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{{Short description|Type of emission nebula created by dying red giants}} | |||
]]] | |||
{{Infobox astronomical formation|name=Planetary nebula|image=File:N1535s.jpg|caption=]|Mass=0.1{{solar mass}}-1{{solar mass}}<ref name=Osterbrock>{{citation | |||
| title = Astrophysics of gaseous nebulae and active galactic nuclei | |||
| last1 = Osterbrock | |||
| first1 = Donald E. | |||
| last2 = Ferland | |||
| first2 = G. J. | |||
| editor = Ferland, G. J. | |||
| publisher = University Science Books | |||
| date = 2005 | |||
| isbn = 978-1-891389-34-4 | |||
| url-access = registration | |||
| url = https://archive.org/details/astrophysicsofga0000oste | |||
}}</ref>|commonscat=Planetary nebulae|thing=]|size=~1 ly<ref name=Osterbrock/>|density=100 to 10,000 particles per cm{{sup|3}}<ref name=Osterbrock/>|qid=Q13632|discover=1764, ]<ref>{{Cite web |title=Messier 27 (The Dumbbell Nebula) |date=19 Oct 2017|url=https://www.nasa.gov/feature/goddard/2017/messier-27-the-dumbbell-nebula |website=nasa.gov}}</ref> }} | |||
] (NGC 6543)]] | |||
] captured the latest image of this planetary nebula, cataloged as ], and known informally as the Southern Ring Nebula. It is approximately 2,500 light-years away.]] | |||
], a planetary nebula with glowing wisps of outpouring gas that are lit up by a binary<ref name="Miszalski2011">{{harvnb|Miszalski|Jones|Rodríguez-Gil|Boffin|2011}}</ref> central star]] | |||
A '''planetary nebula''' is |
A '''planetary nebula''' is a type of ] consisting of an expanding, glowing shell of ] gas ejected from ] stars late in their lives.<ref name="Frankowskietal2009">{{harvnb|Frankowski|Soker|2009|pp=654–8}}</ref> | ||
The term "planetary nebula" is a ] because they are unrelated to ]s. The term originates from the planet-like round shape of these ]e observed by astronomers through early telescopes. The first usage may have occurred during the 1780s with the English astronomer ] who described these nebulae as resembling planets; however, as early as January 1779, the French astronomer ] described in his observations of the ], "very dim but perfectly outlined; it is as large as Jupiter and resembles a fading planet".<ref name=Darquier>{{cite book | |||
At the end of the star's life, during the ] phase, the outer layers of the star are expelled via pulsations and strong ]s. Without these ] layers, the remaining core of the star shines brightly and is very hot. The ] radiation emitted by this core ]<ref name="Frankowskietal2009" /> the ejected outer layers of the star which ] as a planetary ]. | |||
|last1=Darquier | |||
|first1=A. | |||
|date=1777 | |||
|title=Observations astronomiques, faites à Toulouse (Astronomical observations, made in Toulouse) | |||
|publisher=Avignon: J. Aubert; (and Paris: Laporte, etc.) | |||
|url=https://archive.org/details/BUSA077-240-_126}} | |||
</ref><ref name ="Olsen2017">{{cite magazine | |||
|last1=Olson | |||
|first1=Don | |||
|last2=Caglieris | |||
|first2=Giovanni Maria | |||
|date=June 2017 | |||
|title=Who Discovered the Ring Nebula? | |||
|magazine=Sky & Telescope | |||
|pages= 32–37}}</ref><ref name="Steinicke2018">{{cite web | |||
|title=Antoine Darquier de Pellepoix | |||
|author=Wolfgang Steinicke | |||
|url=http://www.klima-luft.de/steinicke/ngcic/persons/darquier.htm | |||
|access-date=9 June 2018}}</ref> | |||
Though the modern interpretation is different, the old term is still used. | |||
All planetary nebulae form at the end of the life of a star of intermediate mass, about 1-8 solar masses. It is expected that the ] will form a planetary nebula at the end of its life cycle.<ref>{{Cite web |last=Daley |first=Jason |date=May 8, 2018 |title=The Sun Will Produce a Beautiful Planetary Nebula When It Dies |url=https://www.smithsonianmag.com/smart-news/sun-will-produce-beautiful-planetary-nebula-when-it-dies-180969028/ |access-date=30 March 2020 |website=Smithsonian Magazine |language=en}}</ref> They are relatively short-lived phenomena, lasting perhaps a few tens of millennia, compared to considerably longer phases of ].<ref name="FrewParker2010">They are created after the red giant phase, when most of the outer layers of the star have been expelled by strong ]s {{harvnb|Frew|Parker|2010|pp=129–148}}</ref> Once all of the red giant's atmosphere has been dissipated, energetic ] ] from the exposed hot luminous core, called a planetary nebula nucleus (P.N.N.), ionizes the ejected material.<ref name="Frankowskietal2009" /> Absorbed ultraviolet light then energizes the shell of nebulous gas around the central star, causing it to appear as a brightly coloured planetary nebula. | |||
]</center>|alt=Star field with circular shell with green center and red at the edge of the shell.]] | |||
Planetary nebulae |
Planetary nebulae probably play a crucial role in the ] ] by expelling ]s into the ] from stars where those elements were created. Planetary nebulae are observed in more distant ], yielding useful information about their chemical abundances. | ||
Starting from the 1990s, ] images revealed that many planetary nebulae have extremely complex and varied morphologies. About one-fifth are roughly spherical, but the majority are not spherically symmetric. The mechanisms that produce such a wide variety of shapes and features are not yet well understood, but ], stellar winds and ]s may play a role. | |||
==Observations== | == Observations == | ||
], the ]]] | |||
]<br>''Credit: Robert J. Vanderbei''</center>]] | |||
], the ]]] | |||
Planetary nebulae are generally faint objects, and none is visible to the ]. The first planetary nebula discovered was the ] in the constellation of ], observed by ] in 1764 and listed as M27 in his ] of nebulous objects.<ref name=Kwok1>{{harvnb|Kwok|2000|pp=1–7}}</ref> To early observers with low-resolution telescopes, M27 and subsequently discovered planetary nebulae somewhat resembled the giant planets like ], and ], discoverer of this planet, eventually coined<ref name=Kwok1/> the term 'planetary nebula' for them, although, as we now know, they are very different from planets.<ref name=Moore2007>{{harvnb|Moore|2007|pp=279–80}}</ref> | |||
=== Discovery === | |||
]<br>''Credit: NASA, ESA, and C.R. O'Dell (Vanderbilt University)''</center>]] | |||
The nature of planetary nebulae was unknown until the first ] observations were made in the mid-19th century. ] was one of the earliest astronomers to study the ] of astronomical objects, using a ] to disperse their light.<ref name=Moore2007/> On August 29, 1864, Huggins was the first to take the spectrum of a planetary nebula when he analyzed ].<ref name=Kwok1/> His observations of stars showed that their spectra consisted of a ] with many ] superimposed on them, and he later found that many nebulous objects such as the ] (as it was then known) had spectra which were quite similar to this—these nebulae were later shown to be ]. | |||
The first planetary nebula discovered (though not yet termed as such) was the ] in the constellation of ]. It was observed by ] on July 12, 1764 and listed as M27 in his ] of nebulous objects.<ref name=Kwok1>{{harvnb|Kwok|2000|pp=1–7}}</ref> To early observers with low-resolution telescopes, M27 and subsequently discovered planetary nebulae resembled the giant planets like ]. As early as January 1779, the French astronomer ] described in his observations of the ], "a very dull nebula, but perfectly outlined; as large as Jupiter and looks like a fading planet".<ref name=Darquier/><ref name="Olsen2017"/><ref name="Steinicke2018"/> | |||
However, when he looked at the ], he found a very different spectrum. Rather than a strong continuum with absorption lines superimposed, the Cat's Eye Nebula and other similar objects showed only a small number of ]s.<ref name=Moore2007/> The brightest of these was at a wavelength of 500.7 ]s, which did not correspond with a line of any known element.<ref name=Huggins1864>{{harvnb|Huggins|Miller|1864|pp=437–44}}</ref> At first it was hypothesized that the line might be due to an unknown element, which was named ''nebulium''—a similar idea had led to the discovery of ] through analysis of the ]'s spectrum in 1868.<ref name=Kwok1/> | |||
]<br>''Credit: NASA, ESA, Andrew Fruchter (STScI), and the ERO team (STScI + ST-ECF)''</center>]] | |||
The nature of these objects remained unclear. In 1782, ], discoverer of Uranus, found the ] (NGC 7009) and described it as "A curious nebula, or what else to call it I do not know". He later described these objects as seeming to be planets "of the starry kind".<ref>{{Cite journal|last=Zijlstra|first=A.|date=2015|title=Planetary nebulae in 2014: A review of research|url=http://www.astroscu.unam.mx/rmaa/RMxAA..51-2/PDF/RMxAA..51-2_azijlstra.pdf |archive-url=https://ghostarchive.org/archive/20221009/http://www.astroscu.unam.mx/rmaa/RMxAA..51-2/PDF/RMxAA..51-2_azijlstra.pdf |archive-date=2022-10-09 |url-status=live|journal=Revista Mexicana de Astronomía y Astrofísica|volume=51|pages=221–230|arxiv=1506.05508|bibcode=2015RMxAA..51..221Z}}</ref> As noted by Darquier before him, Herschel found that the disk resembled a planet but it was too faint to be one. In 1785, Herschel wrote to ]: | |||
While helium was isolated on earth soon after its discovery in the spectrum of the sun, nebulium was not. In the early 20th century ] proposed that rather than being a new element, the line at 500.7 nm was due to a familiar element in unfamiliar conditions.<ref name=Kwok1/> | |||
<blockquote>These are celestial bodies of which as yet we have no clear idea and which are perhaps of a type quite different from those that we are familiar with in the heavens. I have already found four that have a visible diameter of between 15 and 30 seconds. These bodies appear to have a disk that is rather like a planet, that is to say, of equal brightness all over, round or somewhat oval, and about as well defined in outline as the disk of the planets, of a light strong enough to be visible with an ordinary telescope of only one foot, yet they have only the appearance of a star of about ninth magnitude.<ref>Quoted in {{cite journal|last1=Hoskin|first1=Michael|year=2014|title=William Herschel and the Planetary Nebulae|journal=Journal for the History of Astronomy|volume=45|issue=2|pages=209–225|bibcode=2014JHA....45..209H|doi=10.1177/002182861404500205|s2cid=122897343}}</ref></blockquote> | |||
Physicists showed in the 1920s that in gas at extremely low densities, ]s can populate ] ] ]s in atoms and ions which at higher densities are rapidly de-excited by collisions.<ref name=Bowen1927>{{harvnb|Bowen|1927|pp=295–7}}</ref> Electron transitions from these levels in ] and ] ions ({{nowrap|O<sup>2+</sup>}} or OIII, {{nowrap|O<sup>+</sup>}} and {{nowrap|N<sup>+</sup>}}) give rise to the 500.7 nm line and other lines.<ref name=Kwok1/> These spectral lines, which can only be seen in very low density gases, are called '']s''. Spectroscopic observations thus showed that nebulae were made of extremely rarefied gas.<ref name=Gurzadyan>{{harvnb|Gurzadyan|1997}}</ref> | |||
He assigned these to Class IV of his catalogue of "nebulae", eventually listing 78 "planetary nebulae", most of which are in fact galaxies.<ref>p. 16 in {{cite book|last1=Mullaney|first1=James|title=The Herschel Objects and How to Observe Them|year=2007|isbn=978-0-387-68124-5|series=Astronomers' Observing Guides|bibcode=2007hoho.book.....M|doi=10.1007/978-0-387-68125-2}}</ref> | |||
The central stars of planetary nebulae are very hot.<ref name="Frankowskietal2009" /> Only once a star has exhausted all its nuclear fuel can it collapse to such a small size, and so planetary nebulae came to be understood as a final stage of ]. Spectroscopic observations show that all planetary nebulae are expanding. This led to the idea that planetary nebulae were caused by a star's outer layers being thrown into space at the end of its life.<ref name=Kwok1/> | |||
Herschel used the term "planetary nebulae" for these objects. The origin of this term not known.<ref name="Kwok1" /><ref name="Moore2007">{{harvnb|Moore|2007|pp=279–80}}</ref> The label "planetary nebula" became ingrained in the terminology used by astronomers to categorize these types of nebulae, and is still in use by astronomers today.<ref name="seds2013">{{harvnb|SEDS|2013}}</ref><ref name="hubbleSite1997">{{harvnb|Hubblesite.org|1997}}</ref> | |||
Towards the end of the 20th century, technological improvements helped to further the study of planetary nebulae.<ref name=KwokJun2005 /> ]s allowed astronomers to study light emitted beyond the visible spectrum which is not detectable from ground-based observatories (because only radio waves and visible light penetrate the Earth's atmosphere). ] and ultraviolet studies of planetary nebulae allowed much more accurate determinations of nebular ]s, ] and abundances.<ref name=Hora2004>{{harvnb|Hora|Latter|Allen|Marengo|2004|pp=296–301}}</ref><ref name=Kwoketal2006>{{harvnb|Kwok|Koning|Huang|Churchwell|2006|pp=445–6}}</ref> ] technology allowed much fainter spectral lines to be measured accurately than had previously been possible. The Hubble Space Telescope also showed that while many nebulae appear to have simple and regular structures from the ground, the very high ] achievable by a telescope above the ] reveals extremely complex morphologies.<ref name=Reed1999>{{harvnb|Reed|Balick|Hajian|Klayton|1999|pp=2430–41}}</ref><ref name=Alleretal2003>{{harvnb|Aller|Hyung|2003|p=15}}</ref> | |||
=== Spectra === | |||
The nature of planetary nebulae remained unknown until the first ] observations were made in the mid-19th century. Using a ] to disperse their light, ] was one of the earliest astronomers to study the ] of astronomical objects.<ref name=Moore2007/> | |||
On August 29, 1864, Huggins was the first to analyze the spectrum of a planetary nebula when he observed ].<ref name=Kwok1/> His observations of stars had shown that their spectra consisted of a ] of radiation with many ] superimposed. He found that many nebulous objects such as the ] (as it was then known) had spectra that were quite similar. However, when Huggins looked at the Cat's Eye Nebula, he found a very different spectrum. Rather than a strong continuum with absorption lines superimposed, the Cat's Eye Nebula and other similar objects showed a number of ].<ref name=Moore2007/> Brightest of these was at a wavelength of 500.7 ]s, which did not correspond with a line of any known element.<ref name=Huggins1864>{{harvnb|Huggins|Miller|1864|pp=437–44}}</ref> | |||
At first, it was hypothesized that the line might be due to an unknown element, which was named ]. A similar idea had led to the discovery of ] through analysis of the ]'s spectrum in 1868.<ref name=Kwok1/> While helium was isolated on Earth soon after its discovery in the spectrum of the Sun, "nebulium" was not. In the early 20th century, ] proposed that, rather than being a new element, the line at 500.7 nm was due to a familiar element in unfamiliar conditions.<ref name=Kwok1/> | |||
Physicists showed in the 1920s that in gas at extremely low densities, ]s can occupy ] ] ]s in atoms and ions that would otherwise be de-excited by collisions that would occur at higher densities.<ref name=Bowen1927>{{harvnb|Bowen|1927|pp=295–7}}</ref> Electron transitions from these levels in ] and ] ions ({{nowrap|O<sup>+</sup>}}, ] (a.k.a. O {{Smallcaps|iii}}), and {{nowrap|N<sup>+</sup>}}) give rise to the 500.7 nm emission line and others.<ref name=Kwok1/> These spectral lines, which can only be seen in very low-density gases, are called '']s''. Spectroscopic observations thus showed that nebulae were made of extremely rarefied gas.<ref name=Gurzadyan>{{harvnb|Gurzadyan|1997}}</ref> | |||
] | |||
=== Central stars === | |||
The central stars of planetary nebulae are very hot.<ref name="Frankowskietal2009" /> Only when a star has exhausted most of its nuclear fuel can it collapse to a small size. Planetary nebulae are understood as a final stage of ]. Spectroscopic observations show that all planetary nebulae are expanding. This led to the idea that planetary nebulae were caused by a star's outer layers being thrown into space at the end of its life.<ref name=Kwok1/> | |||
=== Modern observations === | |||
Towards the end of the 20th century, technological improvements helped to further the study of planetary nebulae.<ref name=KwokJun2005>{{harvnb|Kwok|2005|pp=271–8}}</ref> ]s allowed astronomers to study light wavelengths outside those that the Earth's atmosphere transmits. ] and ultraviolet studies of planetary nebulae allowed much more accurate determinations of nebular ]s, ] and elemental abundances.<ref name=Hora2004>{{harvnb|Hora|Latter|Allen|Marengo|2004|pp=296–301}}</ref><ref name=Kwoketal2006>{{harvnb|Kwok|Koning|Huang|Churchwell|2006|pp=445–6}}</ref> ] technology allowed much fainter spectral lines to be measured accurately than had previously been possible. The Hubble Space Telescope also showed that while many nebulae appear to have simple and regular structures when observed from the ground, the very high ] achievable by telescopes above the ] reveals extremely complex structures.<ref name=Reed1999>{{harvnb|Reed|Balick|Hajian|Klayton|1999|pp=2430–41}}</ref><ref name=Alleretal2003>{{harvnb|Aller|Hyung|2003|p=15}}</ref> | |||
Under the ] scheme, planetary nebulae are classified as ''Type-'''P''''', although this notation is seldom used in practice.<ref name=Krause>{{harvnb|Krause|1961|p=187}}</ref> | Under the ] scheme, planetary nebulae are classified as ''Type-'''P''''', although this notation is seldom used in practice.<ref name=Krause>{{harvnb|Krause|1961|p=187}}</ref> | ||
==Origins== | ==Origins== | ||
] | ] | ||
Stars |
Stars greater than 8 ]es (M<sub>⊙</sub>) will probably end their lives in dramatic ]e explosions, while planetary nebulae seemingly only occur at the end of the lives of intermediate and low mass stars between 0.8 M<sub>⊙</sub> to 8.0 M<sub>⊙</sub>.<ref name="Macieletal2009">{{harvnb|Maciel|Costa|Idiart|2009|pp=127–37}}</ref> Progenitor stars that form planetary nebulae will spend most of their lifetimes converting their ] into ] in the star's core by ] at about 15 million ]. This generates energy in the core, which creates outward pressure that balances the crushing inward pressures of gravity.<ref name=Harpaz4>{{harvnb|Harpaz|1994|pp=55–80}}</ref> This state of equilibrium is known as the ], which can last for tens of millions to billions of years, depending on the mass. | ||
When the hydrogen in the core starts to run out, nuclear fusion generates less energy and gravity starts compressing the core, causing a rise in temperature to about 100 million K.<ref name=Harpaz6>{{harvnb|Harpaz|1994|pp=99–112}}</ref> Such high core temperatures then make{{how|date=December 2023}} the star's cooler outer layers expand to create much larger red giant stars. This end phase causes a dramatic rise in stellar luminosity, where the released energy is distributed over a much larger surface area, which in fact causes the average surface temperature to be lower. In ] terms, stars undergoing such increases in luminosity are known as ] (AGB).<ref name=Harpaz6/> During this phase, the star can lose 50–70% of its total mass from its ].<ref name=wood>{{cite journal | |||
Stars spend most of their lifetime shining as a result of ] reactions that convert ] to helium in the star's core. Outward pressure from fusion in the core balances inward collapse due to the star's own gravity.<ref name=Harpaz4>{{harvnb|Harpaz|1994|pp=55–80}}</ref> Such stars are said to be in the ]. | |||
| last1=Wood | first1=P. R. | last2=Olivier | first2=E. A. | |||
| last3=Kawaler | first3=S. D. | year=2004 | |||
| title=Long Secondary Periods in Pulsating Asymptotic Giant Branch Stars: An Investigation of Their Origin | |||
| journal=] | |||
| volume=604 | issue=2 | pages=800 | |||
| bibcode=2004ApJ...604..800W | doi=10.1086/382123 | doi-access= | s2cid=121264287 }}</ref> | |||
For the more massive asymptotic giant branch stars that form planetary nebulae, whose progenitors exceed about 0.6M<sub>⊙</sub>, their cores will continue to contract. When temperatures reach about 100 million K, the available ] fuse into ] and ], so that the star again resumes radiating energy, temporarily stopping the core's contraction. This new helium burning phase (fusion of helium nuclei) forms a growing inner core of inert carbon and oxygen. Above it is a thin helium-burning shell, surrounded in turn by a hydrogen-burning shell. However, this new phase lasts only 20,000 years or so, a very short period compared to the entire lifetime of the star. | |||
Medium to low mass stars run out of hydrogen in their cores after tens of millions to billions of years in the main sequence. Gravity compresses the core and it heats up. Currently the sun's core has a temperature of approximately 15 million ], but when it runs out of hydrogen, the compression of the core will cause the temperature to rise to about 100 million K.<ref name=Harpaz6>{{harvnb|Harpaz|1994|pp=99–112}}</ref> | |||
The venting of atmosphere continues unabated into interstellar space, but when the outer surface of the exposed core reaches temperatures exceeding about 30,000 K, there are enough emitted ] ]s to ] the ejected atmosphere, causing the gas to shine as a planetary nebula.<ref name=Harpaz6/> | |||
The outer layers of the star expand enormously and become much cooler in response to the very high temperature of the core. The star becomes a red giant. The core continues to contract and heat up, and when its temperature reaches 100 million K, helium nuclei begin to fuse into carbon and oxygen. The resumption of fusion reactions stops the core's contraction. Helium burning soon forms an inert core of carbon and oxygen, with both a helium-burning shell and a hydrogen-burning shell surrounding it. In this last stage the star will observationally be a red giant again and structurally an asymptotic giant branch star.<ref name=Harpaz6/> | |||
==Lifetime== | |||
Helium fusion reactions are extremely temperature sensitive, with reaction rates being proportional to {{nowrap|T<sup>40</sup>}} (under relatively low temperatures).<ref name=Iliadis>{{harvnb|Iliadis|2007|pp=18, 439–42}}</ref> This means that just a 2% rise in temperature more than doubles the reaction rate. The star becomes very unstable—a small rise in temperature leads to a rapid rise in reaction rates, which releases a lot of energy, increasing the temperature further. The helium-burning layer rapidly expands and therefore cools, which reduces the reaction rate again. Huge pulsations build up, which eventually become large enough to throw off the whole stellar atmosphere into space.<ref name="Renzini1987">{{harvnb|Renzini|1987|pp=391–400}}</ref> | |||
] consists of a bright ring, measuring about two light-years across, dotted with dense, bright knots of gas that resemble diamonds in a necklace. The knots glow brightly due to absorption of ultraviolet light from the central stars.<ref>{{cite web|title=Hubble Offers a Dazzling Necklace|url=http://www.spacetelescope.org/images/potw1133a/|work=Picture of the Week|publisher=ESA/Hubble|access-date=18 August 2011}}</ref>]] | |||
After a star passes through the ] (AGB) phase, the short planetary nebula phase of stellar evolution begins<ref name=KwokJun2005 /> as gases blow away from the central star at speeds of a few kilometers per second. The central star is the remnant of its AGB progenitor, an electron-degenerate carbon-oxygen core that has lost most of its hydrogen envelope due to mass loss on the AGB.<ref name=KwokJun2005 /> As the gases expand, the central star undergoes a two-stage evolution, first growing hotter as it continues to contract and hydrogen fusion reactions occur in the shell around the core and then slowly cooling when the hydrogen shell is exhausted through fusion and mass loss.<ref name=KwokJun2005 /> In the second phase, it radiates away its energy and fusion reactions cease, as the central star is not heavy enough to generate the core temperatures required for carbon and oxygen to fuse.<ref name=Kwok1/><ref name=KwokJun2005 /> During the first phase, the central star maintains constant luminosity,<ref name=KwokJun2005 /> while at the same time it grows ever hotter, eventually reaching temperatures around 100,000 K. In the second phase, it cools so much that it does not give off enough ultraviolet radiation to ionize the increasingly distant gas cloud. The star becomes a ], and the expanding gas cloud becomes invisible to us, ending the planetary nebula phase of evolution.<ref name=KwokJun2005 /> For a typical planetary nebula, about 10,000 years<ref name=KwokJun2005 /> passes between its formation and recombination of the resulting ].<ref name=Kwok1/> | |||
The ejected gases form a cloud of material around the now-exposed core of the star. As more and more of the atmosphere moves away from the star, deeper and deeper layers at higher and higher temperatures are exposed. When the exposed surface reaches a temperature of about 30,000 K, there are enough ] ]s being emitted to ] the ejected atmosphere, making it glow. The cloud has then become a planetary nebula.<ref name=Harpaz6/> | |||
==Role in galactic enrichment== | |||
==Lifetime== | |||
] located in the constellation of ] (The Scorpion).<ref>{{cite web|title=An Interstellar Distributor|url=https://esahubble.org/images/potw2104a/|work=Picture of the Week|publisher=ESA/Hubble|access-date=29 January 2020}}</ref>]] | |||
After the ] (AGB) phase, the short planetary nebula phase of stellar evolution begins<ref name=KwokJun2005 /> as gases drift away from the central star at speeds of a few kilometers per second. The central star is the remnant of its AGB progenitor, an electron-degenerate carbon-oxygen core that has lost most of its hydrogen envelope due to mass loss on the AGB.<ref name=KwokJun2005 /> As the gases expand, the central star undergoes a two stage evolution, first growing hotter as it continues to contract and hydrogen fusion reactions occur in the shell around the core and then slowly cooling once the hydrogen shell is exhausted through fusion and mass loss.<ref name=KwokJun2005 /> In the second phase, it radiates away its energy and fusion reactions cease, as the central star is not heavy enough to generate the core temperatures required for carbon and oxygen to fuse.<ref name=KwokJun2005 /><ref name=Kwok1/> During the first phase the central star maintains constant luminosity<ref name=KwokJun2005 /> while, at the same time, it grows ever hotter, eventually reaching temperatures around 100,000K. In the second phase, it eventually cools down so much that it doesn't give off enough ultraviolet radiation to ionize the increasingly distant gas cloud. The star becomes a ], and the gas cloud ], becoming invisible, ending the planetary nebula phase of evolution.<ref name=KwokJun2005 /> For a typical planetary nebula, about 10,000 years<ref name=KwokJun2005 /> passes between its formation and recombination of the star.<ref name=Kwok1/> | |||
Planetary nebulae may play a very important role in galactic evolution. Newly born stars consist almost entirely of ] and ],<ref>{{cite web| author=W. Sutherland| url=http://www.maths.qmul.ac.uk/~wjs/MTH726U/chap4.pdf| title=The Galaxy. Chapter 4. Galactic Chemical Evolution| date=26 March 2013| access-date=13 January 2015}}{{dead link|date=January 2018 |bot=InternetArchiveBot |fix-attempted=yes }}</ref> but as stars evolve through the ] phase,<ref>{{Cite journal | last1 = Sackmann | first1 = I. -J. | last2 = Boothroyd | first2 = A. I. | last3 = Kraemer | first3 = K. E. | title = Our Sun. III. Present and Future | doi = 10.1086/173407 | journal = The Astrophysical Journal | volume = 418 | pages = 457 | year = 1993 |bibcode = 1993ApJ...418..457S | doi-access = free }}</ref> they create heavier elements via ] which are eventually expelled by strong ]s.<ref>{{cite journal| bibcode=1975ApJ...200L.107C |last1= Castor|first1=J. |last2=McCray|first2=R. |last3=Weaver|first3=R. | title=Interstellar Bubbles| date=1975| journal=Astrophysical Journal Letters| volume=200| pages=L107–L110| doi=10.1086/181908| doi-access=free}}</ref> Planetary nebulae usually contain larger proportions of elements such as ], ] and ], and these are recycled into the interstellar medium via these powerful winds. In this way, planetary nebulae greatly enrich the ] and their ]e with these heavier elements – collectively known by astronomers as ''metals'' and specifically referred to by the ] ''Z''.<ref name=Kwok19>{{harvnb|Kwok|2000|pp=199–207}}</ref> | |||
==Galactic recyclers== | |||
Planetary nebulae play a very important role in galactic evolution. The early ] consisted almost entirely of hydrogen and helium, but stars create heavier elements via nuclear fusion. The gases of planetary nebulae thus contain a large proportion of elements such as ], nitrogen and oxygen, and as they expand and merge into the interstellar medium, they enrich it with these heavy elements, collectively known as ''metals'' by astronomers.<ref name=Kwok19>{{harvnb|Kwok|2000|pp=199–207}}</ref> | |||
Subsequent generations of stars |
Subsequent generations of stars formed from such nebulae also tend to have higher metallicities. Although these metals are present in stars in relatively tiny amounts, they have marked effects on ] and fusion reactions. When stars formed earlier in the ] they theoretically contained smaller quantities of heavier elements.<ref name=PopIII>{{cite journal|last=Pan|first=Liubin|author2=Scannapieco, Evan|author3= Scalo, Jon|s2cid=119233184|title=Modeling the Pollution of Pristine Gas in the Early Universe|journal=The Astrophysical Journal|date=1 October 2013|volume=775|issue=2|page=111|doi=10.1088/0004-637X/775/2/111|arxiv = 1306.4663 |bibcode = 2013ApJ...775..111P }}</ref> Known examples are the metal poor ] stars. (See ].)<ref name=Marochnik>{{harvnb|Marochnik|Shukurov|Yastrzhembsky|1996|pp=6–10}}</ref><ref name=Gregory>{{cite book|last2=Gregory|first2=Stephen A. |first1=Michael |last1=Zeilik|title=Introductory astronomy & astrophysics|date=1998|publisher=Saunders College Publishing|location=Fort Worth |isbn=0-03-006228-4|page=322|edition=4.}}</ref> Identification of stellar metallicity content is found by ]. | ||
==Characteristics== | ==Characteristics== | ||
===Physical characteristics=== | ===Physical characteristics=== | ||
] |
]]] | ||
] (IC 3568)]] | |||
A typical planetary nebula is roughly one ] across, and consists of extremely rarefied gas, with a density generally from 100 to 10,000 particles {{nowrap|per cm<sup>3</sup>}}.<ref name=Osterbrock1>{{harvnb|Osterbrock|Ferland|2005|p=10}}</ref> (The Earth's atmosphere, by comparison, contains 2.5{{e|19}} particles {{nowrap|per cm<sup>3</sup>}}.) Young planetary nebulae have the highest densities, sometimes as high as 10<sup>6</sup> particles {{nowrap|per cm<sup>3</sup>}}. As nebulae age, their expansion causes their density to decrease. The masses of planetary nebulae range from 0.1 to 1 ]es.<ref name=Osterbrock1/> | A typical planetary nebula is roughly one ] across, and consists of extremely rarefied gas, with a density generally from 100 to 10,000 particles {{nowrap|per cm<sup>3</sup>}}.<ref name=Osterbrock1>{{harvnb|Osterbrock|Ferland|2005|p=10}}</ref> (The Earth's atmosphere, by comparison, contains 2.5{{e|19}} particles {{nowrap|per cm<sup>3</sup>}}.) Young planetary nebulae have the highest densities, sometimes as high as 10<sup>6</sup> particles {{nowrap|per cm<sup>3</sup>}}. As nebulae age, their expansion causes their density to decrease. The masses of planetary nebulae range from 0.1 to 1 ]es.<ref name=Osterbrock1/> | ||
Radiation from the central star heats the gases to temperatures of about 10,000 ].<ref name=Gurzadyan2>{{harvnb|Gurzadyan|1997|p=238}}</ref> The gas temperature in central regions is usually much |
Radiation from the central star heats the gases to temperatures of about 10,000 ].<ref name=Gurzadyan2>{{harvnb|Gurzadyan|1997|p=238}}</ref> The gas temperature in central regions is usually much higher than at the periphery reaching 16,000–25,000 K.<ref name=Gurzadyan3>{{harvnb|Gurzadyan|1997|pp=130–7}}</ref> The volume in the vicinity of the central star is often filled with a very hot (coronal) gas having the temperature of about 1,000,000 K. This gas originates from the surface of the central star in the form of the fast stellar wind.<ref name=Osterbrock261>{{harvnb|Osterbrock|Ferland|2005|pp=261–2}}</ref> | ||
Nebulae may be described as ''matter bounded'' or ''radiation bounded''. In the former case, there is not enough matter in the nebula to absorb all the UV photons emitted by the star, and the visible nebula is fully ionized. In the latter case, there are not enough UV photons being emitted by the central star to ionize all the surrounding gas, and an ionization front propagates outward into the circumstellar neutral |
Nebulae may be described as ''matter bounded'' or ''radiation bounded''. In the former case, there is not enough matter in the nebula to absorb all the UV photons emitted by the star, and the visible nebula is fully ionized. In the latter case, there are not enough UV photons being emitted by the central star to ionize all the surrounding gas, and an ionization front propagates outward into the circumstellar envelope of neutral atoms.<ref name=Osterbrock2>{{harvnb|Osterbrock|Ferland|2005|p=207}}</ref> | ||
===Numbers and distribution=== | ===Numbers and distribution=== | ||
About 3000 planetary nebulae are now known to exist in our galaxy,<ref name="Parkeretal2006">{{harvnb|Parker|Acker|Frew|Hartley|2006|pp= |
About 3000 planetary nebulae are now known to exist in our galaxy,<ref name="Parkeretal2006">{{harvnb|Parker|Acker|Frew|Hartley|2006|pp=79–94}}</ref> out of 200 billion stars. Their very short lifetime compared to total stellar lifetime accounts for their rarity. They are found mostly near the plane of the ], with the greatest concentration near the ].<ref name=majaess2007>{{harvnb|Majaess|Turner|Lane|2007|pp=1349–60}}</ref> | ||
===Morphology=== | ===Morphology=== | ||
] can control the creation of the spectacular jets of material ejected from the object.]] | |||
Only about 20% of planetary nebulae are spherically symmetric (for example, see ]).<ref name=Jacoby2001>{{harvnb|Jacoby|Ferland|Korista|2001|pp= |
Only about 20% of planetary nebulae are spherically symmetric (for example, see ]).<ref name=Jacoby2001>{{harvnb|Jacoby|Ferland|Korista|2001|pp=272–86}}</ref> A wide variety of shapes exist with some very complex forms seen. Planetary nebulae are classified by different authors into: stellar, disk, ring, irregular, helical, ], quadrupolar,<ref name=KwoketalDec2005>{{harvnb|Kwok|Su|2005|pp=L49–52}}</ref> and other types,<ref name=Kwok8>{{harvnb|Kwok|2000|pp=89–96}}</ref> although the majority of them belong to just three types: spherical, elliptical and bipolar. Bipolar nebulae are concentrated in the ], probably produced by relatively young massive progenitor stars; and bipolars in the ] appear to prefer orienting their orbital axes parallel to the galactic plane.<ref>{{harvnb|Rees|Zijlstra|2013}}</ref> On the other hand, spherical nebulae are probably produced by old stars similar to the Sun.<ref name=Osterbrock/> | ||
The huge variety of the shapes is partially the projection effect—the same nebula when viewed under different angles will |
The huge variety of the shapes is partially the projection effect—the same nebula when viewed under different angles will appear different.<ref>{{cite journal | first = Z | last = Chen |author2=A. Frank|author3=E. G. Blackman|author4=J. Nordhaus|author5=J. Carroll-Nellenback| s2cid = 119073723 | title = Mass Transfer and Disc Formation in AGB Binary Systems| journal = Monthly Notices of the Royal Astronomical Society | volume = 468 | issue = 4 | pages = 4465 | date = 2017 | doi = 10.1093/mnras/stx680 | doi-access = free |arxiv = 1702.06160 |bibcode = 2017MNRAS.468.4465C }}</ref> Nevertheless, the reason for the huge variety of physical shapes is not fully understood.<ref name=Kwok8/> Gravitational interactions with companion stars if the central stars are ]s may be one cause. Another possibility is that planets disrupt the flow of material away from the star as the nebula forms. It has been determined that the more massive stars produce more irregularly shaped nebulae.<ref name=Morris>{{harvnb|Morris|1990|pp=526–30}}</ref> In January 2005, astronomers announced the first detection of magnetic fields around the central stars of two planetary nebulae, and hypothesized that the fields might be partly or wholly responsible for their remarkable shapes.<ref>{{harvnb|SpaceDaily Express|2005}}</ref><ref name="Jordanetal2005" /> | ||
==Membership in clusters== | ==Membership in clusters== | ||
] | |||
Planetary nebulae have been detected as members in four ]: ], ], ] and ]. However, there has yet to be an established case of a planetary nebula discovered in an ] as based on a consistent set of distances, reddenings, and radial velocities.<ref name=majaess2007/> The cases of NGC 2348 in ], and ] in the respective open cluster that is designated by the same name, are often cited as ''bona fide'' instances, however, they are instead line-of-sight coincidences granted the radial velocities between the clusters and planetary nebulae are discrepant.<ref name=majaess2007/><ref name=kiss2008>{{harvnb|Kiss|Szabó|Balog|Parker|2008|pp=399–404}}</ref><ref name=mermilliod2001>{{harvnb|Mermilliod|Clariá|Andersen|Piatti|2001|pp=30–9}}</ref> | |||
Planetary nebulae have been detected as members in four Galactic ]: ], ], ] and ]. Evidence also points to the potential discovery of planetary nebulae in globular clusters in the galaxy ].<ref name=ja2013>Jacoby, George H.; Ciardullo, Robin; ]; Lee, Myung Gyoon; Herrmann, Kimberly A.; Hwang, Ho Seong; Kaplan, Evan; Davies, James E., (2013). , ApJ, 769, 1</ref> However, there is currently only one case of a planetary nebula discovered in an ] that is agreed upon by independent researchers.<ref name=fr2008>Frew, David J. (2008). , PhD Thesis, Department of Physics, Macquarie University, Sydney, Australia</ref><ref name=parker2011>{{harvnb|Parker|2011|pp=1835–1844}}</ref><ref name=ma2014>Majaess, D.; Carraro, G.; Moni Bidin, C.; Bonatto, C.; Turner, D.; Moyano, M.; Berdnikov, L.; Giorgi, E., (2014). , A&A, 567</ref> That case pertains to the planetary nebula PHR 1315-6555 and the open cluster Andrews-Lindsay 1. Indeed, through cluster membership, PHR 1315-6555 possesses among the most precise distances established for a planetary nebula (i.e., a 4% distance solution). The cases of ] and NGC 2348 in ], exhibit mismatched velocities between the planetary nebulae and the clusters, which indicates they are line-of-sight coincidences.<ref name=majaess2007/><ref name=kiss2008>{{harvnb|Kiss|Szabó|Balog|Parker|2008|pp=399–404}}</ref><ref name=mermilliod2001>{{harvnb|Mermilliod|Clariá|Andersen|Piatti|2001|pp=30–9}}</ref> A subsample of ''tentative'' cases that may potentially be cluster/PN pairs includes Abell 8 and Bica 6,<ref name=bo2008>Bonatto, C.; Bica, E.; Santos, J. F. C., (2008). , MNRAS, 386, 1</ref><ref name=tu2011>Turner, D. G.; Rosvick, J. M.; Balam, D. D.; Henden, A. A.; Majaess, D. J.; Lane, D. J. (2011). , PASP, 123, 909</ref> and He 2-86 and NGC 4463.<ref name=mo2014>Moni Bidin, C.; Majaess, D.; Bonatto, C.; Mauro, F.; Turner, D.; Geisler, D.; Chené, A.-N.; Gormaz-Matamala, A. C.; Borissova, J.; Kurtev, R. G.; Minniti, D.; Carraro, G.; Gieren, W. (2014). , A&A, 561</ref> | |||
Partly because of their small total mass, open clusters have relatively poor gravitational cohesion. Consequently, open clusters tend to disperse after a relatively short time, typically from 100 to 600 million years, because of external gravitational influences amid other factors. Under exceptional conditions, open clusters can remain intact for up to one billion years or more.<ref name=Allison>{{harvnb|Allison|2006|pp=56–8}}</ref> | |||
Theoretical models predict that planetary nebulae can form from ] stars of between |
Theoretical models predict that planetary nebulae can form from ] stars of between one and eight solar masses, which puts the progenitor star's age at greater than 40 million years. Although there are a few hundred known open clusters within that age range, a variety of reasons limit the chances of finding a planetary nebula within.<ref name=majaess2007/> For one reason, the planetary nebula phase for more massive stars is on the order of millennia, which is a blink of the eye in astronomic terms. Also, partly because of their small total mass, open clusters have relatively poor gravitational cohesion and tend to disperse after a relatively short time, typically from 100 to 600 million years.<ref name=Allison>{{harvnb|Allison|2006|pp=56–8}}</ref> | ||
==Current issues in planetary nebula studies== | ==Current issues in planetary nebula studies== | ||
A long standing problem in the study of planetary nebulae is that in most cases, their distances are very poorly determined. For a very few nearby planetary nebulae, it is possible to determine distances by measuring their expansion ] high resolution observations taken several years apart will show the expansion of the nebula perpendicular to the line of sight, while spectroscopic observations of the ] will reveal the velocity of expansion in the line of sight. Comparing the angular expansion with the derived velocity of expansion will reveal the distance to the nebula.<ref name=Reed1999/> | |||
The distances to planetary nebulae are generally poorly determined,<ref>{{cite news|title=Distances to Planetary Nebulae|author=R. Gathier|url= https://www.eso.org/sci/publications/messenger/archive/no.32-jun83/messenger-no32-20-22.pdf |archive-url=https://ghostarchive.org/archive/20221009/https://www.eso.org/sci/publications/messenger/archive/no.32-jun83/messenger-no32-20-22.pdf |archive-date=2022-10-09 |url-status=live |access-date=31 May 2014|newspaper=ESO Messenger}}</ref> but the '']'' mission is now measuring direct ] between their central stars and neighboring stars.<ref>{{Cite web|url=http://simbad.u-strasbg.fr/simbad/sim-ref?bibcode=2018yCat.1345....0G|title=SIMBAD references}}</ref> It is also possible to determine distances to nearby planetary nebula by measuring their expansion rates. High resolution observations taken several years apart will show the expansion of the nebula perpendicular to the line of sight, while spectroscopic observations of the ] will reveal the velocity of expansion in the line of sight. Comparing the angular expansion with the derived velocity of expansion will reveal the distance to the nebula.<ref name=Reed1999/> | |||
The issue of how such a diverse range of nebular shapes can be produced is a controversial topic. Broadly, it is believed that interactions between material moving away from the star at different speeds gives rise to most shapes observed.<ref name=Kwok8/> However, some astronomers believe that double central stars must be responsible for at least the more complex and extreme planetary nebulae.<ref name="Soker2002">{{harvnb|Soker|2002|pp=481–6}}</ref> One recent study has found that several planetary nebulae contain strong magnetic fields, something which has been hypothesized by Grigor Gurzadyan already in the 1960s.<ref name=Gurzadyan4>{{harvnb|Gurzadyan|1997|p=424}}</ref> Magnetic interactions with ionized gas could be responsible for shaping at least some planetary nebulae.<ref name="Jordanetal2005">{{harvnb|Jordan|Werner|O'Toole|2005|pp=273–9}}</ref> | |||
The issue of how such a diverse range of nebular shapes can be produced is a debatable topic. It is theorised that interactions between material moving away from the star at different speeds gives rise to most observed shapes.<ref name=Kwok8/> However, some astronomers postulate that close binary central stars might be responsible for the more complex and extreme planetary nebulae.<ref name="Soker2002">{{harvnb|Soker|2002|pp=481–6}}</ref> Several have been shown to exhibit strong magnetic fields,<ref name=Gurzadyan4>{{harvnb|Gurzadyan|1997|p=424}}</ref> and their interactions with ionized gas could explain some planetary nebulae shapes.<ref name="Jordanetal2005">{{harvnb|Jordan|Werner|O'Toole|2005|pp=273–9}}</ref> | |||
There are two different ways of determining metal abundances in nebulae, which rely on different types of spectral lines—recombination lines and collisionally excited lines, and large discrepancies are sometimes seen between the results derived from the two methods. Some astronomers put this down to the presence of small temperature fluctuations within planetary nebulae; others claim that the discrepancies are too large to be explained by temperature effects, and hypothesize the existence of cold knots containing very little hydrogen to explain the observations. However, no such knots have yet been observed.<ref name="Liuetal2000">{{harvnb|Liu|Storey|Barlow|Danziger|2000|pp=585–587}}</ref> | |||
There are two main methods of determining ] in nebulae. These rely on recombination lines and collisionally excited lines. Large discrepancies are sometimes seen between the results derived from the two methods. This may be explained by the presence of small temperature fluctuations within planetary nebulae. The discrepancies may be too large to be caused by temperature effects, and some hypothesize the existence of cold knots containing very little hydrogen to explain the observations. However, such knots have yet to be observed.<ref name="Liuetal2000">{{harvnb|Liu|Storey|Barlow|Danziger|2000|pp=585–587}}</ref> | |||
==See also== | ==See also== | ||
{{Multicol}} | |||
'''Preceding evolutionary stage:''' | |||
* ] | * ] | ||
* ] | |||
'''Subsequent evolutionary stage:''' | |||
* ] (''predegenerates'') | |||
* ] | |||
{{Multicol-break}} | |||
'''General topics:''' | |||
* ] | |||
'''Otherwise related:''' | |||
* ] | * ] | ||
* ] | |||
'''Alternative developments:''' | |||
* ] | * ] | ||
* ] (''predegenerates'') | |||
* ] | |||
* ] | * ] | ||
* ] | |||
{{Multicol-end}} | |||
* ] | |||
==References== | == References == | ||
=== Citations === | |||
{{reflist|colwidth=25em}} | |||
{{Reflist}} | |||
==Cited sources== | === Cited sources === | ||
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| year = 2007 | |||
| pages = 18, 439–42 | |||
| isbn = 978-3-527-40602-9 | |||
}} | |||
* {{citation | * {{citation | ||
| last1 = Jacoby | | last1 = Jacoby | ||
Line 250: | Line 316: | ||
| last3 = Korista | | last3 = Korista | ||
| first3 = Kirk T. | | first3 = Kirk T. | ||
| authorlink = | |||
| journal = The Astrophysical Journal | | journal = The Astrophysical Journal | ||
| volume = 560 | | volume = 560 | ||
| issue = 1 | | issue = 1 | ||
| pages = |
| pages = 272–86 | ||
| title = The Planetary Nebula A39: An Observational Benchmark for Numerical Modeling of Photoionized Plasmas | | title = The Planetary Nebula A39: An Observational Benchmark for Numerical Modeling of Photoionized Plasmas | ||
| |
| date = 2001 | ||
| doi = 10.1086/322489 | | doi = 10.1086/322489 | ||
| |
| bibcode = 2001ApJ...560..272J | ||
| url = http://uknowledge.uky.edu/cgi/viewcontent.cgi?article=1104&context=physastron_facpub | |||
}} | |||
| doi-access = free | |||
}} | |||
* {{citation | * {{citation | ||
| year = 2005 | |||
| date = March 2005 | | date = March 2005 | ||
| |
| bibcode = 2005A&A...432..273J | ||
| last1 = Jordan | | last1 = Jordan | ||
| first1 S. | |||
| last2 = Werner | | last2 = Werner | ||
| first2 = K. | | first2 = K. | ||
Line 274: | Line 339: | ||
| volume = 432 | | volume = 432 | ||
| issue = 1 | | issue = 1 | ||
| pages = |
| pages = 273–9 | ||
| doi = 10.1051/0004-6361:20041993 | | doi = 10.1051/0004-6361:20041993 | ||
| first1 = S. | |||
}} | |||
| s2cid = 119361869 | |||
|arxiv = astro-ph/0501040 }} | |||
* {{citation | * {{citation | ||
| year = 2008 | |||
| date = November 2008 | | date = November 2008 | ||
| |
| bibcode = 2008MNRAS.391..399K | ||
| last1 = Kiss | | last1 = Kiss | ||
| first1 = L. L. | | first1 = L. L. | ||
Line 291: | Line 357: | ||
| last5 = Frew | | last5 = Frew | ||
| first5 = D. J. | | first5 = D. J. | ||
| s2cid = 15207860 | |||
| title =AAOmega radial velocities rule out current membership of the planetary nebula NGC 2438 in the open cluster M46 | | title =AAOmega radial velocities rule out current membership of the planetary nebula NGC 2438 in the open cluster M46 | ||
| journal = Monthly Notices of the Royal Astronomical Society | | journal = ] | ||
| volume = 391 | | volume = 391 | ||
| issue = 1 | | issue = 1 | ||
| pages = |
| pages = 399–404 | ||
| doi = 10.1111/j.1365-2966.2008.13899.x | | doi = 10.1111/j.1365-2966.2008.13899.x | ||
| doi-access = free | |||
}} | |||
|arxiv = 0809.0327 }} | |||
* {{citation | * {{citation | ||
| url = |
| url = https://books.google.com/books?id=gDSsAAAAIAAJ | ||
| title = Astronomy | | title = Astronomy | ||
| last1 = Krause | | last1 = Krause | ||
| first1 = Arthur | | first1 = Arthur | ||
| |
| date = 1961 | ||
| publisher = Oliver and Boyd | | publisher = Oliver and Boyd | ||
| page = 187 | | page = 187 | ||
}} | }} | ||
* {{citation | * {{citation | ||
| last = Kwok | | last = Kwok | ||
| first = Sun | | first = Sun | ||
| title = The origin and evolution of planetary nebulae | | title = The origin and evolution of planetary nebulae | ||
| |
| date = 2000 | ||
| publisher = Cambridge University Press | | publisher = Cambridge University Press | ||
| isbn = |
| isbn = 0-521-62313-8 | ||
| url = |
| url = https://books.google.com/books?id=7NfqpZxO_o0C | ||
| archive-url = https://web.archive.org/web/20120302015504/http://books.google.com/books?id=7NfqpZxO_o0C | |||
}} (Chapter 1 can be downloaded .) | |||
| url-status = dead | |||
| archive-date = March 2, 2012 | |||
}} (Chapter 1 can be downloaded .) | |||
* {{citation | * {{citation | ||
| |
| doi = 10.5303/JKAS.2005.38.2.271 | ||
| bibcode = 2005JKAS...38..271K | |||
| title = Planetary Nebulae: New Challenges in the 21st Century | | title = Planetary Nebulae: New Challenges in the 21st Century | ||
| last1 = Kwok | | last1 = Kwok | ||
| first1 = Sun | | first1 = Sun | ||
| author1-link = Sun Kwok | | author1-link = Sun Kwok | ||
| year = 2005 | |||
| date = June 2005 | | date = June 2005 | ||
| journal = Journal of the Korean Astronomical Society | | journal = Journal of the Korean Astronomical Society | ||
| volume = 38 | | volume = 38 | ||
| issue = 2 | | issue = 2 | ||
| pages = |
| pages = 271–8 | ||
| |
| doi-access = free | ||
}} | }} | ||
* {{citation | * {{citation | ||
| |
| bibcode = 2005ApJ...635L..49K | ||
| last1 = Kwok | | last1 = Kwok | ||
| first1 = Sun | | first1 = Sun | ||
| last2 = Su | | last2 = Su | ||
| first2 = Kate Y. L. | | first2 = Kate Y. L. | ||
| year = 2005 | |||
| date = December 2005 | | date = December 2005 | ||
| title = Discovery of Multiple Coaxial Rings in the Quadrupolar Planetary Nebula NGC 6881 | | title = Discovery of Multiple Coaxial Rings in the Quadrupolar Planetary Nebula NGC 6881 | ||
Line 342: | Line 412: | ||
| volume = 635 | | volume = 635 | ||
| issue = 1 | | issue = 1 | ||
| pages = |
| pages = L49–52 | ||
| doi = 10.1086/499332 | | doi = 10.1086/499332 | ||
| quote = We report the discovery of multiple two-dimensional rings in the quadrupolar planetary nebula NGC 6881. |
| quote = We report the discovery of multiple two-dimensional rings in the quadrupolar planetary nebula NGC 6881. As many as four pairs of rings are seen in the bipolar lobes, and three rings are seen in the central torus. While the rings in the lobes have the same axis as one pair of the bipolar lobes, the inner rings are aligned with the other pair. The two pairs of bipolar lobes are likely to be carved out by two separate high-velocity outflows from the circumstellar material left over from the asymptotic giant branch (AGB) wind. The two-dimensional rings could be the results of dynamical instabilities or the consequence of a fast outflow interacting with remnants of discrete AGB circumstellar shells. | ||
| doi-access = free | |||
}} | |||
}} | |||
* {{citation | * {{citation | ||
| |
| bibcode = 2006IAUS..234..445K | ||
| title = Planetary nebulae in the GLIMPSE survey | | title = Planetary nebulae in the GLIMPSE survey | ||
| last1 = Kwok | | last1 = Kwok | ||
Line 357: | Line 428: | ||
| last4 = Churchwell | | last4 = Churchwell | ||
| first4 = Edward | | first4 = Edward | ||
| |
| date = 2006 | ||
| series = Planetary Nebulae in our Galaxy and Beyond | | series = Planetary Nebulae in our Galaxy and Beyond | ||
| editor1-last = Barlow | |||
| jornal = Proceedings of the International Astronomical Union, Symposium #234 | |||
| |
| editor1-first = M. J. | ||
| |
| editor2-last = Méndez | ||
| |
| editor2-first = R. H. | ||
| editor-last2 = Méndez | |||
| place = Cambridge | | place = Cambridge | ||
| publisher = Cambridge University Press | | publisher = Cambridge University Press | ||
| pages = |
| pages = 445–6 | ||
| doi = 10.1017/S1743921306003668 | | doi = 10.1017/S1743921306003668 | ||
| quote = Planetary nebulae (PNs) have high dust content and radiate strongly in the infrared. |
| quote = Planetary nebulae (PNs) have high dust content and radiate strongly in the infrared. For young PNs, the dust component accounts for about one third of the total energy output of the nebulae (Zhang & Kwok 1991). The typical color temperatures of PNs are between 100 and 200 K, and at λ >5 μm, dust begins to dominate over bound-free emission from the ionized component. Although PNs are traditionally discovered through examination of photographic plates or Hα surveys, PNs can also be identified in infrared surveys by searching for red objects with a rising spectrum between 4–10 μm. | ||
| issue = S234 | |||
}} | |||
| journal = Proceedings of the International Astronomical Union | |||
| volume = 2 | |||
| doi-broken-date = 1 November 2024 | |||
| doi-access = free | |||
}} | |||
* {{citation | * {{citation | ||
| |
| bibcode = 2000MNRAS.312..585L | ||
| year = 2000 | |||
| date = March 2000 | | date = March 2000 | ||
| last1 = Liu | | last1 = Liu | ||
Line 390: | Line 464: | ||
| volume = 312 | | volume = 312 | ||
| issue = 3 | | issue = 3 | ||
| pages = |
| pages = 585–628 | ||
| doi = 10.1046/j.1365-8711.2000.03167.x | | doi = 10.1046/j.1365-8711.2000.03167.x | ||
| doi-access = free | |||
}} | |||
}} | |||
* {{citation | * {{citation | ||
| |
| bibcode = 2009RMxAA..45..127M | ||
| title = Planetary nebulae and the chemical evolution of the Magellanic Clouds | | title = Planetary nebulae and the chemical evolution of the Magellanic Clouds | ||
| last1 = Maciel | | last1 = Maciel | ||
Line 402: | Line 477: | ||
| last3 = Idiart | | last3 = Idiart | ||
| first3 = T. E. P. | | first3 = T. E. P. | ||
| year = 2009 | |||
| date = October 2009 | | date = October 2009 | ||
| journal = Revista Mexicana de Astronomía y Astrofísica | | journal = Revista Mexicana de Astronomía y Astrofísica | ||
| volume = 45 | | volume = 45 | ||
| pages = |
| pages = 127–37 | ||
| quote = These objects are produced by low and intermediate mass stars, with main sequence masses roughly between 0.8 and 8 M<sub>⊙</sub>, and present a reasonably large age and metallicity spread. | | quote = These objects are produced by low and intermediate mass stars, with main sequence masses roughly between 0.8 and 8 M<sub>⊙</sub>, and present a reasonably large age and metallicity spread. | ||
|arxiv = 0904.2549}} | |||
}} | |||
* {{citation | * {{citation | ||
| last1 = Majaess | | last1 = Majaess | ||
Line 416: | Line 490: | ||
| last3 = Lane | | last3 = Lane | ||
| first3 = D. | | first3 = D. | ||
| |
| s2cid = 18640979 | ||
| date = December 2007 | | date = December 2007 | ||
| |
| bibcode = 2007PASP..119.1349M | ||
| title = In Search of Possible Associations between Planetary Nebulae and Open Clusters | | title = In Search of Possible Associations between Planetary Nebulae and Open Clusters | ||
| journal = Publications of the Astronomical Society of the Pacific | | journal = Publications of the Astronomical Society of the Pacific | ||
| volume = 119 | | volume = 119 | ||
| issue = 862 | | issue = 862 | ||
| pages = |
| pages = 1349–60 | ||
| doi = 10.1086/524414 | | doi = 10.1086/524414 | ||
|arxiv = 0710.2900 }} | |||
}} | |||
* {{citation | * {{citation | ||
| chapter = Chapter 19: Chemical abundances | |||
| last1 = Marochnik | | last1 = Marochnik | ||
| first1 = L.S. | | first1 = L.S. | ||
Line 434: | Line 509: | ||
| first3 = Igor | | first3 = Igor | ||
| title = The Milky Way galaxy | | title = The Milky Way galaxy | ||
| date = 1996 | |||
| chapter = Chapter 19: Chemical abundances | |||
| year = 1996 | |||
| chapter = Chapter 1: Introduction | |||
| publisher = Taylor & Francis | | publisher = Taylor & Francis | ||
| pages = |
| pages = 6–10 | ||
| isbn = |
| isbn = 978-2-88124-931-0 | ||
| url = |
| url = https://books.google.com/books?id=uRgWHDGpKZIC | ||
}} | }} | ||
* {{citation | * {{citation | ||
| last1 = Mermilliod | | last1 = Mermilliod | ||
Line 453: | Line 526: | ||
| last5 = Mayor | | last5 = Mayor | ||
| first5 = M. | | first5 = M. | ||
| year = 2001 | |||
| date = August 2001 | | date = August 2001 | ||
| |
| bibcode = 2001A&A...375...30M | ||
| title = Red giants in open clusters. IX. NGC 2324, 2818, 3960 and 6259 | | title = Red giants in open clusters. IX. NGC 2324, 2818, 3960 and 6259 | ||
| journal = Astronomy and Astrophysics | | journal = Astronomy and Astrophysics | ||
| volume = 375 | | volume = 375 | ||
| |
| issue = 1 | ||
| pages = 30–9 | |||
| doi = 10.1051/0004-6361:20010845 | | doi = 10.1051/0004-6361:20010845 | ||
| citeseerx = 10.1.1.30.7545 | |||
}} | |||
| s2cid = 122773065 | |||
}} | |||
* {{citation | |||
| last1 = Miszalski | |||
| first1 = B. | |||
| last2 = Jones | |||
| first2 = D. | |||
| last3 = Rodríguez-Gil | |||
| first3 = P. | |||
| last4 = Boffin | |||
| first4 = H. M. J. | |||
| last5 = Corradi | |||
| first5 = R. L. M. | |||
| last6 = Santander-García | |||
| first6 = M. | |||
| s2cid = 15010950 | |||
| title = Discovery of close binary central stars in the planetary nebulae NGC 6326 and NGC 6778 | |||
| journal = Astronomy and Astrophysics | |||
| date = 2011 | |||
| volume = 531 | |||
| pages = A158 | |||
| bibcode = 2011A&A...531A.158M | |||
| doi = 10.1051/0004-6361/201117084|arxiv = 1105.5731 }} | |||
* {{citation | * {{citation | ||
| last1 = Moore | | last1 = Moore | ||
Line 467: | Line 563: | ||
| title = Observing the Cat's Eye Nebula | | title = Observing the Cat's Eye Nebula | ||
| journal = Journal of the British Astronomical Association | | journal = Journal of the British Astronomical Association | ||
| year = 2007 | |||
| date = October 2007 | | date = October 2007 | ||
| volume = 117 | | volume = 117 | ||
| issue = 5 | | issue = 5 | ||
| pages = |
| pages = 279–80 | ||
| |
| bibcode = 2007JBAA..117R.279M | ||
}} | }} | ||
* {{citation | * {{citation | ||
Line 479: | Line 574: | ||
| title = From Miras to planetary nebulae: which path for stellar evolution? | | title = From Miras to planetary nebulae: which path for stellar evolution? | ||
| chapter = Bipolar asymmetry in the mass outflows of stars in transition | | chapter = Bipolar asymmetry in the mass outflows of stars in transition | ||
| |
| date = 1990 | ||
| publisher = Atlantica Séguier Frontières | | publisher = Atlantica Séguier Frontières | ||
| location = Montpellier, France, September |
| location = Montpellier, France, September 4–7, 1989 IAP astrophysics meeting | ||
| pages = |
| pages = 526–30 | ||
| isbn = |
| isbn = 978-2-86332-077-8 | ||
| |
| editor = Mennessier, M.O. | ||
| editor2 = Omont, Alain | |||
| url = |
| url = https://books.google.com/books?id=qTZld_-Y5qYC | ||
}} | }} | ||
* {{citation | * {{citation | ||
| title=Astrophysics of gaseous nebulae and active galactic nuclei | | title = Astrophysics of gaseous nebulae and active galactic nuclei | ||
| |
| last1 = Osterbrock | ||
| |
| first1 = Donald E. | ||
| last2 = Ferland | | last2 = Ferland | ||
| first2 = G. J. | | first2 = G. J. | ||
| editor = Ferland, G. J. | | editor = Ferland, G. J. | ||
| publisher = University Science Books | | publisher = University Science Books | ||
| |
| date = 2005 | ||
| isbn = |
| isbn = 978-1-891389-34-4 | ||
| url-access = registration | |||
}} | |||
| url = https://archive.org/details/astrophysicsofga0000oste | |||
|ref=none | |||
}} | |||
* {{citation | * {{citation | ||
| last1 = Parker | | last1 = Parker | ||
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| first4 = M. | | first4 = M. | ||
| last5 = Peyaud | | last5 = Peyaud | ||
| first5 = |
| first5 = A. E. J. | ||
| last6 = Ochsenbein | | last6 = Ochsenbein | ||
| first6 = F. | | first6 = F. | ||
Line 531: | Line 631: | ||
| last16 = Vaughan | | last16 = Vaughan | ||
| first16 = A. E. | | first16 = A. E. | ||
| year = 2006 | |||
| date = November 2006 | | date = November 2006 | ||
| title = The Macquarie/AAO/Strasbourg Hα Planetary Nebula Catalogue: MASH | | title = The Macquarie/AAO/Strasbourg Hα Planetary Nebula Catalogue: MASH | ||
| |
| bibcode = 2006MNRAS.373...79P | ||
| journal = Monthly Notices of the Royal Astronomical Society | | journal = Monthly Notices of the Royal Astronomical Society | ||
| volume = 373 | | volume = 373 | ||
| issue = 1 | | issue = 1 | ||
| pages = |
| pages = 79–94 | ||
| doi = 10.1111/j.1365-2966.2006.10950.x | | doi = 10.1111/j.1365-2966.2006.10950.x | ||
| doi-access = free | |||
}} | |||
}} | |||
* {{citation | |||
| last1 = Parker | |||
| first1 = Quentin A. | |||
| last2 = Frew | |||
| first2 = David J. | |||
| last3 = Miszalski | |||
| first3 = B. | |||
| last4 = Kovacevic | |||
| first4 = Anna V. | |||
| last5 = Frinchaboy | |||
| first5 = Peter. | |||
| last6 = Dobbie | |||
| first6 = Paul D. | |||
| last7 = Köppen | |||
| first7 = J. | |||
| s2cid = 16164749 | |||
| date = May 2011 | |||
| title = PHR 1315–6555: A bipolar planetary nebula in the compact Hyades-age open cluster ESO 96-SC04 | |||
| bibcode = 2011MNRAS.413.1835P | |||
| journal = Monthly Notices of the Royal Astronomical Society | |||
| volume = 413 | |||
| issue = 3 | |||
| pages = 1835–1844 | |||
| doi = 10.1111/j.1365-2966.2011.18259.x | |||
| doi-access = free | |||
| ref = {{Harvid|Parker|2011}} | |||
|arxiv = 1101.3814 }} | |||
* {{citation | * {{citation | ||
| last1 = Reed | | last1 = Reed | ||
Line 558: | Line 685: | ||
| last8 = Terzian | | last8 = Terzian | ||
| first8 = Yervant | | first8 = Yervant | ||
| s2cid = 14746840 | |||
| title = Hubble Space Telescope Measurements of the Expansion of NGC 6543: Parallax Distance and Nebular Evolution | | title = Hubble Space Telescope Measurements of the Expansion of NGC 6543: Parallax Distance and Nebular Evolution | ||
| journal = Astronomical Journal | | journal = Astronomical Journal | ||
| year = 1999 | |||
| date = November 1999 | | date = November 1999 | ||
| volume = 118 | | volume = 118 | ||
| issue = 5 | | issue = 5 | ||
| pages = |
| pages = 2430–41 | ||
| |
| bibcode = 1999AJ....118.2430R | ||
| doi = 10.1086/301091 | | doi = 10.1086/301091 | ||
|arxiv = astro-ph/9907313 }} | |||
}} | |||
* {{citation | * {{citation | ||
| last1 = Renzini | |||
| first1 = A. | |||
| year = 1987 | |||
| title = Thermal pulses and the formation of planetary nebula shells | |||
| url = http://adsabs.harvard.edu/abs/1989IAUS..131..391R | |||
| journal = Proceedings of the 131st symposium of the IAU | |||
| editor = S. Torres-Peimbert | |||
| pages = 391–400 | |||
}} | |||
* {{citation | |||
| year = 2002 | |||
| date = February 2002 | | date = February 2002 | ||
| last1 = Soker | | last1 = Soker | ||
| first1 = Noam | | first1 = Noam | ||
| title = Why every bipolar planetary nebula is |
| s2cid = 16616082 | ||
| title = Why every bipolar planetary nebula is 'unique' | |||
| |
| bibcode = 2002MNRAS.330..481S | ||
| journal = Monthly Notices of the Royal Astronomical Society | | journal = Monthly Notices of the Royal Astronomical Society | ||
| volume = 330 | | volume = 330 | ||
| issue = 2 | | issue = 2 | ||
| pages = |
| pages = 481–6 | ||
| doi = 10.1046/j.1365-8711.2002.05105.x | | doi = 10.1046/j.1365-8711.2002.05105.x | ||
| doi-access = free | |||
}} | |||
|arxiv = astro-ph/0107554 }} | |||
* {{citation | * {{citation | ||
| url = http://www.spacedaily.com/news/stellar-chemistry-05a.html | | url = http://www.spacedaily.com/news/stellar-chemistry-05a.html | ||
Line 596: | Line 714: | ||
| publisher = SpaceDaily Express | | publisher = SpaceDaily Express | ||
| date = January 6, 2005 | | date = January 6, 2005 | ||
| year = 2005 | |||
| quote = Source: Journal Astronomy & Astrophysics | | quote = Source: Journal Astronomy & Astrophysics | ||
| |
| access-date = October 18, 2009 | ||
| ref = CITEREFSpaceDaily |
| ref = CITEREFSpaceDaily Express2005 | ||
}} | |||
* {{citation | |||
| last1 = Rees | |||
| first1 = B. | |||
| last2 = Zijlstra | |||
| first2 = A.A. | |||
| s2cid = 118414177 | |||
| date = July 2013 | |||
| title = Alignment of the Angular Momentum Vectors of Planetary Nebulae in the Galactic Bulge | |||
| journal = Monthly Notices of the Royal Astronomical Society | |||
| volume=435 |issue=2 |pages=975–991 | |||
| arxiv=1307.5711 | |||
| bibcode=2013MNRAS.435..975R | |||
| doi=10.1093/mnras/stt1300 | |||
| doi-access = free | |||
}} | |||
* {{citation | |||
| url = http://messier.seds.org/planetar.html | |||
| title = Planetary Nebulae | |||
| publisher = SEDS | |||
| date = September 9, 2013 | |||
| access-date = 2013-11-10 | |||
| ref = CITEREFSEDS2013 | |||
}} | |||
{{refend}} | |||
==Further reading== | |||
* {{citation | |||
| last1 = Iliadis | |||
| first1 = Christian | |||
| title = Nuclear physics of stars. Physics textbook | |||
| publisher = Wiley-VCH | |||
| date = 2007 | |||
| pages = 18, 439–42 | |||
| isbn = 978-3-527-40602-9 | |||
| ref = none | |||
}} | |||
* {{citation | |||
| last1 = Renzini | |||
| first1 = A. | |||
| date = 1987 | |||
| title = Thermal pulses and the formation of planetary nebula shells | |||
| bibcode = 1989IAUS..131..391R | |||
| journal = Proceedings of the 131st Symposium of the IAU | |||
| editor = S. Torres-Peimbert | |||
| pages = 391–400 | |||
| volume = 131 | |||
| ref = none | |||
}} | }} | ||
{{ref end}} | |||
==External links== | == External links == | ||
{{ |
{{Commonscat|Planetary nebulae}} | ||
* | * | ||
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* , SEDS Messier Pages | * , SEDS Messier Pages | ||
* | * | ||
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* | * | ||
{{Star}} | |||
{{-}} | |||
{{featured article}} | |||
{{star}} | |||
{{nebula}} | |||
{{Portal bar|Astronomy|Stars|Outer space}} | |||
{{Authority control}} | |||
{{DEFAULTSORT:Planetary Nebula}} | {{DEFAULTSORT:Planetary Nebula}} | ||
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Latest revision as of 13:08, 2 November 2024
Type of emission nebula created by dying red giantsPlanetary nebula | |
---|---|
NGC 1535 | |
Characteristics | |
Type | Emission nebula |
Mass range | 0.1M☉-1M☉ |
Size range | ~1 ly |
Density | 100 to 10,000 particles per cm |
External links | |
Media category | |
Q13632 | |
Additional Information | |
Discovered | 1764, Charles Messier |
A planetary nebula is a type of emission nebula consisting of an expanding, glowing shell of ionized gas ejected from red giant stars late in their lives.
The term "planetary nebula" is a misnomer because they are unrelated to planets. The term originates from the planet-like round shape of these nebulae observed by astronomers through early telescopes. The first usage may have occurred during the 1780s with the English astronomer William Herschel who described these nebulae as resembling planets; however, as early as January 1779, the French astronomer Antoine Darquier de Pellepoix described in his observations of the Ring Nebula, "very dim but perfectly outlined; it is as large as Jupiter and resembles a fading planet". Though the modern interpretation is different, the old term is still used.
All planetary nebulae form at the end of the life of a star of intermediate mass, about 1-8 solar masses. It is expected that the Sun will form a planetary nebula at the end of its life cycle. They are relatively short-lived phenomena, lasting perhaps a few tens of millennia, compared to considerably longer phases of stellar evolution. Once all of the red giant's atmosphere has been dissipated, energetic ultraviolet radiation from the exposed hot luminous core, called a planetary nebula nucleus (P.N.N.), ionizes the ejected material. Absorbed ultraviolet light then energizes the shell of nebulous gas around the central star, causing it to appear as a brightly coloured planetary nebula.
Planetary nebulae probably play a crucial role in the chemical evolution of the Milky Way by expelling elements into the interstellar medium from stars where those elements were created. Planetary nebulae are observed in more distant galaxies, yielding useful information about their chemical abundances.
Starting from the 1990s, Hubble Space Telescope images revealed that many planetary nebulae have extremely complex and varied morphologies. About one-fifth are roughly spherical, but the majority are not spherically symmetric. The mechanisms that produce such a wide variety of shapes and features are not yet well understood, but binary central stars, stellar winds and magnetic fields may play a role.
Observations
Discovery
The first planetary nebula discovered (though not yet termed as such) was the Dumbbell Nebula in the constellation of Vulpecula. It was observed by Charles Messier on July 12, 1764 and listed as M27 in his catalogue of nebulous objects. To early observers with low-resolution telescopes, M27 and subsequently discovered planetary nebulae resembled the giant planets like Uranus. As early as January 1779, the French astronomer Antoine Darquier de Pellepoix described in his observations of the Ring Nebula, "a very dull nebula, but perfectly outlined; as large as Jupiter and looks like a fading planet".
The nature of these objects remained unclear. In 1782, William Herschel, discoverer of Uranus, found the Saturn Nebula (NGC 7009) and described it as "A curious nebula, or what else to call it I do not know". He later described these objects as seeming to be planets "of the starry kind". As noted by Darquier before him, Herschel found that the disk resembled a planet but it was too faint to be one. In 1785, Herschel wrote to Jérôme Lalande:
These are celestial bodies of which as yet we have no clear idea and which are perhaps of a type quite different from those that we are familiar with in the heavens. I have already found four that have a visible diameter of between 15 and 30 seconds. These bodies appear to have a disk that is rather like a planet, that is to say, of equal brightness all over, round or somewhat oval, and about as well defined in outline as the disk of the planets, of a light strong enough to be visible with an ordinary telescope of only one foot, yet they have only the appearance of a star of about ninth magnitude.
He assigned these to Class IV of his catalogue of "nebulae", eventually listing 78 "planetary nebulae", most of which are in fact galaxies.
Herschel used the term "planetary nebulae" for these objects. The origin of this term not known. The label "planetary nebula" became ingrained in the terminology used by astronomers to categorize these types of nebulae, and is still in use by astronomers today.
Spectra
The nature of planetary nebulae remained unknown until the first spectroscopic observations were made in the mid-19th century. Using a prism to disperse their light, William Huggins was one of the earliest astronomers to study the optical spectra of astronomical objects.
On August 29, 1864, Huggins was the first to analyze the spectrum of a planetary nebula when he observed Cat's Eye Nebula. His observations of stars had shown that their spectra consisted of a continuum of radiation with many dark lines superimposed. He found that many nebulous objects such as the Andromeda Nebula (as it was then known) had spectra that were quite similar. However, when Huggins looked at the Cat's Eye Nebula, he found a very different spectrum. Rather than a strong continuum with absorption lines superimposed, the Cat's Eye Nebula and other similar objects showed a number of emission lines. Brightest of these was at a wavelength of 500.7 nanometres, which did not correspond with a line of any known element.
At first, it was hypothesized that the line might be due to an unknown element, which was named nebulium. A similar idea had led to the discovery of helium through analysis of the Sun's spectrum in 1868. While helium was isolated on Earth soon after its discovery in the spectrum of the Sun, "nebulium" was not. In the early 20th century, Henry Norris Russell proposed that, rather than being a new element, the line at 500.7 nm was due to a familiar element in unfamiliar conditions.
Physicists showed in the 1920s that in gas at extremely low densities, electrons can occupy excited metastable energy levels in atoms and ions that would otherwise be de-excited by collisions that would occur at higher densities. Electron transitions from these levels in nitrogen and oxygen ions (O, O (a.k.a. O iii), and N) give rise to the 500.7 nm emission line and others. These spectral lines, which can only be seen in very low-density gases, are called forbidden lines. Spectroscopic observations thus showed that nebulae were made of extremely rarefied gas.
Central stars
The central stars of planetary nebulae are very hot. Only when a star has exhausted most of its nuclear fuel can it collapse to a small size. Planetary nebulae are understood as a final stage of stellar evolution. Spectroscopic observations show that all planetary nebulae are expanding. This led to the idea that planetary nebulae were caused by a star's outer layers being thrown into space at the end of its life.
Modern observations
Towards the end of the 20th century, technological improvements helped to further the study of planetary nebulae. Space telescopes allowed astronomers to study light wavelengths outside those that the Earth's atmosphere transmits. Infrared and ultraviolet studies of planetary nebulae allowed much more accurate determinations of nebular temperatures, densities and elemental abundances. Charge-coupled device technology allowed much fainter spectral lines to be measured accurately than had previously been possible. The Hubble Space Telescope also showed that while many nebulae appear to have simple and regular structures when observed from the ground, the very high optical resolution achievable by telescopes above the Earth's atmosphere reveals extremely complex structures.
Under the Morgan-Keenan spectral classification scheme, planetary nebulae are classified as Type-P, although this notation is seldom used in practice.
Origins
Stars greater than 8 solar masses (M⊙) will probably end their lives in dramatic supernovae explosions, while planetary nebulae seemingly only occur at the end of the lives of intermediate and low mass stars between 0.8 M⊙ to 8.0 M⊙. Progenitor stars that form planetary nebulae will spend most of their lifetimes converting their hydrogen into helium in the star's core by nuclear fusion at about 15 million K. This generates energy in the core, which creates outward pressure that balances the crushing inward pressures of gravity. This state of equilibrium is known as the main sequence, which can last for tens of millions to billions of years, depending on the mass.
When the hydrogen in the core starts to run out, nuclear fusion generates less energy and gravity starts compressing the core, causing a rise in temperature to about 100 million K. Such high core temperatures then make the star's cooler outer layers expand to create much larger red giant stars. This end phase causes a dramatic rise in stellar luminosity, where the released energy is distributed over a much larger surface area, which in fact causes the average surface temperature to be lower. In stellar evolution terms, stars undergoing such increases in luminosity are known as asymptotic giant branch stars (AGB). During this phase, the star can lose 50–70% of its total mass from its stellar wind.
For the more massive asymptotic giant branch stars that form planetary nebulae, whose progenitors exceed about 0.6M⊙, their cores will continue to contract. When temperatures reach about 100 million K, the available helium nuclei fuse into carbon and oxygen, so that the star again resumes radiating energy, temporarily stopping the core's contraction. This new helium burning phase (fusion of helium nuclei) forms a growing inner core of inert carbon and oxygen. Above it is a thin helium-burning shell, surrounded in turn by a hydrogen-burning shell. However, this new phase lasts only 20,000 years or so, a very short period compared to the entire lifetime of the star.
The venting of atmosphere continues unabated into interstellar space, but when the outer surface of the exposed core reaches temperatures exceeding about 30,000 K, there are enough emitted ultraviolet photons to ionize the ejected atmosphere, causing the gas to shine as a planetary nebula.
Lifetime
After a star passes through the asymptotic giant branch (AGB) phase, the short planetary nebula phase of stellar evolution begins as gases blow away from the central star at speeds of a few kilometers per second. The central star is the remnant of its AGB progenitor, an electron-degenerate carbon-oxygen core that has lost most of its hydrogen envelope due to mass loss on the AGB. As the gases expand, the central star undergoes a two-stage evolution, first growing hotter as it continues to contract and hydrogen fusion reactions occur in the shell around the core and then slowly cooling when the hydrogen shell is exhausted through fusion and mass loss. In the second phase, it radiates away its energy and fusion reactions cease, as the central star is not heavy enough to generate the core temperatures required for carbon and oxygen to fuse. During the first phase, the central star maintains constant luminosity, while at the same time it grows ever hotter, eventually reaching temperatures around 100,000 K. In the second phase, it cools so much that it does not give off enough ultraviolet radiation to ionize the increasingly distant gas cloud. The star becomes a white dwarf, and the expanding gas cloud becomes invisible to us, ending the planetary nebula phase of evolution. For a typical planetary nebula, about 10,000 years passes between its formation and recombination of the resulting plasma.
Role in galactic enrichment
Planetary nebulae may play a very important role in galactic evolution. Newly born stars consist almost entirely of hydrogen and helium, but as stars evolve through the asymptotic giant branch phase, they create heavier elements via nuclear fusion which are eventually expelled by strong stellar winds. Planetary nebulae usually contain larger proportions of elements such as carbon, nitrogen and oxygen, and these are recycled into the interstellar medium via these powerful winds. In this way, planetary nebulae greatly enrich the Milky Way and their nebulae with these heavier elements – collectively known by astronomers as metals and specifically referred to by the metallicity parameter Z.
Subsequent generations of stars formed from such nebulae also tend to have higher metallicities. Although these metals are present in stars in relatively tiny amounts, they have marked effects on stellar evolution and fusion reactions. When stars formed earlier in the universe they theoretically contained smaller quantities of heavier elements. Known examples are the metal poor Population II stars. (See Stellar population.) Identification of stellar metallicity content is found by spectroscopy.
Characteristics
Physical characteristics
A typical planetary nebula is roughly one light year across, and consists of extremely rarefied gas, with a density generally from 100 to 10,000 particles per cm. (The Earth's atmosphere, by comparison, contains 2.5×10 particles per cm.) Young planetary nebulae have the highest densities, sometimes as high as 10 particles per cm. As nebulae age, their expansion causes their density to decrease. The masses of planetary nebulae range from 0.1 to 1 solar masses.
Radiation from the central star heats the gases to temperatures of about 10,000 K. The gas temperature in central regions is usually much higher than at the periphery reaching 16,000–25,000 K. The volume in the vicinity of the central star is often filled with a very hot (coronal) gas having the temperature of about 1,000,000 K. This gas originates from the surface of the central star in the form of the fast stellar wind.
Nebulae may be described as matter bounded or radiation bounded. In the former case, there is not enough matter in the nebula to absorb all the UV photons emitted by the star, and the visible nebula is fully ionized. In the latter case, there are not enough UV photons being emitted by the central star to ionize all the surrounding gas, and an ionization front propagates outward into the circumstellar envelope of neutral atoms.
Numbers and distribution
About 3000 planetary nebulae are now known to exist in our galaxy, out of 200 billion stars. Their very short lifetime compared to total stellar lifetime accounts for their rarity. They are found mostly near the plane of the Milky Way, with the greatest concentration near the Galactic Center.
Morphology
Only about 20% of planetary nebulae are spherically symmetric (for example, see Abell 39). A wide variety of shapes exist with some very complex forms seen. Planetary nebulae are classified by different authors into: stellar, disk, ring, irregular, helical, bipolar, quadrupolar, and other types, although the majority of them belong to just three types: spherical, elliptical and bipolar. Bipolar nebulae are concentrated in the galactic plane, probably produced by relatively young massive progenitor stars; and bipolars in the galactic bulge appear to prefer orienting their orbital axes parallel to the galactic plane. On the other hand, spherical nebulae are probably produced by old stars similar to the Sun.
The huge variety of the shapes is partially the projection effect—the same nebula when viewed under different angles will appear different. Nevertheless, the reason for the huge variety of physical shapes is not fully understood. Gravitational interactions with companion stars if the central stars are binary stars may be one cause. Another possibility is that planets disrupt the flow of material away from the star as the nebula forms. It has been determined that the more massive stars produce more irregularly shaped nebulae. In January 2005, astronomers announced the first detection of magnetic fields around the central stars of two planetary nebulae, and hypothesized that the fields might be partly or wholly responsible for their remarkable shapes.
Membership in clusters
Planetary nebulae have been detected as members in four Galactic globular clusters: Messier 15, Messier 22, NGC 6441 and Palomar 6. Evidence also points to the potential discovery of planetary nebulae in globular clusters in the galaxy M31. However, there is currently only one case of a planetary nebula discovered in an open cluster that is agreed upon by independent researchers. That case pertains to the planetary nebula PHR 1315-6555 and the open cluster Andrews-Lindsay 1. Indeed, through cluster membership, PHR 1315-6555 possesses among the most precise distances established for a planetary nebula (i.e., a 4% distance solution). The cases of NGC 2818 and NGC 2348 in Messier 46, exhibit mismatched velocities between the planetary nebulae and the clusters, which indicates they are line-of-sight coincidences. A subsample of tentative cases that may potentially be cluster/PN pairs includes Abell 8 and Bica 6, and He 2-86 and NGC 4463.
Theoretical models predict that planetary nebulae can form from main-sequence stars of between one and eight solar masses, which puts the progenitor star's age at greater than 40 million years. Although there are a few hundred known open clusters within that age range, a variety of reasons limit the chances of finding a planetary nebula within. For one reason, the planetary nebula phase for more massive stars is on the order of millennia, which is a blink of the eye in astronomic terms. Also, partly because of their small total mass, open clusters have relatively poor gravitational cohesion and tend to disperse after a relatively short time, typically from 100 to 600 million years.
Current issues in planetary nebula studies
The distances to planetary nebulae are generally poorly determined, but the Gaia mission is now measuring direct parallactic distances between their central stars and neighboring stars. It is also possible to determine distances to nearby planetary nebula by measuring their expansion rates. High resolution observations taken several years apart will show the expansion of the nebula perpendicular to the line of sight, while spectroscopic observations of the Doppler shift will reveal the velocity of expansion in the line of sight. Comparing the angular expansion with the derived velocity of expansion will reveal the distance to the nebula.
The issue of how such a diverse range of nebular shapes can be produced is a debatable topic. It is theorised that interactions between material moving away from the star at different speeds gives rise to most observed shapes. However, some astronomers postulate that close binary central stars might be responsible for the more complex and extreme planetary nebulae. Several have been shown to exhibit strong magnetic fields, and their interactions with ionized gas could explain some planetary nebulae shapes.
There are two main methods of determining metal abundances in nebulae. These rely on recombination lines and collisionally excited lines. Large discrepancies are sometimes seen between the results derived from the two methods. This may be explained by the presence of small temperature fluctuations within planetary nebulae. The discrepancies may be too large to be caused by temperature effects, and some hypothesize the existence of cold knots containing very little hydrogen to explain the observations. However, such knots have yet to be observed.
See also
- Asymptotic giant branch
- Cosmic distance ladder
- Fast Low-Ionization Emission Region
- Nova remnant
- PG 1159 star (predegenerates)
- Protoplanetary nebula
- Supernova remnant
- White dwarf
- List of planetary nebulae
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We report the discovery of multiple two-dimensional rings in the quadrupolar planetary nebula NGC 6881. As many as four pairs of rings are seen in the bipolar lobes, and three rings are seen in the central torus. While the rings in the lobes have the same axis as one pair of the bipolar lobes, the inner rings are aligned with the other pair. The two pairs of bipolar lobes are likely to be carved out by two separate high-velocity outflows from the circumstellar material left over from the asymptotic giant branch (AGB) wind. The two-dimensional rings could be the results of dynamical instabilities or the consequence of a fast outflow interacting with remnants of discrete AGB circumstellar shells.
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Planetary nebulae (PNs) have high dust content and radiate strongly in the infrared. For young PNs, the dust component accounts for about one third of the total energy output of the nebulae (Zhang & Kwok 1991). The typical color temperatures of PNs are between 100 and 200 K, and at λ >5 μm, dust begins to dominate over bound-free emission from the ionized component. Although PNs are traditionally discovered through examination of photographic plates or Hα surveys, PNs can also be identified in infrared surveys by searching for red objects with a rising spectrum between 4–10 μm.
{{citation}}
: CS1 maint: DOI inactive as of November 2024 (link) - Liu, X.-W.; Storey, P. J.; Barlow, M. J.; Danziger, I. J.; Cohen, M.; Bryce, M. (March 2000), "NGC 6153: a super–metal–rich planetary nebula?", Monthly Notices of the Royal Astronomical Society, 312 (3): 585–628, Bibcode:2000MNRAS.312..585L, doi:10.1046/j.1365-8711.2000.03167.x
- Maciel, W. J.; Costa, R. D. D.; Idiart, T. E. P. (October 2009), "Planetary nebulae and the chemical evolution of the Magellanic Clouds", Revista Mexicana de Astronomía y Astrofísica, 45: 127–37, arXiv:0904.2549, Bibcode:2009RMxAA..45..127M,
These objects are produced by low and intermediate mass stars, with main sequence masses roughly between 0.8 and 8 M⊙, and present a reasonably large age and metallicity spread.
- Majaess, D. J.; Turner, D.; Lane, D. (December 2007), "In Search of Possible Associations between Planetary Nebulae and Open Clusters", Publications of the Astronomical Society of the Pacific, 119 (862): 1349–60, arXiv:0710.2900, Bibcode:2007PASP..119.1349M, doi:10.1086/524414, S2CID 18640979
- Marochnik, L.S.; Shukurov, Anwar; Yastrzhembsky, Igor (1996), "Chapter 19: Chemical abundances", The Milky Way galaxy, Taylor & Francis, pp. 6–10, ISBN 978-2-88124-931-0
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- Miszalski, B.; Jones, D.; Rodríguez-Gil, P.; Boffin, H. M. J.; Corradi, R. L. M.; Santander-García, M. (2011), "Discovery of close binary central stars in the planetary nebulae NGC 6326 and NGC 6778", Astronomy and Astrophysics, 531: A158, arXiv:1105.5731, Bibcode:2011A&A...531A.158M, doi:10.1051/0004-6361/201117084, S2CID 15010950
- Moore, S. L. (October 2007), "Observing the Cat's Eye Nebula", Journal of the British Astronomical Association, 117 (5): 279–80, Bibcode:2007JBAA..117R.279M
- Morris, M. (1990), "Bipolar asymmetry in the mass outflows of stars in transition", in Mennessier, M.O.; Omont, Alain (eds.), From Miras to planetary nebulae: which path for stellar evolution?, Montpellier, France, September 4–7, 1989 IAP astrophysics meeting: Atlantica Séguier Frontières, pp. 526–30, ISBN 978-2-86332-077-8
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: CS1 maint: location (link) - Osterbrock, Donald E.; Ferland, G. J. (2005), Ferland, G. J. (ed.), Astrophysics of gaseous nebulae and active galactic nuclei, University Science Books, ISBN 978-1-891389-34-4
- Parker, Quentin A.; Acker, A.; Frew, D. J.; Hartley, M.; Peyaud, A. E. J.; Ochsenbein, F.; Phillipps, S.; Russeil, D.; Beaulieu, S. F.; Cohen, M.; Köppen, J.; Miszalski, B.; Morgan, D. H.; Morris, R. A. H.; Pierce, M. J.; Vaughan, A. E. (November 2006), "The Macquarie/AAO/Strasbourg Hα Planetary Nebula Catalogue: MASH", Monthly Notices of the Royal Astronomical Society, 373 (1): 79–94, Bibcode:2006MNRAS.373...79P, doi:10.1111/j.1365-2966.2006.10950.x
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- Reed, Darren S.; Balick, Bruce; Hajian, Arsen R.; Klayton, Tracy L.; Giovanardi, Stefano; Casertano, Stefano; Panagia, Nino; Terzian, Yervant (November 1999), "Hubble Space Telescope Measurements of the Expansion of NGC 6543: Parallax Distance and Nebular Evolution", Astronomical Journal, 118 (5): 2430–41, arXiv:astro-ph/9907313, Bibcode:1999AJ....118.2430R, doi:10.1086/301091, S2CID 14746840
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- The first detection of magnetic fields in the central stars of four planetary nebulae, SpaceDaily Express, January 6, 2005, retrieved October 18, 2009,
Source: Journal Astronomy & Astrophysics
- Rees, B.; Zijlstra, A.A. (July 2013), "Alignment of the Angular Momentum Vectors of Planetary Nebulae in the Galactic Bulge", Monthly Notices of the Royal Astronomical Society, 435 (2): 975–991, arXiv:1307.5711, Bibcode:2013MNRAS.435..975R, doi:10.1093/mnras/stt1300, S2CID 118414177
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Further reading
- Iliadis, Christian (2007), Nuclear physics of stars. Physics textbook, Wiley-VCH, pp. 18, 439–42, ISBN 978-3-527-40602-9
- Renzini, A. (1987), S. Torres-Peimbert (ed.), "Thermal pulses and the formation of planetary nebula shells", Proceedings of the 131st Symposium of the IAU, 131: 391–400, Bibcode:1989IAUS..131..391R
External links
- Entry in the Encyclopedia of Astrobiology, Astronomy, and Spaceflight
- Press release on recent observations of the Cat's Eye Nebula
- Planetary Nebulae, SEDS Messier Pages
- The first detection of magnetic fields in the central stars of four planetary nebulae
- Planetary Nebulae—Information and amateur observations
- Planetary nebula on arxiv.org
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