A3.14

Statistical Physics and Cosmology | Part II, 2002

(i) Write down the first law of thermodynamics for the change dUd U in the internal energy U(N,V,S)U(N, V, S) of a gas of NN particles in a volume VV with entropy SS.

Given that

PV=(γ1)U,P V=(\gamma-1) U,

where PP is the pressure, use the first law to show that PVγP V^{\gamma} is constant at constant NN and

Write down the Boyle-Charles law for a non-relativistic ideal gas and hence deduce that the temperature TT is proportional to V1γV^{1-\gamma} at constant NN and SS.

State the principle of equipartition of energy and use it to deduce that

U=32NkTU=\frac{3}{2} N k T

Hence deduce the value of γ\gamma. Show that this value of γ\gamma is such that the ratio Ei/kTE_{i} / k T is unchanged by a change of volume at constant NN and SS, where EiE_{i} is the energy of the ii-th one particle eigenstate of a non-relativistic ideal gas.

(ii) A classical gas of non-relativistic particles of mass mm at absolute temperature TT and number density nn has a chemical potential

μ=mc2kTln(gsn(mkT2π2)32)\mu=m c^{2}-k T \ln \left(\frac{g_{s}}{n}\left(\frac{m k T}{2 \pi \hbar^{2}}\right)^{\frac{3}{2}}\right)

where gsg_{s} is the particle's spin degeneracy factor. What condition on nn is needed for the validity of this formula and why?

Thermal and chemical equilibrium between two species of non-relativistic particles aa and bb is maintained by the reaction

a+αb+βa+\alpha \leftrightarrow b+\beta

where α\alpha and β\beta are massless particles with zero chemical potential. Given that particles aa and bb have masses mam_{a} and mbm_{b} respectively, but equal spin degeneracy factors, find the number density ratio na/nbn_{a} / n_{b} as a function of ma,mbm_{a}, m_{b} and TT. Given that ma>mbm_{a}>m_{b} but mambmbm_{a}-m_{b} \ll m_{b} show that

nanbf((mamb)c2kT)\frac{n_{a}}{n_{b}} \approx f\left(\frac{\left(m_{a}-m_{b}\right) c^{2}}{k T}\right)

for some function ff which you should determine.

Explain how a reaction of the above type is relevant to a determination of the neutron to proton ratio in the early universe and why this ratio does not fall rapidly to zero as the universe cools. Explain briefly the process of primordial nucleosynthesis by which neutrons are converted into stable helium nuclei. Let

YHe=ρHeρY_{H e}=\frac{\rho_{H e}}{\rho}

be the fraction of the universe that ends up in helium. Compute YHeY_{H e} as a function of the ratio r=na/nbr=n_{a} / n_{b} at the time of nucleosynthesis.

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