Thermal Physics · Problem 5

Kinetic Theory — Charles Kittel & Herbert Kroemer

Physics — Statistical Mechanics · boltzmann-equation-thermal-conductivity

Problem

Boltzmann equation and thermal conductivity. Consider a medium with temperature gradient dτ/dxd\tau/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(−32τ+ετ2)f0dτdx.(125)f \simeq f_0 - v_x \tau_c \left(-\frac{3}{2\tau} + \frac{\varepsilon}{\tau^2}\right) f_0 \frac{d\tau}{dx}. \tag{125} (b) Show that the energy flux in the xx direction is Ju=−(dτdx)τc∫vx2(−3ε2τ+ε2τ2)f0D(ε)dε ,(126)J_u = -\left(\frac{d\tau}{dx}\right) \tau_c \int v_x^2 \left(-\frac{3\varepsilon}{2\tau} + \frac{\varepsilon^2}{\tau^2}\right) f_0 \mathfrak{D}(\varepsilon) d\varepsilon\,, \tag{126} where vx2=2ε/3mv_x^2 = 2\varepsilon/3m. (c) Evaluate the integral to obtain for the thermal conductivity K=5nττc/mK = 5n\tau\tau_c/m.

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