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A convection zone, convective zone or convective region of a star is a layer which is unstable to convection. Energy is primarily or partially transported by convection in such a region. In a radiation zone, energy is transported by radiation and conduction.

Stellar convection consists of mass movement of plasma within the star which usually forms a circular convection current with the heated plasma ascending and the cooled plasma descending.

The Schwarzschild criterion expresses the conditions under which a region of a star is unstable to convection. A parcel of gas that rises slightly will find itself in an environment of lower pressure than the one it came from. As a result, the parcel will expand and cool. If the rising parcel cools to a lower temperature than its new surroundings, so that it has a higher density than the surrounding gas, then its lack of buoyancy will cause it to sink back to where it came from. However, if the temperature gradient is steep enough (i.e. the temperature changes rapidly with distance from the center of the star), or if the gas has a very high heat capacity (i.e. its temperature changes relatively slowly as it expands) then the rising parcel of gas will remain warmer and less dense than its new surroundings even after expanding and cooling. Its buoyancy will then cause it to continue to rise. The region of the star in which this happens is the convection zone.

Main sequence stars
See also: Radiation zone § Stability against convection

In main sequence stars more than 1.3 times the mass of the Sun, the high core temperature causes nuclear fusion of hydrogen into helium to occur predominantly via the carbon-nitrogen-oxygen (CNO) cycle instead of the less temperature-sensitive proton-proton chain. The high temperature gradient in the core region forms a convection zone that slowly mixes the hydrogen fuel with the helium product. The core convection zone of these stars is overlaid by a radiation zone that is in thermal equilibrium and undergoes little or no mixing.[1] In the most massive stars, the convection zone may reach all the way from the core to the surface.[2]

In main sequence stars of less than about 1.3 solar masses, the outer envelope of the star contains a region where partial ionization of hydrogen and helium raises the heat capacity. The relatively low temperature in this region simultaneously causes the opacity due to heavier elements to be high enough to produce a steep temperature gradient. This combination of circumstances produces an outer convection zone, the top of which is visible in the Sun as solar granulation. Low mass main sequences of stars, such as red dwarfs below 0.35 solar masses,[3] as well as pre-main sequence stars on the Hayashi track, are convective throughout and do not contain a radiation zone.[4]

In main sequence stars similar to the Sun, which have a radiative core and convective envelope, the transition region between the convection zone and the radiation zone is called the tachocline.
Red giants

In red giant stars, and particularly during the asymptotic giant branch phase, the surface convection zone varies in depth during the phases of shell burning. This causes dredge-up events, short-lived very deep convection zones that transport fusion products to the surface of the star.[5]

Behrend, R.; Maeder, A. (2001). "Formation of massive stars by growing accretion rate". Astronomy and Astrophysics. 373: 190–198.arXiv:astro-ph/0105054. Bibcode:2001A&A...373..190B. doi:10.1051/0004-6361:20010585. S2CID 18153904.
Martins, F.; Depagne, E.; Russeil, D.; Mahy, L. (2013). "Evidence of quasi-chemically homogeneous evolution of massive stars up to solar metallicity". Astronomy and Astrophysics. 554: A23.arXiv:1304.3337. Bibcode:2013A&A...554A..23M. doi:10.1051/0004-6361/201321282. S2CID 54707309.
Reiners, A.; Basri, G. (March 2009). "On the magnetic topology of partially and fully convective stars". Astronomy and Astrophysics. 496 (3): 787–790.arXiv:0901.1659. Bibcode:2009A&A...496..787R. doi:10.1051/0004-6361:200811450. S2CID 15159121.
d'Antona, F.; Montalbán, J. (2003). "Efficiency of convection and Pre-Main Sequence lithium depletion". Astronomy and Astrophysics. 212: 213–218.arXiv:astro-ph/0309348. Bibcode:2003A&A...412..213D. doi:10.1051/0004-6361:20031410. S2CID 2590382.

Lebzelter, T.; Lederer, M. T.; Cristallo, S.; Hinkle, K. H.; Straniero, O.; Aringer, B. (2008). "AGB stars of the intermediate-age LMC cluster NGC 1846". Astronomy and Astrophysics. 486 (2): 511.arXiv:0805.3242. Bibcode:2008A&A...486..511L. doi:10.1051/0004-6361:200809363. S2CID 18811290.

Further reading

Hansen, C. J.; Kawaler, S. D. & Trimble, V. (2004). Stellar Interiors. Springer. ISBN 0-387-20089-4.
Zeilik, M.; Gregory, S. A. (1998). Introductory Astronomy and Astrophysics. Brooks Cole. ISBN 978-0-03-006228-5.

External links

Animated explanation of the Convection zone (University of South Wales).
Animated explanation of the temperature and density of the Convection zone (University of South Wales).


Accretion Molecular cloud Bok globule Young stellar object
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Shell B[e]


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The Sun by the Atmospheric Imaging Assembly of NASA's Solar Dynamics Observatory - 20100819.jpg

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Spectral class: G-type main-sequence star

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