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Consider a star of Radius R and mass M, with a pressure gradient given by
\frac{dP}{dr} = \frac{4\pi}{3}G\rho2r exp(-\frac{rr}{\lambda\lambda})
where \rho is the central density. calculate the gravitational energy, using the Virial theorem. Show that in the limit \lambda « R this energy is given by
E = \frac{RGMM}{3R\lambda}for tecnical reasons:
MM = M2
rr = r2
\lambda\lambda = \lambda2
\frac{dP}{dr} = \frac{4\pi}{3}G\rho2r exp(-\frac{rr}{\lambda\lambda})
where \rho is the central density. calculate the gravitational energy, using the Virial theorem. Show that in the limit \lambda « R this energy is given by
E = \frac{RGMM}{3R\lambda}for tecnical reasons:
MM = M2
rr = r2
\lambda\lambda = \lambda2
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