Modeling a Star: Struggling with Newton-Raphson Technique

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The discussion focuses on modeling a star using the shooting method, with particular challenges arising from the integration process. The need for a multi-dimensional Newton-Raphson technique is emphasized, suggesting that the initial implementation may be flawed. Key steps include applying the equations of stellar structure and hydrostatic equilibrium, along with boundary conditions related to core temperature and pressure. The use of the Saha equation for ion abundance and opacity is highlighted, as well as the importance of transitioning from radius fraction to mass fraction using the chain rule. The conversation concludes with a suggestion to use the Runge-Kutta method for calculating the power fraction enclosed.
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I am trying to model a star using the old shooting method technique. I've encountered problems after my very first pass of integration. I know that I need to use a multi-dimensional Newton-Raphson technique and i think that I've not done this correctly. Could anybody please try and explain this technique.
 
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mccizmt2 said:
I am trying to model a star using the old shooting method technique. I've encountered problems after my very first pass of integration. I know that I need to use a multi-dimensional Newton-Raphson technique and i think that I've not done this correctly. Could anybody please try and explain this technique.
Start with the equations of stellar structure and the equation of hydrostatic equilibrium, apply the boundary conditions you know: core temperature and pressure, and T=0 and P=0 at r=Rsun. The XYZ composition and the Saha equation gives you the abundance of free ions and the opacity. Use the chain rule to change the independent variable from radius fraction to mass fraction. Begin by assuming constant density. Solve the equation set to obtain a revised density function, and repeat until rho(M) converges. Runga Kutta might give you the power fraction enclosed from M=0 to M=Mi. If there's a name for doing this, I never heard what it was.

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