80 Chapter 3. Motion of a single plasma particlê
R̂
R
B
center of curvatureFigure 3.5: Local cylindrical coordinate system defined by curved magnetic field,ˆφ=B.ˆ
The drifts can be summarized asv⊥gc=vE+v∇B+vc+vP (3.87)
where- the ‘EcrossB’ drift is
vE=
E×B
B^2
(3.88)
- the ‘gradB’ drift is
v∇B=−
mv^2 L 0
2 qB^3
∇B×B (3.89)
- the ‘curvature’ drift is
vc=−mv‖^2 gc
qB^2B̂·∇B̂×B=^1
qB^2(
mv‖^2 gcRˆ
R)
×B (3.90)
- the ‘polarization’ drift is
vP=−
m
qB^2[
d
dt(vE+v∇B+vc)