Calculating Solar Core Radius Using Emden's Equation

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Discussion Overview

The discussion centers around calculating the solar core radius using Emden's equation, focusing on the modeling of the sun's interior through polytropic approximations. Participants explore theoretical approaches, assumptions, and the implications of using different polytropic indices.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant proposes a homologous polytropic core model (n=3) to calculate the core radius, suggesting a relationship between energy generation rate and density.
  • Another participant argues that the sun is not well approximated by an n=3 polytrope and suggests that central density and temperature should emerge from the model rather than being guessed.
  • A different participant defends the use of a 3-polytrope as a good model for the sun, questioning the previous assertion and seeking clarification on the derivation of the variable "eta."
  • Further discussion reveals that "eta" is defined as a ratio of energy generation rates, and a participant references Chandrasekhar's work to support their approach.
  • One participant defines the core radius as the point where energy generation equals zero, proposing a method to compute it based on luminosity and energy generation rates.
  • There is a shift in terminology from "eta" to "lambda" to clarify the relationship being discussed, with "lambda" being a constant specific to the polytropic formulation.

Areas of Agreement / Disagreement

Participants express differing views on the appropriateness of using an n=3 polytrope to model the sun, with some supporting its validity while others contest it. The discussion remains unresolved regarding the best approach to determine the core radius and the assumptions underlying the models presented.

Contextual Notes

Participants highlight limitations in their models, including the non-uniform equation of state in the sun and the dependence on specific definitions of variables like "eta" and "lambda." There are unresolved mathematical steps in deriving the core radius from the proposed relationships.

Helios
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I've begun a study of the sun's interior and Emden's equation. Yet nowhere on the web does anyone divulge how to calculate the core radius or the inner core variables. One thing I did was to suppose a homologous polytropic core ( n = 3 ) with:
epsilon = energy generation rate
mean epsilon = L / M
rho = density
mean rho = M / V
so I postulated the homology:
epsilon (center) / epsilon (mean) = rho (center) / rho (mean) = eta
This immediately leads to results that closely match one computer model I found, with
core radius = .2643 R = eta^(-1/3) R,
but my approach seems ad hoc. Any help?
 
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The sun isn't very well approximated by an n=3 polytrope (or any polytrope, for that matter), but if you wish to model it that way, you shouldn't need to guess the central density or temperature. These should fall out naturally when you insist that the total mass be equal to the observed mass of the sun (assuming the usual solar composition).
 
A 3-polytrope is a very good model of the sun. If you disagree, please explain. I did not "guess" at the central density or temperature. I know these derivations. I asked for a way to determine the core radius.
 
Helios said:
A 3-polytrope is a very good model of the sun. If you disagree, please explain.

The sun has both radiative and convective regions, so has a non-uniform equation of state. Of the simple models, however, n=3 probably is the best.


I did not "guess" at the central density or temperature.

Where did your value of "eta" come from?


I know these derivations. I asked for a way to determine the core radius.

Once given a mass, radius, and polytropic index, I was under the impression you would be able to model the entire star and take from that whatever parameters you want (though I've never done it myself). How are you defining the core radius?
 
Eta is used as a some ratio like epsilon/ mean epsilon or the like.
Chandrasekhar ( in 1939 ) uses it when presenting several star models in his book " Intro to Stellar Structure" at the time when fusion was not well understood.
Lamda is a constant of the polytrope formulation ( = 54.1825 for n=3 ) and ( by proof ) equals rho ( center ) / rho ( mean )
So I set Eta = epsilon (center) / epsilon (mean)
and supposed Eta = Lamda, a homology.
How do I define the core radius? It's the radius where the energy generation equals zero and luminosity becomes constant. The core I defined borrows the polytrope mathematics of the sun at large and replaces density with energy generation rate and mass with luminosity -- a sort of sun within a sun. Then as easy as comparing similar triangles, a core radius can be computed, which looks good ( core = .2643 R ), but is somewhat ad hoc.

I would now rather use lamda instead of eta to avoid any confusion, hence;
epsilon (center) / epsilon (mean) = rho (center) / rho (mean) = lamda = 54.1825
 
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