as flow separation. Any residual lift is still accompanied by the original drag force. The lift to drag ratio is so small that this solid body doesn’t qualify as an airfoil. I believe this is an explanation for the operation of oddly shaped lifting bodies which glide without conventional wings. Dolphin (t) 05:22, 17 June 2024 (UTC)
- I'm continuing this discussion since I think I may learn something. I'm not trying to be "sneaky", just trying to understand what evidence there is that zero-circulation/zero-lift/ETT is the usual or normal state of affairs rather than a rare exception.
- >Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge.\
- Agree that Kutta condition requires a sharp trailing edge, because without one it's not obvious where the rear stagnation point occurs. And without that it's not clear how much circulation to apply to model the fluid re-joining at the rear stagnation point. But you don't need a sharp trailing edge to have an asymmetrical airflow with non-zero circulation, you just can't apply the Kutta contidion. As Gale Craig states, (paraphrasing) you don't need an airfoil shape to get lift, as anyone who has ever handled a sheet of plywood in the wind knows. Of course, if you want enough lift to fly a plane of propel a sailboat, you'll want something with more lift than a non-arifoil can provide. That doesn't mean only airfoils with sharp trailing edges can generate lift.
- I have sailed boats with rudders that have a rounded trailing edge. Performance is sub-optimal, but the rudder most definitely provides enough lift to steer the boat. When I look at leaves on trees or flags on a flagpole in the wind, they never settle down into an equilibrium of zero lift as you describe above. Spinning balls have lift, as any tennis player understands. Here in the US, there's a baseball pitch called the knuckleball where the ball is thrown with a little spin as possible, with the effect that it's impossible to predict which direction the lift will take the ball making it very hard to hit. So, my experience is quite at odds with your assertions.
- You say that "The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation." but don't provide anything to back that up. Along with your 99% figure, I would need some more to go on than your assertion.
- Agree that my examples above are anecdotal or original research. Here's an interesting treatment of bluff bodies which seems to be in conflict with your assertion that Circulation greater than zero requires the Kutta condition...
- For bluff bodies, the interest is usually in the drag on that body, mainly because experiments have found that drag is the dominant force. This observation, however, does not imply that bluff bodies cannot produce lift because many do. Nevertheless, examining just the drag characteristics of such bodies is convenient in the first instance. Furthermore, bluff bodies may also produce pitching moments, which sometimes need to be known for certain types of engineering work, e.g., to determine torsional loads.
- Mr. Swordfish (talk) 13:56, 17 June 2024 (UTC)
- Here's an excerpt from another paper BLUFF-BODY AERODYNAMICS
- Bluff bodies are obviously also subjected to forces in the across-wind direction and to
- moments around the various axes due to non-symmetries of the pressure distribution on their
- surface. Therefore, these loads depend fundamentally both of the body shape and on the
- orientation of the incoming freestream. Particularly in the two-dimensional case, the force
- component in the across-wind direction is often called lift force, in analogy to the
- corresponding force acting on an aeronautical wing section (airfoil).
- (elision of details about the starting vortex and consequential circulation around an arifoil)
- Coming back to bluff bodies, the above described mechanism does not apply in all its
- details, particularly because the boundary layer cannot remain attached to their surface even
- after the end of the initial transient. However, if the body is sufficiently elongated (like an
- ellipse), a starting vortex is shed anyway (even if not as strong as that of an airfoil), and the
- asymmetry of the final flow configuration for non-symmetrical wind orientations may be
- sufficient for producing significant lateral forces.
- Seems to me that if it were the case that almost all bluff bodies experience zero lift the paper would say that at some point. Mr. Swordfish (talk) 14:32, 17 June 2024 (UTC)
- One of the frustrating aspects of discussing this subject is the variation in meaning given to the word “airfoil”. On these Talk pages I see the word used with three different meanings:
- A two-dimensional shape that can be employed in three-dimensional bodies to generate lift. For example, the shape known as NACA 2412 is an airfoil section commonly used for the wings of low-speed aircraft.
- A three-dimensional body that generates at least a little lift. Some Users point to an irregular body or a sheet of plywood or a sycamore seed and, noting that it experiences a small lift force, say “see, it is an airfoil!”
- A three-dimensional body that, over a usable range of angle of attack, is capable of generating significantly more lift than drag. With this meaning, airfoils are manmade structures that have the generation of lift as their primary purpose. Airfoils are carefully designed and manufactured structures to ensure the lift-to-drag ratio is high enough to achieve its intended purpose.
- Misplaced Pages’s current definition of airfoil closely matches No 3 above. Airfoil says:
When the wind is obstructed by an object such as a flat plate, a building, or the deck of a bridge, the object will experience drag and also an aerodynamic force perpendicular to the wind. This does not mean the object qualifies as an airfoil. Airfoils are highly-efficient lifting shapes, able to generate more lift than similarly sized flat plates of the same area, and able to generate lift with significantly less drag. Airfoils are used in the design of aircraft, propellers, rotor blades, wind turbines and other applications of aeronautical engineering
- The layman imagines that the essential feature of an airfoil (meaning No 3) is its generously rounded leading edge, or its curved surface. In fact it is the trailing edge. That is partly the explanation of why a flat sheet of plywood will experience lift in a flow of air - it has a sharp trailing edge.
- Since the days of Joukowski and Kutta, mathematicians and physicists have been able to model the flow of an inviscid fluid around suitable geometric shapes. With a sharp trailing edge it is possible to determine the lift and pitching moment on the shapes. Tests on real models of wings in wind tunnels show there is close agreement between the math and the real world for these shapes with sharp trailing edges. For bodies without a sharp trailing edge, the math shows that an inviscid fluid imparts no lift or pitching moment to the body.
- Wind tunnel tests on bodies without sharp trailing edges, and anecdotal evidence, show that these bodies can experience a little lift. This does not mean they qualify as airfoils under meaning No 3 above. Engineering, and most science, have little interest in these bodies. What lift they develop is not due to airfoil action - exploiting the Kutta condition to generate lift. It is due solely to viscous effects such as flow separation. These bodies, at best, have a very low lift-to-drag ratio. Little is written about them in mainstream science or engineering publications. This type of lift has little or no engineering application.
- We know that eating a tablespoon of salt a day won’t cure cancer, but it is probably impossible to find a reliable published source that confirms eating a tablespoon of salt a day won’t cure cancer! Similarly it is probably impossible to find a reliable published source that confirms that no bluff body has ever been found that is capable of a high lift-to-drag ratio.
- We use the Kutta condition to determine, mathematically, the circulation around a 2-D shape with a sharp trailing edge edge. There is no similar model, theory or equation to determine circulation around a 2-D shape with no sharp trailing edge. I suspect that wind tunnel tests would not show a usable relationship because, being reliant entirely on viscous effects, the results would be strongly influenced by the surface conditions of each model being used - roughness, smoothness, manufacturing imperfections etc.
- When I say that bodies without sharp trailing edges do not generate circulation in fluid flows around them, I am speaking as an aerodynamicist applying the model of the inviscid fluid. There is no doubt that my statement is true for inviscid flows, which admittedly are fictitious, but this is usually a good, simple guide to the reality of high Reynolds number flows. When you say that all bodies in a fluid flow experience viscous forces and these forces will provide at least a very small amount of circulation that cannot be eliminated by the flow pattern adjusting itself you are possibly speaking as a scientist focussed on observing the complex realities of the real world. You aren’t able to determine how much circulation there will be, or say exactly how that circulation is sustained. What circulation exists is small and I say it is zero. You possibly describe the same situation by saying circulation is not zero. That might be as close to consensus as we can hope to reach. Dolphin (t) 15:39, 17 June 2024 (UTC)
- Agree that I am sometimes a bit loose with the terminology re: airfoil. One other possible avenue of miscommunication here is that when I see the word "lift" in this context I think of the definition used in the first sentence of the article:
- and as a mathematician rather than an aerodynamic engineer lift=0 means actually zero, as opposed to "too small to be useful or significant." One of the arts of engineering is to figure out what things can be ignored, and for most non-airfoil applications the fact that there is some component of the aerodynamic force perpendicular to the airflow is negligible. I'm sure that there are many situations where we would agree that whatever small amount of lift might be present, it's too small to matter so let's assume it is zero. This would imply ETT in that situation.
- Other situations I wouldn't agree that it's too small to matter, for instance, a leaf on a tree in a breeze - the leaf repeatedly flutters back and forth in a direction perpendicular to the airflow and this implies to me that there is some force making it move that way and the obvious one is that there is some non-zero component of force transverse to the airflow. I would call that "lift" according to the definition above. But since I doubt either of us will be hired as an engineer to design tree leaves any time soon we can leave it there. Mr. Swordfish (talk) 17:56, 17 June 2024 (UTC)
- Thanks. I agree with most, if not all, of what you have written. I now realise that the concepts of streamlines, time slices, circulation and ETT are all concepts that rely on steady flow. When we are talking about a turbulent wake, separated flow, oscillatory flow, the erratic dancing of the leaves and branches of a tree, we can’t claim the protection offered by retreating to steady flow. Debating about streamlines, time slices and ETT in a non-steady flow is deeply flawed.
- The dancing of leaves on a tree is definitely caused by the interaction of aerodynamic forces and elastic forces within the highly flexible structures of a tree. This kind of motion could be caused entirely by drag, so I’m not persuaded that the dancing motion of a leaf necessarily shows the presence of lift.
- The concepts of lift and drag rely on knowing the direction of the local velocity of the fluid. The air moving through the branches and leaves of a tree is highly disorganised and the velocity at each point is changing rapidly so it is probably true to say that while we can possibly identify aerodynamic forces acting on branches and leaves, the concepts of a drag component and a lift component are not applicable. The distinction between a lift component and a drag component seems to be reliant on steady flow, and flow in which the speed and direction at one point is almost identical to the speed and direction at all nearby points.
- The Kutta-Joukowski theorem is remarkably similar to Newton’s 1st and 2nd laws. Scientists and engineers say Newton’s laws are valid. Perhaps a mathematician and philosopher might say Newton’s 1st law is redundant because there is no such thing as a body whose acceleration is truly zero; and no such thing as a body experiencing a net force that is truly zero. Dolphin (t) 00:30, 18 June 2024 (UTC)
- In my edit dated 15 June 2024 (14:30) I wrote “I can supply a quotation from Anderson’s Fundamentals of Aerodynamics that will help on this topic.” See the diff. In section 3.16 Anderson writes about the Kutta-Joukowski theorem:
"Although the result given by the equation was derived for a circular cylinder, it applies in general to cylindrical bodies of arbitrary cross section."
- This confirms that the Kutta-Joukowski theorem is not confined to airfoils. It applies to all cylindrical bodies regardless of their cross sectional shape. If a cylinder of arbitrary cross section causes no circulation in the flow in which it is immersed the cylinder will experience no lift.
- It is not too great a leap to say that, just as airfoils are associated with the Kutta condition to explain when they will generate lift, and when they won’t, cylindrical bodies of arbitrary cross section also rely on a feature resembling a sharp edge to obtain a well-defined lift. If these bodies of arbitrary cross section experience lift in the absence of a sharp edge, it is due to viscous effects such as flow separation and asymmetric boundary layers, rather than due to airfoil action.
- My mention of a well-defined lift is from "sharp trailing edge to obtain a well-defined lift" as written by Richard von Mises. See citation No. 4 in Airfoil. Dolphin (t) 12:44, 30 June 2024 (UTC)
- In my edit dated 15 June 2024 (14:30) I wrote “I can supply a quotation from Anderson’s Fundamentals of Aerodynamics that will help on this topic.” See the diff. In section 3.16 Anderson writes about the Kutta-Joukowski theorem:
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