Paper 3, Section II, B

Cosmology | Part II, 2018

The pressure support equation for stars is

1r2ddr[r2ρdPdr]=4πGρ\frac{1}{r^{2}} \frac{d}{d r}\left[\frac{r^{2}}{\rho} \frac{d P}{d r}\right]=-4 \pi G \rho

where ρ\rho is the density, PP is the pressure, rr is the radial distance, and GG is Newton's constant.

(a) What two boundary conditions should we impose on the above equation for it to describe a star?

(b) By assuming a polytropic equation of state,

P(r)=Kρ1+1n(r)P(r)=K \rho^{1+\frac{1}{n}}(r)

where KK is a constant, derive the Lane-Emden equation

1ξ2ddξ[ξ2dθdξ]=θn\frac{1}{\xi^{2}} \frac{d}{d \xi}\left[\xi^{2} \frac{d \theta}{d \xi}\right]=-\theta^{n}

where ρ=ρcθn\rho=\rho_{c} \theta^{n}, with ρc\rho_{c} the density at the centre of the star, and r=aξr=a \xi, for some aa that you should determine.

(c) Show that the mass of a polytropic star is

M=12π((n+1)KG)32ρc3n2nYnM=\frac{1}{2 \sqrt{\pi}}\left(\frac{(n+1) K}{G}\right)^{\frac{3}{2}} \rho_{c}^{\frac{3-n}{2 n}} Y_{n}

where Ynξ12dθdξξ=ξ1Y_{n} \equiv-\left.\xi_{1}^{2} \frac{d \theta}{d \xi}\right|_{\xi=\xi_{1}} and ξ1\xi_{1} is the value of ξ\xi at the surface of the star.

(d) Derive the following relation between the mass, MM, and radius, RR, of a polytropic star

M=AnKnn1R3n1nM=A_{n} K^{\frac{n}{n-1}} R^{\frac{3-n}{1-n}}

where you should determine the constant AnA_{n}. What type of star does the n=3n=3 polytrope represent and what is the significance of the mass being constant for this star?

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