Stellar Evolution: After Hydrogen Exhaustion

Click For Summary
SUMMARY

After hydrogen exhaustion in low mass stars, the core becomes isothermal due to the absence of nuclear burning and a radiative temperature gradient. This occurs during an intermediate stage where gravitational energy is released until the core reaches the Schönberg-Chandrasekhar limit, defined as the mass of the core divided by the mass of the star being approximately 0.1. At this point, thermal pressure is insufficient to counteract gravitational pressure, leading to rapid core contraction and triggering hydrogen shell burning.

PREREQUISITES
  • Understanding of stellar evolution concepts
  • Familiarity with the Schönberg-Chandrasekhar limit
  • Knowledge of nuclear fusion processes in stars
  • Basic principles of thermodynamics in astrophysics
NEXT STEPS
  • Research the mechanisms of hydrogen shell burning in stars
  • Study the implications of the Schönberg-Chandrasekhar limit on stellar stability
  • Explore the differences between low mass and high mass star evolution
  • Investigate the role of radiative temperature gradients in stellar cores
USEFUL FOR

Astronomers, astrophysicists, and students studying stellar evolution and nuclear astrophysics will benefit from this discussion.

vertices
Messages
62
Reaction score
0
why after hydrogen exhaustion (of low mass stars) does the the core become isothermal. (according to my notes)

I mean, after exhaustion, its all helium, and it keeps on contracting right? So by the virial therem it must heat up (so by definition, it is NOT isothermal)! Indeed it must do so so as to trigger hydrogen shell burning.

Thanks:)
 
Astronomy news on Phys.org
I think you're right, but missing a stage between the exhaustion and rapid contraction of the core. I always thought there was an intermediate stage where the core released energy gravitationally until a critical mass was reached (there's a name to the limit, probably to do with Chandrasekhar!) and rapid core contraction happened. It is this stage that's isothermal, not the rapid contraction.

EDIT:

http://en.wikipedia.org/wiki/Schönberg-Chandrasekhar_limit
 
thanks astrorob...

Yes you are right.

1)hydrogen burns in shell around inert core (shell-burning phase)

2)*The core grows until Mass of core DIVIDED by Mass of star ~ 0.1. (Schoneberg - Chandresekar limit)*

3)At this stage, the core the thermal pressure is not sufficient to balance gravitational pressure and it rapidly contracts...

questions:

a)am i wrong about the fact that the inner core must heat up to trigger hydrogen shell burning? Or does this just occur spontaneously when the core hydrogen is depleted?

b)why is the core isothermal between stages (1) and (2) anyway? What's the physical explanation for this?

thanks:)
 
i) The only reason the core becomes inert is because it uses its fuel up much faster than the outermost layers. Normally hydrogen continues burning in a shell which causes the accumulation of matter onto the inert core until the SC limit is reached.

ii) It arises from the fact that there is no nuclear burning and the temperature gradient is radiative, so its thermal stratification is essentially isothermal.
 
astrorob said:
i) The only reason the core becomes inert is because it uses its fuel up much faster than the outermost layers. Normally hydrogen continues burning in a shell which causes the accumulation of matter onto the inert core until the SC limit is reached.

ii) It arises from the fact that there is no nuclear burning and the temperature gradient is radiative, so its thermal stratification is essentially isothermal.

thanks rob.
 
no problem buddy, glad to be of help.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 16 ·
Replies
16
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 21 ·
Replies
21
Views
3K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 1 ·
Replies
1
Views
3K