Using the mobility closure given by Equation 2.57 the fluxes can be eliminated. The system of first order moment equations then becomes a system of second order equations in the even moments.
With the relaxation time approximation the general equation for is of the following form:
(2.74) |
Besides the moments which enter in the equation for are and . In addition we need for the relaxation term. Furthermore relaxation times and mobilities depend on , which needs (and ) for its calculation.
Equation 2.74 gives an infinite hierarchy of equations. If is fixed, we get the self-consistent electrical field from the Poisson equation. Then we can calculate by solving the linear Equation 2.74 (with ) for . For order this is a nonlinear equation due to the dependence of on and via the temperature.
In an infinite chain we then can solve linear equations with linear operator 2.76 to get , , and so on. The linearity is due to the exclusive dependence of and on and via the temperature. We also see that the infinite hierarchy has a solution for arbitrary chosen . This is a weakness of the model, the infinite hierarchy represents an underdetermined system of equations and is not equivalent to the full Boltzmann equation. The infinite system lacks a closure condition or constraint which picks out the ``one'' solution. In Section 3.2 we propose to apply the maximum entropy principle for this purpose.
As the infinite hierarchy is not equivalent to the Boltzmann equation it is reasonable to truncate the series at a low order . We then have to impose an additional equation for the highest occurring moment with order , to get an equal number of equations and unknowns. This closure condition is the topic of the next chapter.
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