Question: Consider problem 11.10, but taking E = 0 and, instead of the adiabatic case, consider a constant kinetic pressure (a) Show that the electron distribution

Consider problem 11.10, but taking E = 0 and, instead of the adiabatic case, consider a constant kinetic pressure

p = n(r) k T(r) = constant

(a) Show that the electron distribution function is given by

(b) Evaluate the heat flux vector q and show that it can be written as

where the thermal conductivity K is equal to 5kp/(2mv).

(c) What is the value of the electric current density J in this case?


Data from Problem 11.10.

An electron gas (Lorentz gas), in a background of stationary ions, is acted upon by a weak, externally applied electric field E, under steady state conditions. Using the Boltzmann equation for the electrons, with the relaxation model for the collision term (considering a constant collision frequency ν),

and considering the adiabatic case for which

show that the electron distribution function is given by

Assume that f = f0 + f1, where |f1| ≪ f0 and where f0 is the following modified Maxwellian distribution

and neglect all second-order terms in the Boltzmann equation. Consider the term involving ∇f1 as a second-order quantity.

p = n(r) k T(r) = constant

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