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== direction of centrifugal force == | |||
== Subject matter discussion == | |||
Okay. So we're discussion a subject matter. And somebody says it doesn't exist. And then I say it does exist, and then you throw me out based on a requirement related to the composition of the article about the subject matter. Does that make sense? I'm not in the article trying to change it. I merely provided a rational method of refuting the statement in the article that centrifugal force doesn't doesn't exist. And I don't know what you're trying to do. So please tell me how else I would be able to provide that information if I got some from your proposed source. And I really don't care about the composition of the article, because I read it to get correct information about the subject matter.] (]) 14:52, 10 May 2010 (UTC) | |||
:I really can't make any sense of what you are trying to say. Anyway, this is not the place to discuss the subject matter. Please read the first sentence of the ], then read the guidelines and policies at ] and ]. Thanks. ] (]) 15:22, 10 May 2010 (UTC) | |||
Okay. Have it your way. And I can see now why it is so hard to get articles corrected.] (]) 16:45, 10 May 2010 (UTC) If I referred You to Clerk Maxwell's discussion of force vectors in the "Atom" section of the 9th edition of the EB,would that solve your ] requirement?] (]) 16:58, 10 May 2010 (UTC) | |||
:I don't find anything related to the ''subject of this article''. The word force appears 27 times in the context of electromagnetic attraction and repulsion between atoms. If you intend to draw conclusions from anything in there about the subject of ''this'' article, then that is ] - see the section ]. What we need is a reliable source saying what you want to say. So, no, I don't think that "Atom" solves the ] requirement. ] (]) 17:31, 10 May 2010 (UTC) | |||
Well, how about the references in the article, like about "Newton's Bucket" etc. Do the writers of the article read those references? And I particularly like the one about ], where people in a rotating space station are able to stand up and walk on tha outside wall of the station due to the action of the "nonexistent?" centrifugal force exerted on their bodies towards the wall of the station.] (]) 19:16, 10 May 2010 (UTC) And I don't think you read about Boscovitch's argument that the motions of the atoms are controlled bu the force vectors and not by any physical contact. But thanks for the computer link to the article and I didn't know you could do that. And I am very impressed by the power of the computer to organize and present data. But if you're just worried about the composition of the article, and not about it's subject matter rationale, I don't think you're going to wind up with a good and informative article.] (]) 19:43, 10 May 2010 (UTC) | |||
:I don't understand what you mean with this question: "''Well, how about the references in the article, like about "Newton's Bucket" etc''". What do you mean with "''How about...''"? ] (]) 19:51, 10 May 2010 (UTC) | |||
The question has always been as to whether there is or is not a real centrifugal force. And Newton used the whirling bucket phenomenon to argue that there had to be a force that moved the water away from the center of rotation until it ran into a force that constrained it. But there wasn't any explainable force within the attention sphere of the bucket, so they got into an argument about relative motion activities, and lost sight of the local problem, which is still as to why the water piles up in the direction away from the center of rotation. | |||
And I don't see the reason for the complications. If something accelerates in some direction, it's because something is pushing (applying a force) in that direction. That's part of Newton's laws of motion. But you can keep it complex if you want, by either disregarding the space and motion relationship of the components of the subject matter, or by developing some mathematical formula that leaves out some relationship factor that leaves out something related to the process of the event.] (]) 20:28, 10 May 2010 (UTC) | |||
:I'm not asking for your opinions about and reflections upon something that is written, or not written, in the article. As you ''really'' should know by now (see ]), this is ''not the place to discuss such things''. I asked what you meant with the question: "''Well, how about the references in the article, like about "Newton's Bucket" etc''". I assume that this was a question about a reference in the article, so we can discuss that. But I did't understand the question, so I asked what you meant with "''What about...''"? ] (]) 20:41, 10 May 2010 (UTC) | |||
Well I assume that the information contained in the article includes the information contained in the references and that it should be compatible with the references as to concept and rationale. But maybe not. So it's not about my information and references versus your information and references, but rather the subjective opinion of the editor about the relative importance of a given subject matter with relation to his point of view. And I thought that the editor's POV was supposed to be neutral about subject matters.] (]) | |||
And what do you think about the information in the Acceleration and force in circular motion article? does it imply the existence of a real centrifugal force or not?[[User:WFPM|WFPM | |||
I'm afraid I don't understand your intent as to the proper controlling of the message of an article. Are you interested in the correctness of the grammar? Or of the agreed definition of word meanings, (which is important) or the Syntax of the discussion, or of the punctuation, or what else? How about the ability of the article to meet the requirement of Newton's first rule of Philosophy? Which requires the simplest correct and adequate explanation of the phenomenon and nothing more. And since there are many things in the hierarchy of the entities of physical entities and events that need to be explained and understood, that sounds like a good idea to me.] | |||
:You say that you "''assume that the information contained in the article includes the information contained in the references''". Ok, so there is no problem with the references then.<p>What I "''think about the information in the Acceleration and force in circular motion article''" is of no importance.<p>If you have some text to add to the article, then it must be ], it cannot be ], it needs a non-] ], and it should not put ] on the article. Otherwise, please stop discussing the subject matter on this talk page. ] (]) 07:43, 11 May 2010 (UTC) | |||
Well could I put some text into the article asking about the forces involved in those whirling swing devices that they have at the fairs, where they swing out over the audience, and which is obviously an unstable balance between the gravitational force and some force that's pushing the swing out over the audience, and that you say is a fictitious force?] (]) 14:46, 11 May 2010 (UTC) And after all, the primary purpose of this contraption is to create and demonstrate this so called centrifugal force. And I think that it would be in order for the article to explain it in an understandable manner.] (]) 15:21, 11 May 2010 (UTC) | |||
:No, you cannot put some text into the article asking about anything. ] (]) 15:25, 11 May 2010 (UTC) | |||
::WFPM: To me it seems you wish to argue that centrifugal force is "real", and don't think that the article does that. If we use "real" in the everyday sense, the article does agree that centrifugal force is real. On the ride at the fair, you do feel a real centrifugal force. Of course, as the person swinging on the ride, you are a ''rotating'' observer, not a stationary observer. | |||
::The only way the centrifugal force is not "real" is in a very technical sense, that is, in the sense that stationary observers don't use the concept of centrifugal force in their description of events. The article tries to explain that too. | |||
::So, there are at least three issues here. First, do you agree with the orthodox interpretation of the article in terms of stationary and rotating observers? Second, do you believe the article to misrepresent the orthodox view? Third, assuming you agree with the objectives of the article, what portions are unclear or misleading? | |||
::I have a hunch that you do not accept the orthodox view that the stationary observer (the one on the ground) can explain everything they see without using the centrifugal force. As that view is not correct, the article may need to be reworded to make even more clear that position is false. ] (]) 16:49, 19 August 2010 (UTC) | |||
I try to tie my concepts to a memorable physical event; so I can keep thinking about it when I have the time and inclination. And the memorable Centrifugal force event that I remember is seeing the people at the fairs sitting in the chairs which were whirling around over my head, and which were restrained by some taut chain tethers. And I know that I could measure the centripetal tensile force existing in the tethers. And if I had to make a sketch of the balance of forces explaining the tension in the tethers, I'd have have to show an inward centripetal force which is counteracting an outward "centrifugal" force. Now if I neglect the mass of the tether apparatus, and just concentrate on the mass of the (constant speed) traveling passenger, I can see that the tether is applying a restraining force to him which is perpendicular to his path of travel, and just capable of diverting his inertia driven straight line travel tendency into a circular path with a retained amount of angular momentum. And after he attains this state of constant velocity circular motion, I note that the affected mass of his body becomes static with respect to its motion related to the centrifugal and centripetal force vectors and that consequently no energy is being supplied to or taken from the system. And at that point, as far as I can see, the existence of both the centrifugal force and restraining centripetal force are real. But if it doesn't foul up the physical calculations, I wouldn't belabour the point.] (]) 06:05, 20 August 2010 (UTC) | |||
== Constitutive law of inertia == | |||
This material is not appropriate for the introduction, which is a qualitative section. Also, the term "constitutive law of inertia" and a good deal of the math here appears to me to be unsourced and a bit out of the main stream. To be included, it must be properly introduced and sourced, and a basis laid for a new section on this topic. ] (]) 15:06, 18 August 2010 (UTC) | |||
: I had added it there for the benefit of people like me who find it difficult to process large chunks of text and just need to refresh their memory of what a centrifugal force is. In my opinion, Noll's skew tensor notation is much clearer than the standard multiple curl of vector notation for the same formula. However, that formula does not appear in any discussion of centrifugal forces within Misplaced Pages. ] (]) 22:33, 22 August 2010 (UTC) | |||
== Bloat == | |||
This article was intended to be summary style, but it keeps accumulating bloat. Brews ohare reverted my latest attempt to remove unnecessary junk that was recently added to a section (I was responding to someone's suggestion that a cleanup was needed). Can anyone comment on whether it's helpful to have that level of detail in a summary of another article? ] (]) 02:49, 19 August 2010 (UTC) | |||
:I removed the detailed material that you removed, but with an explanation (immediately above). I left the "Common experiences" portion, which seems to me appropriate for such a preliminary article. ] (]) 05:41, 19 August 2010 (UTC) | |||
::And now you've got that as part of "Context and Usages", which says its main article is "Centrifugal force (rotating reference frame)". Can you repair that at least? ] (]) 05:59, 19 August 2010 (UTC) | |||
:Now that the latest ado has reached some kind of definitive consequences, I'm in agreement with you, Dicklyon. I think your removal of bloat was warranted and an improvement, and I'd support redoing it (in fact I think I'll go do that right now). There might have been a few references for the Lagrangian formulation that brews added in that it might be worth salvaging, but overemphasis on the lagrangian usage by be a bit undue weight. | |||
:In line with this, I think there are a few other concerns that I have. | |||
:*The "See also" section needs trimming so it matches the ]. | |||
:*The section headings could use tweaking - mainly I'm looking at the 4th item in ] and some of the guidelines on article titles. | |||
:*Finally, I still don't understand why we have both this article and ]. It seems like both pages are trying to do the same thing. Perhaps I'll make a subsection just for this item since I could see discussion on this getting pretty lengthy. | |||
:--] (]) 21:09, 22 August 2010 (UTC) | |||
== Re-merging == | |||
Right now we have at least three separate pages (this page, a disambiguation page, and one specific to rotating reference frames) and a lot of overlap in material and in function. For example, this page and ] are performing nearly the same function. Perhaps someone knows the rational for why we have both of them? I'm wondering if we can't re-merge this page and ], since a good argument could be made (imo) that the rotating reference topic is the ]. That way the disambiguation page can still exist (to help distinguish between this and the ]). The only aspect that might not nicely fit is the ] but which is (afaik) a very limited and slightly esoteric usage. I could very easily see that as a subsection. I could be wrong on this point, in which case it could be spun off into a separate article ('''Centrifugal force (Lagrangian mechanics)''' perhaps), but I still think the rotating reference frame should be the primary topic rather than the expanded faux disambiguation page we have now. Thoughts? --] (]) 19:53, 13 September 2010 (UTC) | |||
: I would agree with a three way merge, between ], ] and ]. The latter two seem far less encyclopaedic than they should be, with a surplus of examples and large, confusing diagrams needing overlong captions to explain them (and even then they are unclear). If the unencyclopaedic content were pared back it could be merged into the sections in ] and I don't think the resulting article would be too large. | |||
: The DAB page I think should stay for now, though once the articles are merged this could be reassessed, as what would be left might be too trivial - there would only be one page on centrifugal force. But the page at ] has no content and would not get in the way of the merge, so need not be considered.--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 20:23, 13 September 2010 (UTC) | |||
::For the most part I agree with you John, especially on the paring of surplus (imo, textbook-y) examples. The only difference in opinion I have is I would not advocate merging Reactive centrifugal force back in. The two are sufficiently distinct physical concepts (one's a fictitious force and frame dependent, the other a very real force that exists independent of frame; they will only equal in magnitude in a co-rotating frame) that I think separate articles are warranted. The concept of reactive centrifugal force is also a very common in engineering and one doesn't have to go searching for esoteric sources to find some that clearly make the distinction between the two. IIRC, one of the reasons for spinning it off was that one or two editors were constantly confusing the two and making the claim that they were the same thing. That isn't to say that ] couldn't use some paring and de-bloating, but I believe that there could still be enough information there to warrant its own article. | |||
::I should probably add some merger tags as a courtesy and to encourage others to chime in. --] (]) 16:30, 14 September 2010 (UTC) | |||
I think you should do away with the disambiguation page, since I can't see what it's for, but leave the summary-style ] article, and keep the other bloated articles separate (and separately work on de-bloating them). ] (]) 04:18, 15 September 2010 (UTC) | |||
::I would support this merger idea. One single article is all that is required for the topic 'centrifugal force'. ] (]) 11:42, 21 October 2010 (UTC) | |||
:::It wasn't a merger idea, so it's not clear what you're supporting. ] (]) 20:51, 21 October 2010 (UTC) | |||
Dick, the title of this section says re-merging, and from reading the lead that is what the author seems to be advocating, and I am supporting the re-merger. We only need one 'centrifugal force' article. The Germans don't have a multitude of articles on 'centrifugal force'. ] (]) 00:17, 22 October 2010 (UTC) | |||
::::But your reply to me above seemed to say you were supporting me; sorry I misunderstood. ] (]) 05:42, 22 December 2010 (UTC) | |||
So everybody involved in this discussion supports the re-merge, but two months later it hasn't happened yet. Why not? (I support it too FWIW.) ] (]) 20:48, 21 December 2010 (UTC) | |||
:Well, not quite. I agreed with getting rid of the new disambiguation article, but keeping the summary-style article (this one) and keeping the bigger and more specific articles (the ones I called "bloated") separate. I went ahead and merged the disambig (by redirecting it here, since there was nothing else to do). ] (]) 05:40, 22 December 2010 (UTC) | |||
:JohnBlackburne and FyzixFighter, do you have a merge plan that would get rid of some of the 48 KB of Brews ohare's bloat from ] as you merge? I might consider agreeing to a merge if I didn't think it would just add a lot of junk to what's currently not such a bad article. ] (]) 05:46, 22 December 2010 (UTC) | |||
::My suggestion would be to merge only the first three sections of ] and drop the rest entirely, but I'd guess that others would probably disagree. ] (]) 18:26, 22 December 2010 (UTC) | |||
::I would just trim the article as it is now: it's something that I've thought of before but never got around too, but even as a standalone article there's too much bloat from ] onwards, and too many references for them to be useful. It should be easy to do now without Brews's disruptive objections.--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 19:12, 22 December 2010 (UTC) | |||
:The Lagrangian section could do with considerable trimming also. I think this is a specialist and somewhat informal use of the term. ] (]) 18:14, 22 December | |||
:I'm opposed to the merge. This article is the sister article of ] and shouldn't be merged with others. It's a completely different topic; the maths is different, and the equation that it comes out of is different one.] (]) 17:00, 13 January 2011 (UTC) | |||
:: I get the feeling that you have confused the merge here. The proposal entails a merge of ] into ]. How are those a completely different topic? '''Yoenit''' (]) 17:39, 13 January 2011 (UTC) | |||
:I'm opposed, too. I think this is a stale proposal, that we partially fulfilled by phasing out the disambig page. If someone still thinks that it's important to do more merging, they should speak up right away, or start a new proposal explaining why. ] (]) 19:18, 13 January 2011 (UTC) | |||
Dick, are you against merging ] into ]? It seems like a good idea to me. ~~ | |||
:Yes, I '''Oppose''' the merge, because, as I've explained before, ] is a summary-style article that introduces the deeper treatments in ], ], ], ], and other articles. This seems like exactly the right place to have a summary-style article. ] (]) 23:07, 13 January 2011 (UTC) | |||
::I do not believe that a disambiguation page is desirable. There is only one definition of centrifugal force in widespread modern use and that is ]. A disambiguation page is in my opinion confusing to the general reader and gives undue weight to specialist, historical, or fringe meanings of the term. ] (]) 12:45, 14 January 2011 (UTC) | |||
:::I agree with you that a disambiguation page is not desirable here; that's why I eliminated it. I'm not sure why Wolfkeeper created it in the first place, or why Brews felt a need to bloat it to over 1600 bytes, but now it's gone. As for your assertion that "There is only one definition of centrifugal force in widespread modern use," that's sort of true, but a lot of disclaimers. Some dispatch to the other less modern, less widespread, and related points of view is still important, I think. A summary article is a good way to let the reader know what the different aspects are; for most, it's all they'll need. Or are you saying that some of the other articles are just junk that should be eliminated? ] (]) 16:17, 14 January 2011 (UTC) | |||
::::I am thinking of how this looks to an average reader who wants to know what centrifugal force is, or maybe a student needing some help on the subject. At the moment they see two articles, suggesting that the term has two, or more meanings. Personally, I would like to see one article on the standard modern meaning of the with short sections on historical or other meanings. ] (]) 22:43, 14 January 2011 (UTC) | |||
Dicklyon, anybody with a reasonable comprehension of the subject would know that there is only one 'centrifugal force', and that a single article could very easily accomodate all of the various perspectives on the matter. What you seem to have failed to grasp is that there is a big difference between, | |||
(1) considering centrifugal force to be a fictitious force as viewed from a rotating frame of reference, and | |||
(2) considering centrifugal force to be a radially outward inertial force that arises in conjunction with ], and which is revealed when Newton's laws are expressed in a rotating coordinate system such as polar coordinates. | |||
Regarding , asserting that: | |||
The former involves the idea that centrifugal force even exists when an object is not co-rotating with the rotating frame, while the latter attributes centrifugal force specifically to absolute angular momentum. The two perspectives overlap in the co-rotating scenario, but it is unnecessary to involve a rotating frame of reference when doing planetary orbital analyis. ] (]) 11:44, 14 January 2011 (UTC) | |||
''ω x (ω x r) is always perpendicular to ω'' | |||
:David, a rotating coordinate system is the same as a rotating frame of reference. Fictitious forces and inertial forces are two terms for the same thing. In the context of a rotating frame of reference (or coordinate system) rotating refers to absolute rotation. The distinction you make simply does not exist. ] (]) 22:43, 14 January 2011 (UTC) | |||
I don't think this is true. | |||
Martin, Part of what you are saying is right. I agree with you that centrifugal force is a single topic. I also agree that most modern textbooks introduce it as a fictitious force that is observed in a rotating frame of reference. I also agree with you that that the words 'fictitious' and 'inertial' are used inter-changeably in the modern literature. But you are also overlooking some important factors. When an object is co-rotating with a rotating frame of reference, the centrifugal force will be an inertial effect which can actually be felt pushing outwards. However, within the context of the 'rotating frame of reference' perspective, if an object is stationary and not co-rotating with the rotating frame of reference, it is still deemed to be subjected to a centrifugal force based on the angular speed of the frame of reference. That is where this approach differs from the polar coordinates approach. | |||
If F_centrifugal = mω x (ω x r) | |||
When we deal in polar coordinates, we are only concerned with the centrifugal force that arises in connection with absolute rotation, and which can be felt physically pushing outwards. And it is this perspective which is used in planetary orbital analysis where the rotation doesn't in general have a uniform angular speed. In other words, there is a branch of physics in which we consider centrifugal force as an outward radial force, and in which we don't normally invoke the concept of a rotating frame of reference, and in which the centrifugal force is induced by absolute rotation. This perspective needs to have a section of its own in the article. | |||
then by the rules of the ]: | |||
What I would like to ask you is 'what category do you place this latter perspective in? Is it specialist? Or is it fringe? Or is it historical?' I would say that it is general and historical. It was originally devised by Leibniz, and it is used today in planetary orbital analysis. At any rate, we have identified two different perspectives on centrifugal force. We have one in which it is a fictitious force which is a function of the rotating frame of reference, whether the object is co-rotating or not. And we have another in which the centrifugal force is an inertial force which can be physically felt and which is a product of absolute rotation, and which doesn't require the concept of a rotating frame of reference. Both of these perspectives are sourced, although I admit that the former is currently much more widely sourced. ] (]) 23:17, 14 January 2011 (UTC) | |||
=F_centrifugal=m(<math> \mathbf{\omega}(\mathbf{\omega}\cdot\mathbf{r}) - \mathbf{r}(\mathbf{\omega}\cdot\mathbf{\omega})</math> | |||
:It's essentially unsourced, idiosyncratic, and fringe. Goldstein made it clear enough that radial distance is a coordinate in a rotating coordinate system, not a concept different from the usual. ] (]) 00:06, 15 January 2011 (UTC) | |||
=m(<math> \mathbf{\omega}(\mathbf{\omega}\cdot\mathbf{r}) - \mathbf{r}\omega^2</math>). | |||
Yes, the second term is always radially outward, since it has magnitude <math>m*\omega^2</math> in the r direction, but the first time doesn't have to be 0 so long as <math>\omega</math> and r are not perpendicular. | |||
David, you seem completely confused, I suggest that we continue this discussion on your talk page. ] (]) 02:19, 15 January 2011 (UTC) | |||
For example, consider an objective in helical motion such that it is completing counterclockwise circles in xy plane as viewed from +z direction so that its r has a component n the z direction so that <math>\omega</math> has a component in the xy plane. That would make <math>\omega\cdot\mathbf{r} \ne 0</math> and thus ω x (ω x r) has a component in the <math>\mathbf{\omega}</math> direction and is not only radially outward.--] (]) 11:43, 5 June 2017 (UTC) | |||
::OK. We'll go there. But based on what you have written above, I am guessing that you have done one of those university courses in applied maths entitled 'rotating frames of reference' in which the coordinate transformations are done, and where centrifugal force and Coriolis force emerge and are introduced as fictitious effects which are a product of observation from the rotating frame. That of course, despite being prolific in modern textbooks, is a specialist approach for advanced mathematicians and it is not the common understanding of centrifugal force amongst the public at large. The public at large think of centrifugal force as being the outward radial pressure which arises when something is spun. And the common understanding is the one that is used in planetary orbital analysis. Anyway, by all means carry on on my talk page. ] (]) 11:44, 15 January 2011 (UTC) | |||
:I have just realised that the formula for centrifugal force you quote from the article was missing a minus sign. But with that correction, yes indeed, {{math|'''''F'''''<sub>centrifugal</sub> {{=}} – ''m'' {('''''ω · r''''') '''''ω''''' – ('''''ω · ω''''') '''''r'''''} }}, and therefore | |||
== The James Bond Cartoon == | |||
:::::{{math|'''''ω · F'''''<sub>centrifugal</sub> {{=}} – ''m'' {('''''ω · r''''') ('''''ω · ω''''') – ('''''ω · ω''''') ('''''ω · r''''')} {{=}} 0 }}. | |||
:That is, {{math| '''''F'''''<sub>centrifugal</sub>}} is perpendicular to {{math|'''''ω'''''}}. It is, in fact, a well-known property of the vector ], {{math|'''''a × b'''''}}, that it is ''always'' perpendicular to both of its multiplicands, {{math|'''''a'''''}} and {{math|'''''b'''''}}, and, in particular, –{{math|'''''ω ×''''' ('''''ω × r''''')}} is always perpendicular to {{math|'''''ω'''''}}. It is, in fact, just {{math|''ω''<sup>2</sup>}} times the projection of the vector {{math|'''''r'''''}} onto the plane perpendicular to {{math|'''''ω'''''}}. | |||
:Note also that the centrifugal force is an artefact of the motion of the ''coordinate system'' in which the motion of objects is being described, and this does not necessarily bear any relation whatsoever to the motion of any of those objects themselves. I presume the helical motion you have in mind is one in which the body's position {{math|'''''r'''''(''t'')}} at time {{math|''t''}} is given by something like {{math|'''''r'''''(''t'') {{=}} ''ρ'' cos(''ω t'') '''i''' + ''ρ'' sin(''ω t'') '''j''' + ''v<sub>z</sub> t'' '''k'''}}. But the {{math|''ω''}} in this expression is the angular velocity of ''the body in question'' about the {{math|''z''}} axis, and ''not'' (necessarily) that of the coordinate system in which the motion of the body is being described. If the coordinate system determined by the three unit vectors {{math|'''i'''}}, {{math|'''j'''}} and {{math|'''k'''}} is inertial, for instance, then the angular velocity of that coordinate sytem is zero, and there will be ''no'' centrifugal force on the body in ''that'' coordinate system. For the body to be following such a helical path, there must, of course, be a ''proper'' force, | |||
:::::::: {{math| ''m'' {{overset|'''..'''|'''''r'''''}}(''t'') {{=}} − ''m ω''<sup>2</sup> ( ''ρ'' cos(''ω t'') '''i''' + ''ρ'' sin(''ω t'') '''j''' )}} , | |||
:acting on it. This force is directed towards, and perpendicular to, the {{math|''z''}} axis of the inertial coordinate system. In a coordinate system whose origin and {{math|''z''}} axis coincide with those of the inertial system, but is rotating with angular velocity {{math|'''''ω''''' {{=}} ''ω'' '''k'''}}, the {{math|''x''}} and {{math|''y''}} coordinates of the body will be constant, and it will be moving with uniform velocity parallel to the {{math|''z''}} axis. In ''this'' coordinate system there will be a centrifugal force {{math| ''m ω''<sup>2</sup> ( ''ρ'' cos(''ω t'') '''i''' + ''ρ'' sin(''ω t'') '''j''' )}} acting on the body which exactly balances the proper force. This centrifugal force is clearly, as it must always be, perpendicular to {{math|'''''ω'''''}}.<br> | |||
:] <small>(] · ])</small> 14:21, 5 June 2017 (UTC) | |||
== A Commons file used on this page or its Wikidata item has been nominated for speedy deletion == | |||
There was alot of fuss about a James Bond cartoon while I was away and I didn't get the chance to state my 2 cents. The cartoon should not be in the main article, but it makes an excellent basis for a talk page discussion for the purpose of improving the article. The cartoon highlights the controversy very clearly. And here is an even better cartoon. Check out card number 12 at this weblink . ] (]) 19:49, 21 October 2010 (UTC) | |||
The following Wikimedia Commons file used on this page or its Wikidata item has been nominated for speedy deletion: | |||
* ]<!-- COMMONSBOT: speedy | 2022-12-09T15:53:00.202461 | Centrifugal force xkcd.png --> | |||
You can see the reason for deletion at the file description page linked above. —] (]) 15:53, 9 December 2022 (UTC) | |||
== |
== Inertial Motion == | ||
I changed the lead sentence because it's inertial motion and not observation that gives rise to centrifugal force. If an object is drawn to the edge of a rotating system by centrifugal force, this can be observed from any vantage point. Newton's rotating bucket is a prime example. You don't have to be rotating inside the bucket in order to observe the water being pushed against the bucket's walls. ] (]) 21:45, 14 December 2023 (UTC) | |||
On another point, the last sentence in the top paragraph talks about something called reactive centrifugal force, as though it's something different. It's just the same centrifugal force pushing or pulling against a centripetal force. It would be there anyway, even if the centripetal force wasn't there, and so it's not a reaction. The centripetal force curves the path of the object and it doesn't even have to be equal in magnitude to the centrifugal force unless it is causing circular motion.] (]) 21:52, 14 December 2023 (UTC) | |||
:I'm in favor of simplifying, but that oversimplification crosses into being incorrect. It's not observation that gives rise to centrifugal force, but describing the motion using a rotating/non-inertial coordinate system. From an inertial coordinate system, there is never a reason to invoke this centrifugal force to explain the motion - Newton's second law and a centripetal force are sufficient to explain the Newton's rotating bucket thought experiment. In Newton's thought experiment, it is actually the need to invoke an ad hoc centrifugal force that tells you the coordinate system is rotating. The text follows what is found in reliable sources such as journal articles and university textbooks. If you can indicate where the text does not appear to follow reliable sources, that would be helpful in refining the article. --] (]) 23:35, 14 December 2023 (UTC) | |||
I just reverted edit which changed the description of the two types of centrifugal force, fictitious and reactive, into I'm not sure what. I had a look at the source for the 'five different contexts' but could not find it, and frankly the source is very poor one, a long and poorly written essay which is no substitute for the reliable academic sources already in the article. More generally if there is some source which introduces new material it should be worked into the article alongside existing material, not added to the lede in a way which disagrees with the rest of the article.--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 17:31, 6 November 2010 (UTC) | |||
Well I'm afraid I'll have to disagree with you. The first paragraph mentions mechanical devices that operate on the basis of centrifugal force. How would these work if centrifugal force is only something that depends on the choice of coordinate frame? Surely centrifugal force has to be caused by inertial motion and not by choice of coordinate frame. ] (]) 10:36, 15 December 2023 (UTC) | |||
::John, it was in the paragraph third from the bottom. It read, | |||
:I agree with FyzixFighter. I have amended the lead to remove the suggestion that there are mechanical devices that operate on the basis of centrifugal force. Centrifugal force is a fictitious force, and it is lacking in rigour to use this force to attempt to explain the operation of certain rotating machines. Nevertheless there are people who incorporate the words “centrifugal force” into their explanation of operation of these machines. | |||
::''Thus Newton uses the term “centrifugal force” in the Principia to describe three very distinct concepts. First, he uses it to refer to a hypothetical repulsive force (such as the force between two electrons), which would result in a hyperbolic path, accelerating away from the source of the “central” repulsive force. Second, he uses the term to refer to the outward force exerted by a revolving object on some framework (such as the force exerted by a roulette marble on the housing). Third, he uses the term to refer to the “fictitious” outward force on a revolving object when viewed from a revolving frame of reference. A fourth context in which the concept of “centrifugal force” may arise is when phenomena are described in terms of curved coordinate systems, such as polar coordinates. Such non-linear coordinate systems are not inertial in the spatial sense, even though they may be static (i.e., not accelerating), as discussed in the note on Curved Coordinate Systems and Fictitious Forces. A fifth usage of the term “centrifugal force” occurs when the inertial forces on an object, relative to a momentarily co-moving inertial frame, are de-composed into tangent and normal components (in the osculating plane). The normal component is called centrifugal force. There is no Coriolis force with this convention, because the particle is always at rest with respect to the co-moving inertial coordinates. Needless to say, all these usages are very closely related, and differ only by context and convention.'' | |||
:Centrifugal force is like the ] and ] - scientists now know they don’t exist even though in by-gone days everyone thought they did. ] ''(])'' 12:32, 15 December 2023 (UTC) | |||
In a centrifuge, the material that is rotating with the machine, flies out to the edge because of its tendency to continue in its straight line inertial path. It pushes against the edge of the machine and Archimedes' principle is invoked, segregating the heavier particles from the lighter particles. That's an example of centrifugal force. I don't see this as being an effect that depends on the choice of coordinate frame for analysis. Same principle with a centrifugal clutch or a centrifugal governor. However you might analyse these, there is a force pressing outwards that has a mechanical effect. | |||
::You cannot leave the article lead stating that there are only two concepts of centrifugal force when there are clearly more. Polar coordinates is one such context. That is the context which is used in planetary orbital analysis. It is not something which is in any doubt. ] (]) 17:44, 6 November 2010 (UTC) | |||
Are you one hundred percent sure about what you have said above? Think about it. I simply can't agree with you. ] (]) 13:01, 15 December 2023 (UTC) | |||
:Thanks for your prompt reply. If you spend some time carefully reading a physics textbook that covers introductory mechanics, and you focus on displacement, velocity and acceleration; and Newton’s laws of motion, we will end up agreeing with each other. When we try to explain some physical phenomenon using our intuition we often fail, showing that intuition is a poor teacher. ] ''(])'' 13:36, 15 December 2023 (UTC) | |||
:::What Newton thought might be of interest historically but physics has moved on a long way since his time, in both what we know and how we describe it. From my reading of that he used it for more than we would today: e.g. the first example of repulsing electrons. But no, there are two concepts as expressed in the article and it summarises in the lede. And that essay hardly seems a reliable source: more a personal essay by someone with some odd views, on a web site created to push his self-published book.--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 17:57, 6 November 2010 (UTC) | |||
I don't think that maths needs to come into it at all. And I don't think our intuition is failing us when we observe the phenomenon of centrifugal force having a real physical effect. The non-physics public have usually been aware of centrifugal force since they were children, when they saw somebody swing a bucket of water over their heads and the water not falling out. It seems to me that you have got too distracted by the mathematical analysis, to the extent that you have made yourself believe that centrifugal force as a practical reality is merely a figment of a particular method of mathematical analysis. Before you wrote what you wrote above, I was going to sarcastically suggest that you remove all those references to centrifugal clutches and centrifugal governors etc., just in case the readers might get ideas that conflict with the fictitious narrative which the article seems to be promoting. Anyway, I've said all I can say and so I'll leave you to think about it. ] (]) 16:14, 15 December 2023 (UTC) | |||
John, The article mentioned three concepts in connection with Newton. I had discounted the first concept in my count of five. Newton's other two concepts are exactly the same two concepts that you have already accepted. Ie. the reactive force and the inertial force in a rotating frame of reference. So you should have no problem with the bit about what Newton said. The article then went on to talk about polar coordinates. That is not in any doubt. We formulate the planetary orbital equation in polar coordinates and the radial equation has an outward centrifugal force term. Then he mentioned about normal and tangential resolutions of velocity. I found his remarks about 'no Coriolis force' in this system to be very interesting. I see no grounds for you to either doubt what the author has said, or to deem the source to be unreliable. | |||
:We don't need to argue maths or intuition - we could, but we've been down that path before and it rarely helps improve the article. We just need to follow reliable sources. Reliable sources indicate that when we are rigorous in our definition of what is a force (eg, something that appears on the left hand side of Newton's second law), the centrifugal force does not appear in inertial frames. When motion is described in rotating frames/coordinate systems, then it is included in the sum of forces if we want to "bootstrap" of Newton's laws to non-inertial frames. If you have reliable sources that say otherwise, or provide additional insight or commentary not currently found in the article, please share them and help us make this article better. --] (]) 18:09, 15 December 2023 (UTC) | |||
And for your information, in my own personal opinion, there is only one single concept of centrifugal force. In my view, four of the five mentioned in the source are one and the same thing. The so-called reactive force is merely a knock-on effect of the inertial force, just as a brick falling on somebody's head is a knock-on effect of gravity. ] (]) 18:12, 6 November 2010 (UTC) | |||
OK, I see what you are saying now. You are saying that centrifugal force doesn't conform to the definition of force as per Newton's laws of motion. And of course, that should be stated in the article. But I've been thinking more about the matter, and I think you are giving undue weight to a scientific definition of force, over the head of the common understanding of the very real phenomenon known as centrifugal force. | |||
:None of this really matters. The is a ''very'' intereresting work (- i.m.o. it is piece of art -) but it can never serve as an authoritative source as a basis for Misplaced Pages content. It is someone's personal (and, apart from one chapter, ''book-unpublished'') view. It clearly is an ideal entry for the ''External links'' section, and perhaps even for the ''Further reading'' list, but the unpublished parts can never be used as a ], and can certainly never replace a solid textbook source. ] (]) 18:37, 6 November 2010 (UTC) | |||
Look at it this way. A car swerves round a corner at high speed and a passenger gets flung out the back door. We would all agree that this was because of the passenger's tendency to continue in their straight line inertial path. And this tendency caused the passenger to push against the car door, causing the car door to open and the passenger to be thrown out into the road. Now we'll all agree that this tendency was very real. But are we not allowed to call this tendency centrifugal force? | |||
What exactly is it that you are claiming is only an illusion in a rotating frame of reference? We can't write off the tendency to be pushed against the door, simply on the grounds that it is only an illusion under a certain kind of mathematical analysis. The effect is very real, and it's now clear to me that this discussion is purely over semantics. It's all about whether or not we are allowed to refer to, what is commonly known as centrifugal force, by its common name. | |||
I think we're all agreed that centrifugal force, under the common understanding, arises as a result of inertial motion, and not because of any choice of coordinate frame. But I do see your argument that centrifugal force within the common understanding does not conform with the strictly scientific definition of force as per Newton's laws of motion. | |||
I think the common understanding of centrifugal force should come first in the article, followed by the clarification that it is a local term not strictly in line with the definition of force as is used in Newtonian mechanics. | |||
I say this, because as the article stands now, it is counter intuitive, giving the impression that what most people see as a real effect with a familiar name, can be made to become an illusion by mathematicians operating in a rotating frame of reference. Those devices listed in the introduction really do operate by centrifugal force under the common understanding. You cannot write that fact off by insisting that it doesn't conform to a strict scientific definition of force. The issue is semantics, not physics. ] (]) 20:15, 15 December 2023 (UTC) | |||
:And one final comment. The issue of contention lies totally with the fact that a centrifugal force is not a Newtonian force. But its physical effect in a rotating space station for the purpose of simulating weight, is identical to that of the force of gravity. Therefore it's more accurate to state that centrifugal force is a force in a different category of forces than Newtonian forces. It's a bit like that a lion and a tiger are both cats, but a lion isn't a tiger. A Newtonian force and a centrifugal force are both forces, but a centrifugal force is not a Newtonian force. I can't get this idea of writing centrifugal force off completely, as an illusion in a rotating frame, just because it isn't a Newtonian force. In fact, more accurately a centrifugal force is an inertial force, independent of whatever mathematical way we analyse it. ] (]) 23:03, 15 December 2023 (UTC) | |||
Dvdm, Is your only concern about a solid textbook source which uses polar coordinates as an illustration of centrifugal force? Are you seriously doubting that centrifugal force is a polar coordinate term in the radial planetary orbital equation? ] (]) 19:07, 6 November 2010 (UTC) | |||
::Hence the article we have on this other category of forces, ], which you will find is linked in the opening sentence of the article by one of its other names, 'Inertial force'. No changes appear to be needed to the article. ] (]) 23:15, 15 December 2023 (UTC) | |||
: Even if it were properly sourced the introduction is not the place to introduce sourced material. It should be introduced into the body of the article, properly integrated in what is a well established article. As for the content I still find what you added confusing and unclear, in particular what you mean by context. Polar coordinates are just another coordinate system, but there are an infinite number of them, any of which could be used to calculate the force, as they are largely interchangeable – Lagrangian mechanics is one way of approaching this. It's not clear what "normal and tangential resolutions of velocity" have to do with centrifugal force. And the others are what is there already, and in the article.--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 19:45, 6 November 2010 (UTC) | |||
:You have written “A car swerves round a corner at high speed and a passenger gets flung out the back door. ... ...” This is a useful example and it is worth examining in further detail. | |||
: The car and its occupants are all travelling in a straight line at constant speed so the net force acting on each one is zero. The car then swerves and the passenger is ejected from the car and continues in a straight line at constant speed, at least for a short time. As the passenger is leaving the car a centrifugal force is acting on this unfortunate person. Once clear of the vehicle, the centrifugal force acting on the passenger falls to zero again. You are suggesting that the commencement of the centrifugal force, its magnitude, direction and duration are not determined by the trajectory of the passenger, but by the trajectory of the car. That is not consistent with Newton’s second law. ] ''(])'' 01:37, 16 December 2023 (UTC) | |||
Mr. Ollie. The first sentence in this article confuses the issue. We're agreed that centrifugal force is not a Newtonian force. Therefore we need to remove the bit where it says "in Newtonian mechanics". The next bit where it says that centrifugal force is an inertial force is fine. But then it immediately delves into the issue that I first raised. Just because it is an inertial force doesn't mean that it is an illusion only observed in a rotating frame of reference. It's no illusion that centrifugal force can be used to simulate the weight of gravity in a rotating space station. I thought we had it all sorted when you correctly drew my attention to the fact that centrifugal force is not a Newtonian force. But it seems that you still think it is an illusion, dependent on choice of coordinate frame. This is clearly not the case. ] (]) 23:39, 15 December 2023 (UTC) | |||
John, It's a simple yes or no question. Do you accept the fact that centrifugal force is a term in polar coordinates which is used in the radial planetary orbital equation without involving rotating frames of reference? ] (]) 19:53, 6 November 2010 (UTC) | |||
: Take your questions to the ref desk if you don't understand the topic. If this is about the article I don't see how your question relates to it. Perhaps you could point to the section of the article you think is wrong and suggest a, reliably sourced, way to improve it.--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 19:57, 6 November 2010 (UTC) | |||
:The only one who has used the word 'illusion' is you. ] (]) 00:00, 16 December 2023 (UTC) | |||
John, You didn't answer the question. The section in the article which you are asking about doesn't exist for the reason that some editors in the past have rejected the idea that centrifugal force is a term in the radial planetary orbital equation. I have supplied a source which states that centrifugal force is a term in polar coordinates outside of the context of rotating frames of reference. Do you have any objections to that material being put into the article on the basis of your own beliefs, or is it purely a matter of whether or not the source is reliable? ] (]) 20:08, 6 November 2010 (UTC) | |||
: Everything here needs a reliable source, and you have yet to supply one; it has nothing to do with "my beliefs".--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 20:23, 6 November 2010 (UTC) | |||
Mr. Ollie. It says in the first sentence, ''"appears to act on all objects when viewed in a rotating frame of reference"''. I interpret that as stating that it is only an illusion. But we know that it is not an illusion. It may not be a Newtonian force, but it is still a force, and it can have the same physical effect as a Newtonian force, as per the example I gave of weight being caused by rotation in a space station. I suggest that the introduction runs through the following key points, | |||
::See also at the ]. ] (]) 20:30, 6 November 2010 (UTC) | |||
'''''″When an object is forced to rotate in a rotating system, a centrifugal force draws it away from the centre of rotation, due to the tendency of the object to continue along its uniform straight line inertial path. Centrifugal force is therefore an inertial force and not a Newtonian force, as the latter kind is not involved in uniform straight line motion. Centrifugal force is often analysed in a frame of reference that rotates with the rotating system″''''' | |||
::Didn't we have some of this discussion re: the radial equation of planetary orbits a little more than a year ago? "Introduction to Classical Mechanics" Atam P. Arya (1990), pg 231 is a reference that explicitly connects the moving the centripetal acceleration term to the force of the equation to get the radial equation as equivalent to viewing the physics from a non-inertial frame rotating with the planet. Jeremy B. Tatum "Celestial Mechanics" Chapter 16 also clearly places the radial equation in a co-rotating, non-inertial frame. --] (]) 20:44, 6 November 2010 (UTC) | |||
:::Ah, I see. So this is nothing new, just reopening the ] interrupted only by ]. I suggest that if David Tombe has nothing new to bring to this discussion he stops it now, especially disrupting multiple venues with the same flawed arguments, in case he attracts the same sort of attention that got him banned a year ago.--<small>]</small><sup>]</sup><sub style="margin-left:-2.0ex;">]</sub> 20:59, 6 November 2010 (UTC) | |||
::::I agree. All input from David Tombe is best ignored; it was a large part of the reason for the massive bloat in these articles and for Brews ohare's problem and eventual banning. He is well known as a physics crank, and has done nothing to move away from that position in his year off. ] (]) 18:37, 22 December 2010 (UTC) | |||
In fact, that's about all there is to it. It's not a very extensive topic. ] (]) 00:28, 16 December 2023 (UTC) | |||
Dicklyon, That is quite untrue. My input to the various centrifugal force articles has been negligible, and I have consistently advocated that we only need to have one very short article. As regards the 'crank' position which are are referring to, it is very well depicted by Bond's adversary in that cartoon that you seem so keen to include in these articles. ] (]) 19:47, 14 January 2011 (UTC) | |||
:The "Appears to act" version is correct. Your suggestion is incorrect because it leaves out crucial information. If an observer is outside of the rotating system, they will not observe any such force - that is what distinguishes a fictitious force. It only 'appears' when the observer (that is, the frame of reference) is undergoing acceleration (in this case as rotation). ] (]) 00:42, 16 December 2023 (UTC) | |||
:Your several hundred article edits and several hundred talk-page edits in April–July 2008 kicked off and fueled the period of Brews hyper-inflation. ] (]) 00:12, 15 January 2011 (UTC) | |||
:(after ec) As MrOllie points out, that definition is incorrect and not supported by reliable sources. An object does not need to be forced to rotate in a rotating system for the centrifugal force to act on it. In the inertial frame there is no force that is pushing the passenger into the wall of the car or pushing astronauts against the floor in a spinning space station. Our intuition that there is one is due to our observations being in the non-inertial frame. | |||
:In the cartoon, when 'hat guy' says, "A laughable claim, Mister Bond, perpetuated by overzealous teachers of science. Simply construct Newton's laws into a rotating system and you will see a centrifugal force term appear as plain as day," he is indeed displaying some of your confusion. In one sense, he is entirely correct: "construct Newton's laws into a rotating system and you will see a centrifugal force term appear." That's what's called a "fictitious force", and I think we all agree that it arises from a rotating reference system. On the other hand, he is probably just confused about "overzealous teachers of science," likely because he doesn't know what to make of the term "fictitious"; this is the same problem you have exhibited many times. Mr Bond is also perhaps confused when he says "there's no such things as..."; you can interpret his position as meaning that he understands that he'll be crashed by the rim of wheel accelerating him along a curved path. Perhaps it's true that these "overzealous teachers" who deny "centrifugal force" actually exist; it would be interesting to find a sourced discussion of that if so. ] (]) 00:26, 15 January 2011 (UTC) | |||
:The centrifugal force that you mention is as real as the apparent force one feels pulling down when going up in an elevator. In the inertial frame the effects in the car, space station, and elevator are due to inertia and require no new force. In my opinion this is evident when we consider an object that is stationary in the inertial frame - when viewed in a rotating frame, the object appears to be moving in a circle and therefore undergoing centripetal acceleration. In the rotating frame, the centripetal acceleration is attributed to a combination of fictitious/inertial forces - the centrifugal force pointed outward and a Coriolis force pointed inward. The centrifugal force in this situation is the same as what arises for the passenger and astronauts, and appears because the frame has a rotational acceleration relative to the inertial frame. This is what reliable sources say. Again if you have reliable sources that say otherwise or clarify the concept, then please share. --] (]) 00:59, 16 December 2023 (UTC) | |||
Dolphin51, You misrepresented what I said above. I said that when the car swerves, centrifugal force throws the passenger against the door of the car, due to the tendency of the passenger to undergo his uniform straight line inertial path. We were already agreed that this centrifugal force is not a Newtonian force, but it is a force nevertheless. ] (]) 09:30, 16 December 2023 (UTC) | |||
Dick, The centrifugal force(rotating frame of reference) perspective is certainly the most prolific in the modern literature. But it is also specialist. It is for advanced mathematicians. It is a mathematical subject about describing how things are viewed from a rotating frame of reference. It is not about physical inertia. It involves using mutually cancelling fictitious forces in relation to stationary objects which have no inertia. That is not the perspective that Bond's adversary is invoking in the cartoon. Bond's adversary is invoking real physical inertia which crushes bones. Bonds adversary is talking about coordinates fixed in a physically rotating system which induces an outward inertial force. These are two distinct ideological perspectives on centrifugal force. They both need to be treated in separate sections within a single article on centrifugal force. The two perspectives overlap in the co-rotating scenario in which case the fictitious term is describing an actual inertial force. | |||
:Mr. Ollie, There is a paragraph in this link about how a centrifugal clutch works. We don't have to be rotating with the clutch in order it observe it working. https://www.lancereal.com/centrifugal-clutch-explained/ And here's another about the centrifugal pump, https://www.northridgepumps.com/article-346_what-is-a-centrifugal-pump You claimed above that we only observe the centrifugal force if we are in a rotating frame. This is obviously not the case. ] (]) 09:33, 16 December 2023 (UTC) | |||
Mr. Bond's perspective is yet a third perspective which is popular amongst high school students. And then of course there is Isaac Newton's perspective about centrifugal force being a reaction to centripetal force. You have your opinion on which is the correct perspective, and I have mine. But both need to be represented in a single article. And at least we are both agreed that neither Newton's nor Bond's opinions are correct. It seems to be a battle over whether it is the rotating frames of reference perspective or the Leibniz perspective, with myself supporting the latter. ] (]) 00:42, 15 January 2011 (UTC) | |||
::Fyzixfighter, If an object in a rotating system doesn't rotate with the system, say due to lack of friction for example, then the object will not move outwards. There will be no centrifugal force. You seem to be totally absorbed in the mathematical analysis from the perspective of a rotating frame of reference, to the neglect of the actual concept of centrifugal force itself. Your example of viewing a stationary object from a rotating frame of reference is a totally unnatural example which turns the whole topic upside down. It was like asking how do children on a roundabout see a stationary child on the ground below the roundabout. The stationary child experiences no centrifugal force, while the ones on the roundabout see the stationary child moving in a circle. Meanwhile you are trying to use maths to account for why the child on the ground experiences no centrifugal force, as in, because it is cancelled by another fictitious force. That is totally inverted logic, well over the top. As regards reliable sources, that would be fine if reliable sources all spoke with a single narrative. But they don't. Reliable sources are a morass of confusion telling many different narratives. Some talk about rotating frames and fictitious forces, some talk about Newton's third law, and some think there has to be circular motion. It won't be possible to taper the article to the correct balance of reliable sources until there is first some evidence of comprehension of the topic on the part of the editors. So, are we first going to try and reason it out using natural reasoning, or are we going to use the canard about reliable sources every time a point is made that undermines the current narrative in the article? What about this source here, https://www.irjet.net/archives/V4/i1/IRJET-V4I1185.pdf ? It says in the abstract that the centrifugal governor works by centrifugal force. It doesn't say that it only works if you are rotating with the apparatus. And by the way, your analogy about the elevator was wrong. When an elevator accelerates upwards, the people feel an upward force coming from the elevator floor. No inertial forces are involved, and the floor exerts an active force on the people. But in the rotating space station, centrifugal force pushes the people against the floor. It's the other way around. ] (]) 09:36, 16 December 2023 (UTC) | |||
:David, you seem to have a completely different understanding of this subject from physicists. I suggest that you continue on your talk page with those interested. ] (]) 02:53, 15 January 2011 (UTC) | |||
We've been down this path multiple times before. The archives are full of lengthy discussions with multiple editors, one in particular (FDT/David Tombe), that led to only marginal improvements in the article and certain editors (eg, FDT/David Tombe) being banned from physics-related articles and discussions. I'm not seeing anything new in this discussion, and in fact it seems to be largely rehashing those previous discussions. As we've fallen into trying to teach each other "correct" physics/semantics, I really don't see any further value in talk page discussion - this isn't a forum or discussion board. Perhaps an RFC or other dispute resolution avenue would be beneficial if you feel that there is a specific improvement needed in the article. --] (]) 16:19, 16 December 2023 (UTC) | |||
Martin, OK. See you there. ] (]) 11:48, 15 January 2011 (UTC) | |||
:Well, if you've been down this path multiple times before, then maybe it's time to take note of the fact that the lead paragraph contains a ridiculous contradiction. On the one hand it lists mechanical devices that operate on the principle of centrifugal force, while on the other hand it claims that centrifugal force is only an illusion seen by those in a rotating frame of reference. I have explained to you, that you have got yourself absorbed in the mathematical analysis of centrifugal force in a rotating frame, at the expense of the concept itself. Just because it is not a Newtonian force doesn't mean that it is not a force. It still pushes and pulls. I have supplied references above that contradict the view that centrifugal force is only an illusion observed from a rotating frame of reference, and so there's not much more that I can do to help. Whatever, the article as it stands, is a total morass of confusion. By the way, I see reference to another article called "reactive centrifugal force". There is no such thing. It's just inertial centrifugal force pushing or pulling against an obstacle. Was that article, by any chance, started up in order to package away out of sight all scenarios that exposed centrifugal force as a frame-independent force? ] (]) 16:55, 16 December 2023 (UTC) | |||
::Right, except nobody is interested. I'll go back to following my advice and ignoring David. ] (]) 05:12, 15 January 2011 (UTC) | |||
::{{tq|Was that article, by any chance, started up in order to package away out of sight all scenarios that exposed centrifugal force as a frame-independent force?}} You will find that launching conspiracy theories will not help your arguments. It seems that we are done here. ] (]) 16:59, 16 December 2023 (UTC) | |||
Well if I am wrong, then why aren't those examples simply included in this article? Why did they have to be sided off to a separate article? ] (]) 17:05, 16 December 2023 (UTC) | |||
Dick, The problem would be greatly assisted if we could actually pin you down to a definite opinion in all of this. ] (]) 11:47, 15 January 2011 (UTC) |
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direction of centrifugal force
Regarding this edit, asserting that:
ω x (ω x r) is always perpendicular to ω
I don't think this is true.
If F_centrifugal = mω x (ω x r)
then by the rules of the :
=F_centrifugal=m( =m().
Yes, the second term is always radially outward, since it has magnitude in the r direction, but the first time doesn't have to be 0 so long as and r are not perpendicular.
For example, consider an objective in helical motion such that it is completing counterclockwise circles in xy plane as viewed from +z direction so that its r has a component n the z direction so that has a component in the xy plane. That would make and thus ω x (ω x r) has a component in the direction and is not only radially outward.--Louiedog (talk) 11:43, 5 June 2017 (UTC)
- I have just realised that the formula for centrifugal force you quote from the article was missing a minus sign. But with that correction, yes indeed, Fcentrifugal = – m {(ω · r) ω – (ω · ω) r} , and therefore
- ω · Fcentrifugal = – m {(ω · r) (ω · ω) – (ω · ω) (ω · r)} = 0 .
- That is, Fcentrifugal is perpendicular to ω. It is, in fact, a well-known property of the vector cross product, a × b, that it is always perpendicular to both of its multiplicands, a and b, and, in particular, –ω × (ω × r) is always perpendicular to ω. It is, in fact, just ω times the projection of the vector r onto the plane perpendicular to ω.
- Note also that the centrifugal force is an artefact of the motion of the coordinate system in which the motion of objects is being described, and this does not necessarily bear any relation whatsoever to the motion of any of those objects themselves. I presume the helical motion you have in mind is one in which the body's position r(t) at time t is given by something like r(t) = ρ cos(ω t) i + ρ sin(ω t) j + vz t k. But the ω in this expression is the angular velocity of the body in question about the z axis, and not (necessarily) that of the coordinate system in which the motion of the body is being described. If the coordinate system determined by the three unit vectors i, j and k is inertial, for instance, then the angular velocity of that coordinate sytem is zero, and there will be no centrifugal force on the body in that coordinate system. For the body to be following such a helical path, there must, of course, be a proper force,
- m ..r(t) = − m ω ( ρ cos(ω t) i + ρ sin(ω t) j ) ,
- acting on it. This force is directed towards, and perpendicular to, the z axis of the inertial coordinate system. In a coordinate system whose origin and z axis coincide with those of the inertial system, but is rotating with angular velocity ω = ω k, the x and y coordinates of the body will be constant, and it will be moving with uniform velocity parallel to the z axis. In this coordinate system there will be a centrifugal force m ω ( ρ cos(ω t) i + ρ sin(ω t) j ) acting on the body which exactly balances the proper force. This centrifugal force is clearly, as it must always be, perpendicular to ω.
- David Wilson (talk · cont) 14:21, 5 June 2017 (UTC)
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Inertial Motion
I changed the lead sentence because it's inertial motion and not observation that gives rise to centrifugal force. If an object is drawn to the edge of a rotating system by centrifugal force, this can be observed from any vantage point. Newton's rotating bucket is a prime example. You don't have to be rotating inside the bucket in order to observe the water being pushed against the bucket's walls. 2A00:23CC:4D80:1101:8D3C:FAAF:EB21:11FE (talk) 21:45, 14 December 2023 (UTC) On another point, the last sentence in the top paragraph talks about something called reactive centrifugal force, as though it's something different. It's just the same centrifugal force pushing or pulling against a centripetal force. It would be there anyway, even if the centripetal force wasn't there, and so it's not a reaction. The centripetal force curves the path of the object and it doesn't even have to be equal in magnitude to the centrifugal force unless it is causing circular motion.2A00:23CC:4D80:1101:8D3C:FAAF:EB21:11FE (talk) 21:52, 14 December 2023 (UTC)
- I'm in favor of simplifying, but that oversimplification crosses into being incorrect. It's not observation that gives rise to centrifugal force, but describing the motion using a rotating/non-inertial coordinate system. From an inertial coordinate system, there is never a reason to invoke this centrifugal force to explain the motion - Newton's second law and a centripetal force are sufficient to explain the Newton's rotating bucket thought experiment. In Newton's thought experiment, it is actually the need to invoke an ad hoc centrifugal force that tells you the coordinate system is rotating. The text follows what is found in reliable sources such as journal articles and university textbooks. If you can indicate where the text does not appear to follow reliable sources, that would be helpful in refining the article. --FyzixFighter (talk) 23:35, 14 December 2023 (UTC)
Well I'm afraid I'll have to disagree with you. The first paragraph mentions mechanical devices that operate on the basis of centrifugal force. How would these work if centrifugal force is only something that depends on the choice of coordinate frame? Surely centrifugal force has to be caused by inertial motion and not by choice of coordinate frame. 2A00:23CC:4D80:1101:58A2:F0FE:6C9A:FB30 (talk) 10:36, 15 December 2023 (UTC)
- I agree with FyzixFighter. I have amended the lead to remove the suggestion that there are mechanical devices that operate on the basis of centrifugal force. Centrifugal force is a fictitious force, and it is lacking in rigour to use this force to attempt to explain the operation of certain rotating machines. Nevertheless there are people who incorporate the words “centrifugal force” into their explanation of operation of these machines.
- Centrifugal force is like the luminiferous aether and caloric - scientists now know they don’t exist even though in by-gone days everyone thought they did. Dolphin (t) 12:32, 15 December 2023 (UTC)
In a centrifuge, the material that is rotating with the machine, flies out to the edge because of its tendency to continue in its straight line inertial path. It pushes against the edge of the machine and Archimedes' principle is invoked, segregating the heavier particles from the lighter particles. That's an example of centrifugal force. I don't see this as being an effect that depends on the choice of coordinate frame for analysis. Same principle with a centrifugal clutch or a centrifugal governor. However you might analyse these, there is a force pressing outwards that has a mechanical effect. Are you one hundred percent sure about what you have said above? Think about it. I simply can't agree with you. 2A00:23CC:4D80:1101:B0C8:EC5D:84BA:4D00 (talk) 13:01, 15 December 2023 (UTC)
- Thanks for your prompt reply. If you spend some time carefully reading a physics textbook that covers introductory mechanics, and you focus on displacement, velocity and acceleration; and Newton’s laws of motion, we will end up agreeing with each other. When we try to explain some physical phenomenon using our intuition we often fail, showing that intuition is a poor teacher. Dolphin (t) 13:36, 15 December 2023 (UTC)
I don't think that maths needs to come into it at all. And I don't think our intuition is failing us when we observe the phenomenon of centrifugal force having a real physical effect. The non-physics public have usually been aware of centrifugal force since they were children, when they saw somebody swing a bucket of water over their heads and the water not falling out. It seems to me that you have got too distracted by the mathematical analysis, to the extent that you have made yourself believe that centrifugal force as a practical reality is merely a figment of a particular method of mathematical analysis. Before you wrote what you wrote above, I was going to sarcastically suggest that you remove all those references to centrifugal clutches and centrifugal governors etc., just in case the readers might get ideas that conflict with the fictitious narrative which the article seems to be promoting. Anyway, I've said all I can say and so I'll leave you to think about it. 2A00:23CC:4D80:1101:59EA:8F9E:A7A5:D64F (talk) 16:14, 15 December 2023 (UTC)
- We don't need to argue maths or intuition - we could, but we've been down that path before and it rarely helps improve the article. We just need to follow reliable sources. Reliable sources indicate that when we are rigorous in our definition of what is a force (eg, something that appears on the left hand side of Newton's second law), the centrifugal force does not appear in inertial frames. When motion is described in rotating frames/coordinate systems, then it is included in the sum of forces if we want to "bootstrap" of Newton's laws to non-inertial frames. If you have reliable sources that say otherwise, or provide additional insight or commentary not currently found in the article, please share them and help us make this article better. --FyzixFighter (talk) 18:09, 15 December 2023 (UTC)
OK, I see what you are saying now. You are saying that centrifugal force doesn't conform to the definition of force as per Newton's laws of motion. And of course, that should be stated in the article. But I've been thinking more about the matter, and I think you are giving undue weight to a scientific definition of force, over the head of the common understanding of the very real phenomenon known as centrifugal force. Look at it this way. A car swerves round a corner at high speed and a passenger gets flung out the back door. We would all agree that this was because of the passenger's tendency to continue in their straight line inertial path. And this tendency caused the passenger to push against the car door, causing the car door to open and the passenger to be thrown out into the road. Now we'll all agree that this tendency was very real. But are we not allowed to call this tendency centrifugal force? What exactly is it that you are claiming is only an illusion in a rotating frame of reference? We can't write off the tendency to be pushed against the door, simply on the grounds that it is only an illusion under a certain kind of mathematical analysis. The effect is very real, and it's now clear to me that this discussion is purely over semantics. It's all about whether or not we are allowed to refer to, what is commonly known as centrifugal force, by its common name. I think we're all agreed that centrifugal force, under the common understanding, arises as a result of inertial motion, and not because of any choice of coordinate frame. But I do see your argument that centrifugal force within the common understanding does not conform with the strictly scientific definition of force as per Newton's laws of motion. I think the common understanding of centrifugal force should come first in the article, followed by the clarification that it is a local term not strictly in line with the definition of force as is used in Newtonian mechanics. I say this, because as the article stands now, it is counter intuitive, giving the impression that what most people see as a real effect with a familiar name, can be made to become an illusion by mathematicians operating in a rotating frame of reference. Those devices listed in the introduction really do operate by centrifugal force under the common understanding. You cannot write that fact off by insisting that it doesn't conform to a strict scientific definition of force. The issue is semantics, not physics. 2A00:23CC:4D80:1101:797D:908D:F9D2:B75A (talk) 20:15, 15 December 2023 (UTC)
- And one final comment. The issue of contention lies totally with the fact that a centrifugal force is not a Newtonian force. But its physical effect in a rotating space station for the purpose of simulating weight, is identical to that of the force of gravity. Therefore it's more accurate to state that centrifugal force is a force in a different category of forces than Newtonian forces. It's a bit like that a lion and a tiger are both cats, but a lion isn't a tiger. A Newtonian force and a centrifugal force are both forces, but a centrifugal force is not a Newtonian force. I can't get this idea of writing centrifugal force off completely, as an illusion in a rotating frame, just because it isn't a Newtonian force. In fact, more accurately a centrifugal force is an inertial force, independent of whatever mathematical way we analyse it. 2A00:23CC:4D80:1101:10E3:814:D19C:C3B (talk) 23:03, 15 December 2023 (UTC)
- Hence the article we have on this other category of forces, Fictitious force, which you will find is linked in the opening sentence of the article by one of its other names, 'Inertial force'. No changes appear to be needed to the article. MrOllie (talk) 23:15, 15 December 2023 (UTC)
- You have written “A car swerves round a corner at high speed and a passenger gets flung out the back door. ... ...” This is a useful example and it is worth examining in further detail.
- The car and its occupants are all travelling in a straight line at constant speed so the net force acting on each one is zero. The car then swerves and the passenger is ejected from the car and continues in a straight line at constant speed, at least for a short time. As the passenger is leaving the car a centrifugal force is acting on this unfortunate person. Once clear of the vehicle, the centrifugal force acting on the passenger falls to zero again. You are suggesting that the commencement of the centrifugal force, its magnitude, direction and duration are not determined by the trajectory of the passenger, but by the trajectory of the car. That is not consistent with Newton’s second law. Dolphin (t) 01:37, 16 December 2023 (UTC)
Mr. Ollie. The first sentence in this article confuses the issue. We're agreed that centrifugal force is not a Newtonian force. Therefore we need to remove the bit where it says "in Newtonian mechanics". The next bit where it says that centrifugal force is an inertial force is fine. But then it immediately delves into the issue that I first raised. Just because it is an inertial force doesn't mean that it is an illusion only observed in a rotating frame of reference. It's no illusion that centrifugal force can be used to simulate the weight of gravity in a rotating space station. I thought we had it all sorted when you correctly drew my attention to the fact that centrifugal force is not a Newtonian force. But it seems that you still think it is an illusion, dependent on choice of coordinate frame. This is clearly not the case. 2A00:23CC:4D80:1101:F0EB:BBD8:6848:CEA1 (talk) 23:39, 15 December 2023 (UTC)
- The only one who has used the word 'illusion' is you. MrOllie (talk) 00:00, 16 December 2023 (UTC)
Mr. Ollie. It says in the first sentence, "appears to act on all objects when viewed in a rotating frame of reference". I interpret that as stating that it is only an illusion. But we know that it is not an illusion. It may not be a Newtonian force, but it is still a force, and it can have the same physical effect as a Newtonian force, as per the example I gave of weight being caused by rotation in a space station. I suggest that the introduction runs through the following key points,
″When an object is forced to rotate in a rotating system, a centrifugal force draws it away from the centre of rotation, due to the tendency of the object to continue along its uniform straight line inertial path. Centrifugal force is therefore an inertial force and not a Newtonian force, as the latter kind is not involved in uniform straight line motion. Centrifugal force is often analysed in a frame of reference that rotates with the rotating system″
In fact, that's about all there is to it. It's not a very extensive topic. 2A00:23CC:4D80:1101:8D8F:9CE:B079:7FFD (talk) 00:28, 16 December 2023 (UTC)
- The "Appears to act" version is correct. Your suggestion is incorrect because it leaves out crucial information. If an observer is outside of the rotating system, they will not observe any such force - that is what distinguishes a fictitious force. It only 'appears' when the observer (that is, the frame of reference) is undergoing acceleration (in this case as rotation). MrOllie (talk) 00:42, 16 December 2023 (UTC)
- (after ec) As MrOllie points out, that definition is incorrect and not supported by reliable sources. An object does not need to be forced to rotate in a rotating system for the centrifugal force to act on it. In the inertial frame there is no force that is pushing the passenger into the wall of the car or pushing astronauts against the floor in a spinning space station. Our intuition that there is one is due to our observations being in the non-inertial frame.
- The centrifugal force that you mention is as real as the apparent force one feels pulling down when going up in an elevator. In the inertial frame the effects in the car, space station, and elevator are due to inertia and require no new force. In my opinion this is evident when we consider an object that is stationary in the inertial frame - when viewed in a rotating frame, the object appears to be moving in a circle and therefore undergoing centripetal acceleration. In the rotating frame, the centripetal acceleration is attributed to a combination of fictitious/inertial forces - the centrifugal force pointed outward and a Coriolis force pointed inward. The centrifugal force in this situation is the same as what arises for the passenger and astronauts, and appears because the frame has a rotational acceleration relative to the inertial frame. This is what reliable sources say. Again if you have reliable sources that say otherwise or clarify the concept, then please share. --FyzixFighter (talk) 00:59, 16 December 2023 (UTC)
Dolphin51, You misrepresented what I said above. I said that when the car swerves, centrifugal force throws the passenger against the door of the car, due to the tendency of the passenger to undergo his uniform straight line inertial path. We were already agreed that this centrifugal force is not a Newtonian force, but it is a force nevertheless. 2A00:23CC:4D80:1101:BDDC:2E1F:8186:E19E (talk) 09:30, 16 December 2023 (UTC)
- Mr. Ollie, There is a paragraph in this link about how a centrifugal clutch works. We don't have to be rotating with the clutch in order it observe it working. https://www.lancereal.com/centrifugal-clutch-explained/ And here's another about the centrifugal pump, https://www.northridgepumps.com/article-346_what-is-a-centrifugal-pump You claimed above that we only observe the centrifugal force if we are in a rotating frame. This is obviously not the case. 2A00:23CC:4D80:1101:BDDC:2E1F:8186:E19E (talk) 09:33, 16 December 2023 (UTC)
- Fyzixfighter, If an object in a rotating system doesn't rotate with the system, say due to lack of friction for example, then the object will not move outwards. There will be no centrifugal force. You seem to be totally absorbed in the mathematical analysis from the perspective of a rotating frame of reference, to the neglect of the actual concept of centrifugal force itself. Your example of viewing a stationary object from a rotating frame of reference is a totally unnatural example which turns the whole topic upside down. It was like asking how do children on a roundabout see a stationary child on the ground below the roundabout. The stationary child experiences no centrifugal force, while the ones on the roundabout see the stationary child moving in a circle. Meanwhile you are trying to use maths to account for why the child on the ground experiences no centrifugal force, as in, because it is cancelled by another fictitious force. That is totally inverted logic, well over the top. As regards reliable sources, that would be fine if reliable sources all spoke with a single narrative. But they don't. Reliable sources are a morass of confusion telling many different narratives. Some talk about rotating frames and fictitious forces, some talk about Newton's third law, and some think there has to be circular motion. It won't be possible to taper the article to the correct balance of reliable sources until there is first some evidence of comprehension of the topic on the part of the editors. So, are we first going to try and reason it out using natural reasoning, or are we going to use the canard about reliable sources every time a point is made that undermines the current narrative in the article? What about this source here, https://www.irjet.net/archives/V4/i1/IRJET-V4I1185.pdf ? It says in the abstract that the centrifugal governor works by centrifugal force. It doesn't say that it only works if you are rotating with the apparatus. And by the way, your analogy about the elevator was wrong. When an elevator accelerates upwards, the people feel an upward force coming from the elevator floor. No inertial forces are involved, and the floor exerts an active force on the people. But in the rotating space station, centrifugal force pushes the people against the floor. It's the other way around. 2A00:23CC:4D80:1101:BDDC:2E1F:8186:E19E (talk) 09:36, 16 December 2023 (UTC)
We've been down this path multiple times before. The archives are full of lengthy discussions with multiple editors, one in particular (FDT/David Tombe), that led to only marginal improvements in the article and certain editors (eg, FDT/David Tombe) being banned from physics-related articles and discussions. I'm not seeing anything new in this discussion, and in fact it seems to be largely rehashing those previous discussions. As we've fallen into trying to teach each other "correct" physics/semantics, I really don't see any further value in talk page discussion - this isn't a forum or discussion board. Perhaps an RFC or other dispute resolution avenue would be beneficial if you feel that there is a specific improvement needed in the article. --FyzixFighter (talk) 16:19, 16 December 2023 (UTC)
- Well, if you've been down this path multiple times before, then maybe it's time to take note of the fact that the lead paragraph contains a ridiculous contradiction. On the one hand it lists mechanical devices that operate on the principle of centrifugal force, while on the other hand it claims that centrifugal force is only an illusion seen by those in a rotating frame of reference. I have explained to you, that you have got yourself absorbed in the mathematical analysis of centrifugal force in a rotating frame, at the expense of the concept itself. Just because it is not a Newtonian force doesn't mean that it is not a force. It still pushes and pulls. I have supplied references above that contradict the view that centrifugal force is only an illusion observed from a rotating frame of reference, and so there's not much more that I can do to help. Whatever, the article as it stands, is a total morass of confusion. By the way, I see reference to another article called "reactive centrifugal force". There is no such thing. It's just inertial centrifugal force pushing or pulling against an obstacle. Was that article, by any chance, started up in order to package away out of sight all scenarios that exposed centrifugal force as a frame-independent force? 2A00:23CC:4D80:1101:DD04:6DDA:A6E1:F358 (talk) 16:55, 16 December 2023 (UTC)
Was that article, by any chance, started up in order to package away out of sight all scenarios that exposed centrifugal force as a frame-independent force?
You will find that launching conspiracy theories will not help your arguments. It seems that we are done here. MrOllie (talk) 16:59, 16 December 2023 (UTC)
Well if I am wrong, then why aren't those examples simply included in this article? Why did they have to be sided off to a separate article? 2A00:23CC:4D80:1101:DD04:6DDA:A6E1:F358 (talk) 17:05, 16 December 2023 (UTC)
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