Paper 1, Section II, D

Cosmology
Part II, 2010

A star has pressure P(r)P(r) and mass density ρ(r)\rho(r), where rr is the distance from the centre of the star. These quantities are related by the pressure support equation

P=Gmρr2P^{\prime}=-\frac{G m \rho}{r^{2}}

where P=dP/drP^{\prime}=d P / d r and m(r)m(r) is the mass within radius rr. Use this to derive the virial theorem

Egrav =3PV,E_{\text {grav }}=-3\langle P\rangle V,

where Egrav E_{\text {grav }} is the total gravitational potential energy and P\langle P\rangle the average pressure.

The total kinetic energy of a spherically symmetric star is related to P\langle P\rangle by

Ekin=αPVE_{\mathrm{kin}}=\alpha\langle P\rangle V

where α\alpha is a constant. Use the virial theorem to determine the condition on α\alpha for gravitational binding. By considering the relation between pressure and 'internal energy' UU for an ideal gas, determine α\alpha for the cases of a) an ideal gas of non-relativistic particles, b) an ideal gas of ultra-relativistic particles.

Why does your result imply a maximum mass for any star? Briefly explain what is meant by the Chandrasekhar limit.

A white dwarf is in orbit with a companion star. It slowly accretes matter from the other star until its mass exceeds the Chandrasekhar limit. Briefly explain its subsequent evolution.