Dazed&Confused
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Homework Statement
Assume that the pressure p in a star with spherical symmetry is related to the density \rho by the (distinctly unrealistic) equation of state p= \tfrac12 k\rho^2, where k is a constant. Use the fluid equilibrium equation obtained in Problem 23 to find a relation between \rho and \Phi. Hence show that Poisson's equation yields
<br /> \frac{d^2[r\rho(r)]}{dr^2} = -\frac{4 \pi G}{k}r \rho(r)<br />
Solve this equation with the boundary conditions that \rho is finite at r=0 and vanishes at the surface of the star. Hence show that the radius a of the star is determinde solely by k and is independent of its mass M. Show also that M =(4/ \pi )a^4 \rho(0).
Homework Equations
\nabla p = \rho \textbf{g} and p + \rho \Phi = \textrm{constant}. And \nabla^2 \Phi = 4\pi G \rho.
The Attempt at a Solution
Assuming the differential equation, I am able to do the rest of the question. The relation they are looking for is \Phi = -k\rho and this can be easily shown by
\nabla p = k\rho'(r) \rho(r) \hat{\textrm{r}} = \rho \textrm{g} and so
-\nabla \Phi = \textrm{g} = k\rho'(r) \hat{\textrm{r}}
from which you can get \Phi. However by the second relevant equation this must also mean that -\tfrac12 k \rho^2 = \textrm{constant}, or I'm missing something. I've also not been able to obtain the differential equation.