A steady fission-like neutron source of strength sits inside a large block of beryllium

PHYSICS · Multi-part · Fermi University Physics · Nuclear Physics · Nuclear reactions · Nuclear reactions

The Nucleus Resolved, Ch Neutrons: the reagent with no barrier

Problem

A steady fission-like neutron source of strength S=8.0×104 cm−3 s−1S = 8.0\times10^{4}\,\mathrm{cm^{-3}\,s^{-1}} sits inside a large block of beryllium, treated as an infinite, non-absorbing, uniform moderator with ξΣs=0.154 cm−1\xi\Sigma_s = 0.154\,\mathrm{cm^{-1}}. ((a)) From a lethargy balance, derive the flux spectrum ϕ(E)\phi(E) below the source energy and evaluate it at E=2.0 eVE = 2.0\,\mathrm{eV}. ((b)) A tritium-breeding tile containing lithium-6, whose (n,α)(n,\alpha) cross section follows the 1/v1/v law with σ0=940 b\sigma_0 = 940\,\mathrm{b} at v0=2200 m s−1v_0 = 2200\,\mathrm{m\,s^{-1}}, sits where the neutrons have thermalised into a Maxwellian at temperature TT. Using the flux-weighted average σˉ(T)=(π/2)(T0/T)1/2σ0\bar\sigma(T) = (\sqrt\pi/2)(T_0/T)^{1/2}\sigma_0 (with T0=293.6 KT_0 = 293.6\,\mathrm{K}) and the mean speed vˉ(T)=(2/π)v0(T/T0)1/2\bar v(T) = (2/\sqrt\pi)v_0(T/T_0)^{1/2}, derive algebraically that the product vˉ(T)σˉ(T)\bar v(T)\bar\sigma(T) equals v0σ0v_0\sigma_0 for every TT, and hence that the tritium-production rate per lithium-6 atom, nvˉ(T)σˉ(T)n\bar v(T)\bar\sigma(T), is temperature-independent. Evaluate vˉ\bar v and σˉ\bar\sigma at T=600 KT = 600\,\mathrm{K} and check the product against v0σ0v_0\sigma_0.

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