Drift kinetic equation and neoclassical transport theory
Drift kinetic equation and neoclassical transport theory
Drift kinetic equation and neoclassical transport theory
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PHYS 7500 Plasma Transport Theory #6 c○Jeong-Young Ji 2<br />
Then the <strong>kinetic</strong> <strong>equation</strong> can be written as<br />
(L − C)f = δ −1 Ω ∂f<br />
∂γ<br />
(3)<br />
where γ is the azimuthal angle of the velocity variable along b = B/B, <strong>and</strong> δ<br />
is introduced explicitly for the perturbation expansion. Note that Ω = qB/m<br />
is the largest frequency scale in the <strong>theory</strong>.<br />
Now we exp<strong>and</strong> the distribution function as<br />
The δ −1 order <strong>equation</strong> yields<br />
f = f 0 + δf 1 + δ 2 f 2 + · · · . (4)<br />
Ω ∂f 0<br />
∂γ<br />
= 0. (5)<br />
This means that f 0 is gyrophase independent, f 0 = ¯f 0 ≡ 〈f 0 〉, where<br />
〈A(v)〉 ≡ 1<br />
2π<br />
∫ 2π<br />
0<br />
A(v)dγ (6)<br />
denotes gyroaveraging A. Here it should be emphasized that the average is taken<br />
at a fixed position x, which is different from when taken at a fixed guiding center<br />
in the gyro<strong>kinetic</strong> <strong>equation</strong>. The δ 0 -order <strong>equation</strong> is<br />
Lf 0 − C(f 0 , f 0 ) = Ω ∂f 1<br />
∂γ . (7)<br />
Its gyroaverage,<br />
¯Lf 0 − ¯C(f 0 , f 0 ) = 0, (8)<br />
provides the <strong>equation</strong> for the lowest order distribution f 0 . Then the gyrophasedependent<br />
part of f 1 can be found from (7) (with other variables suppressed):<br />
˜f 1 (γ) =<br />
1 Ω<br />
∫ γ<br />
dγ [Lf 0 − C(f 0 , f 0 )]<br />
= 1 Ω<br />
∫ γ<br />
dγ [( L − ¯L ) f 0<br />
]<br />
[use Eq. (8)]<br />
≡ L H f 0 .<br />
At this point let us investigate L to calculate ¯L. For convenience, we use<br />
u = v ‖ <strong>and</strong> s = v ⊥ ,<br />
<strong>and</strong> define the gyroradius vector ρ by<br />
ρ = b × v<br />
Ω<br />
= ρˆρ, ρ =<br />
ms<br />
|q|B ,<br />
ˆρ = s ˆρ. (9)<br />
|Ω|