Difference between revisions of "Red giant"

From Conservapedia
Jump to navigation Jump to search
(Created page with 'A Red giant is a very luminous, enormous star typically tens to hundreds the times the diameter of our own sun that represents the late stages of the stellar evolution of a main ...')
 
(→‎top: Spelling/Grammar Check, typos fixed: less then → less than)
 
(17 intermediate revisions by 9 users not shown)
Line 1: Line 1:
−
A Red giant is a very luminous, enormous star typically tens to hundreds the times the diameter of our own sun that represents the late stages of the stellar evolution of a main sequence star of less than 4 solar masses.   
+
[[File:Betelgeuse NASA ESA.jpg|right|thumb|Betelgeuse, an example of a red giant star]]
 +
A '''red giant''' is an enormous, highly luminous star, typically tens to hundreds the times the diameter of our own [[sun]], that represents the late stages of the [[stellar evolution]] of a main sequence [[star]].  Typically for stars between 0.5 and 6 solar masses.<ref>The Cambridge Atlas of Astronomy (2nd ed.). Cambridge University Press. 1988. pp. 255. ISBN 0-521-36360-8.</ref>  The greater the mass of the star, the more quickly it will enter the red giant phase of its evolution.   
  
−
A Red giant forms when after a few billion years when a main sequence star exhausts all of it's [[hydrogen]] fuel in it's core used for [[nuclear fusion]].  At this point the outer shell of the star, still made mainly up of hydrogen, begins to collapse under gravity when the hydrogen gas heats up.  At this point the shell surrounding the core of the star will become hot enough to fuse the hydrogen into [[helium]], providing a new source of energy.  as the core star is now hotter than it was during the stars main sequence life, the outer parts of the star to swell. because of the expansion of the outer layers of the star, the energy produced in the core of the star is spread over a vastly larger surface area.  This results in a lower surface temperature which shifts the star's visible output towards the red side of the visual spectrum.
+
The red giant stage begins when a main sequence star exhausts all of the [[hydrogen]] fuel used for nuclear fusion in its core.  The hydrogen located just outside of the core, however, will not fuse due to the lower temperature of the region.  The star will then begin to contract under [[gravity]], and the outer layers of the star will start to collapse.  As the shells of hydrogen gas contract towards the core, they heat up, eventually reaching the temperature required to fuse the hydrogen into [[helium]], providing a new source of energy and halting the collapse through a renewal of stellar fusion.  As the star has now grown hotter than it was during the star's life during the main sequence, the outer parts of the star begin to swell. Because of the expansion of the outer layers of the star, the energy produced in the core of the star is spread over a vastly larger surface area.  This results in a lower surface temperature, which shifts the star's visible output towards the red side of the visual spectrum.
  
−
At this point the core will become dense enough that electron degeneracy pressure will prevent it from collapsing further. The core will then continue to heat until it reaches a temperature of roughly 10<sup>8</sup>K, hot enough to begin fusing helium to [[carbon]]. Once the core reaches this temperature, depending on the mass of the star, a helium fusion may occur. In more massive stars over 2.57 solar masses, the collapsing core will reach 10<sup>8</sup>K point before electron degeneracy can occur, therefore it will begin to fuse carbon without a helium flash.  
+
Depending of the mass of the star, there are two different routes the red giant's evolution will take.  For those stars that are less than 2.55 solar masses, the core will continue to contract until it becomes degenerate.  At this point, the core will not contract any further, but will continue to heat up.  As the temperature reaches 10<sup>8</sup> K, it will become hot enough for the core to begin fusing helium to [[carbon]] and to a lesser extent, [[oxygen]]. As degenerate matter is an excellent conductor of heat, all the helium will be fused nearly simultaneously in a [[helium flash]]. For more massive stars, the 10<sup>8</sup> K temperature required to fuse helium will happen as the core is still contracting, allowing for a much more fluid fusion of helium, avoiding the flash.<ref>http://hyperphysics.phy-astr.gsu.edu/Hbase/astro/redgia.html</ref>
  
−
Once the helium begins fusing, the star again contracts and leaves the red giant stage. A star who become a red giant lacks the necessary mass to generate enough energy to fuse carbon<ref>http://hyperphysics.phy-astr.gsu.edu/Hbase/astro/redgia.html</ref>.  Once the helium has been all converted to carbon, the star will eject its outer layers as a planetary nebula, exposing the core.  The star thus becomes a [[white dwarf]], slowly cooling off over time<ref> Zeilik, Michael A.; Gregory, Stephan A. (1998). Introductory Astronomy & Astrophysics (4th ed.). Saunders College Publishing. pp. 321–322. ISBN 0030062284.</ref>.
+
Once the helium begins fusing, the star again contracts and leaves the red giant stage. For stars around the mass of our Sun, insufficient mass exists to fuse oxygen and carbon into heavier elements.  Once the star lacks any more helium to fuse, the star will eject its expanded outer layers as a planetary nebula, exposing the core.  The star thus becomes a [[white dwarf]], slowly cooling off over time.<ref>Zeilik, Michael A.; Gregory, Stephan A. (1998). Introductory Astronomy & Astrophysics (4th ed.). Saunders College Publishing. pp. 321–322. ISBN 0030062284.</ref> More massive stars will continue to fuse the carbon and oxygen into heavier elements.  Any stars that are 10 solar masses or greater will instead become  [[supergiant|red supergiants]] before ending their lives in a [[supernova]] explosion.
  
−
===Our sun's fate as a red giant===
+
Low mass [[red dwarf]]s will not have sufficient mass to fuse helium and thus never enter a red giant phase, but instead will simply cool over time once all the hydrogen fuel is consumed.
  
−
It is estimated that in about 5 billion years our sun will have burned through it's hydrogen fuel needed for nuclear fusion and enter into the red giant phase itself<ref>http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1993ApJ...418..457S&data_type=PDF_HIGH&whole_paper=YES&type=PRINTER&filetype=.pdf</ref>.  The sun is then estimated to expand to 200 times it's current diameter but will loss significant mass, perhaps enough so that the orbit the Earth will widen enough not to be swallowed by the expanding red giant, due to it's weakened gravity, although this is debated.  If the Earth does survive intact the red giant phase of the sun, it's atmosphere will be striped and the surface will become hot enough to be molten.
+
[[Category:Astronomy]]
  
 
==References==
 
==References==
 
{{reflist}}
 
{{reflist}}

Latest revision as of 17:17, August 15, 2016

Betelgeuse, an example of a red giant star

A red giant is an enormous, highly luminous star, typically tens to hundreds the times the diameter of our own sun, that represents the late stages of the stellar evolution of a main sequence star. Typically for stars between 0.5 and 6 solar masses.[1] The greater the mass of the star, the more quickly it will enter the red giant phase of its evolution.

The red giant stage begins when a main sequence star exhausts all of the hydrogen fuel used for nuclear fusion in its core. The hydrogen located just outside of the core, however, will not fuse due to the lower temperature of the region. The star will then begin to contract under gravity, and the outer layers of the star will start to collapse. As the shells of hydrogen gas contract towards the core, they heat up, eventually reaching the temperature required to fuse the hydrogen into helium, providing a new source of energy and halting the collapse through a renewal of stellar fusion. As the star has now grown hotter than it was during the star's life during the main sequence, the outer parts of the star begin to swell. Because of the expansion of the outer layers of the star, the energy produced in the core of the star is spread over a vastly larger surface area. This results in a lower surface temperature, which shifts the star's visible output towards the red side of the visual spectrum.

Depending of the mass of the star, there are two different routes the red giant's evolution will take. For those stars that are less than 2.55 solar masses, the core will continue to contract until it becomes degenerate. At this point, the core will not contract any further, but will continue to heat up. As the temperature reaches 108 K, it will become hot enough for the core to begin fusing helium to carbon and to a lesser extent, oxygen. As degenerate matter is an excellent conductor of heat, all the helium will be fused nearly simultaneously in a helium flash. For more massive stars, the 108 K temperature required to fuse helium will happen as the core is still contracting, allowing for a much more fluid fusion of helium, avoiding the flash.[2]

Once the helium begins fusing, the star again contracts and leaves the red giant stage. For stars around the mass of our Sun, insufficient mass exists to fuse oxygen and carbon into heavier elements. Once the star lacks any more helium to fuse, the star will eject its expanded outer layers as a planetary nebula, exposing the core. The star thus becomes a white dwarf, slowly cooling off over time.[3] More massive stars will continue to fuse the carbon and oxygen into heavier elements. Any stars that are 10 solar masses or greater will instead become red supergiants before ending their lives in a supernova explosion.

Low mass red dwarfs will not have sufficient mass to fuse helium and thus never enter a red giant phase, but instead will simply cool over time once all the hydrogen fuel is consumed.

References

  1. ↑ The Cambridge Atlas of Astronomy (2nd ed.). Cambridge University Press. 1988. pp. 255. ISBN 0-521-36360-8.
  2. ↑ http://hyperphysics.phy-astr.gsu.edu/Hbase/astro/redgia.html
  3. ↑ Zeilik, Michael A.; Gregory, Stephan A. (1998). Introductory Astronomy & Astrophysics (4th ed.). Saunders College Publishing. pp. 321–322. ISBN 0030062284.