Environmental Engineering Reference
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can differ remarkably from the Maxwell one. On the other hand, the analysis of the
electron behavior is simplified because of a small mass compared with the mass of
other atomic particles in a gas. This allows one to represent the integral of electron-
atom collisions in the analytical form, as (3.12) and (3.18) for the collision integral
in the case of elastic electron-atom collisions. Formula (3.26) gives the electron
drift velocity in a gas in external fields with elastic collisions between electrons
and atoms. We now derive the expression for the transverse diffusion coefficient of
electrons in a gas under these conditions.
By definition, the diffusion coefficient of electrons D e connects the electron num-
ber density gradient r N e and the electron flux j e by the relation
j e
D
D e r
N e .
On the other hand, the kinetic equation for the electron distribution function has
the following form if the electron number density varies in space:
r
f
D
I ea ( f ),
v x
where I ea is the integral of electron-atom collisions. We take the electron distribu-
tion function in the standard form (3.10)
f
D
f 0 ( v )
C v
x f 1 ( v ),
where the x -axis is directed along the gradient of the electron number density.
Because the distribution function is normalized to the electron number density
f
N e / N e , and the kinetic equation for the electron dis-
tribution function takes the form
N e ,wehave
r
f
D
f
r
x f 0
N e
N e D ν v x f 1
r
v
if we use (3.12) for the collision integral taking into account elastic electron-atom
collisions. From this we obtain for the nonsymmetric part of the electron distribu-
tion function
f 0
r
N e
f 1
D
.
ν
N e
This leads to the following expression for the electron flux:
N e R v
Z
Z
N e v
,
x f 0 d v
x
ν
x f 1 d v D r
2
j e
D
v fd v D
D r
v
ν
N e
where angle brackets mean averaging over the electron distribution function. Com-
paring this formula with the definition of the diffusion coefficient according to the
equation j e
D
D e r
N e , we find for the diffusion coefficient of electrons in a gas
v
.
2
D e
D
3
ν
 
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