Boltzmann equation and thermal conductivity. Consider a medium with temperature gradient dτ/dx. The particle concentration is constant. (a) Employ the Boltzmann transport equation in the relaxation time approximation to find the first order nonequilibrium classical distribution:
f≃f0−vxτc(−2τ3+τ2ε)f0dxdτ.(125)
(b) Show that the energy flux in the x direction is
Ju=−(dxdτ)τc∫vx2(−2τ3ε+τ2ε2)f0D(ε)dε,(126)
where vx2=2ε/3m. (c) Evaluate the integral to obtain for the thermal conductivity K=5nττc/m.