Newsgroups: sci.astro, sci.physics, sci.math
From: tadchem <tadc...@comcast.net>
Date: Sat, 5 Jul 2008 15:24:49 -0700 (PDT)
Local: Sun, Jul 6 2008 3:24 am
Subject: Re: Stellar Hydrostatic Equilibrium with Differential Rotation
On Jul 5, 5:48 pm, John Schutkeker <jschutke...@sbcglobal.net.nospam>
wrote: > I followed the procedure at the following site, You might try a more realistic equation of state. The one you have is > http://www.astro.utu.fi/~cflynn/Stars/l4.html > and I believe that I've correctly added a centripetal force term to the > I added the centripetal force, rho*w^2*r, as a second body force term in > dP/dr=rho(r)*w^2*r*sin(theta)-G*m(r)*rho(r)/r^2, > where w is omega, the rotational frequency of the star, which is allowed to > The middle part is pretty much just algebra, and the answer I got was > (1/r^2)*d[(r^2/rho)(dP/dr)]/dr+4*pi*G*rho=[3w^2+2*w*r*dw/dr]*sin(theta). > Actually, you can tell by the presence of a dw/dr term that I allowed w to > If I were to put in the compressible equation of state for a fluid, > In summary, I need to know whether the above equations and derivation look > Any reasonable input would be greatly appreciated. TIA. an ideal thermodynamic gas equation with considerations made for heat capacities (gamma = Cp / Cv is the adiabatic index - the ratio of specific heats). This might be sufficient for gases at densities well below those found at the critical point, but at higher densities, the fluid becomes 'incompressible'. You might try a 'hardened' equation - one which has special Tom Davidson You must Sign in before you can post messages.
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