526 Appendix C
Ion acoustic velocity (p.(4.33))
cs=√
κTe
mi=9. 8 × 103
√
Te
A
m s−^1Electron diamagnetic drift velocity (p.250)
ud,e=
κT
eB∣
∣
∣
∣
1
n∇n∣
∣
∣
∣=
Te
B∣
∣
∣
∣
1
n∇n∣
∣
∣
∣m s− 1Ion diamagnetic drift velocity (flow in opposite direction from electrons, (p.250)
ud,e=κTi
qiB∣
∣
∣
∣
1
n∇n∣
∣
∣
∣=
Ti
ZB∣
∣
∣
∣
1
n∇n∣
∣
∣
∣m s− 1Alfvén velocity (p.132)
vA=B
√
μ 0 nimi=
B
√
μ 0 neAmp/Z=2. 2 × 1016 B
√
Z
neAm s−^1Wave phase velocity (p.202)
vph=ω
k=fλDimensionless
Plasma beta (p.319)
β=
2 μ 0 nκT
B^2=
4. 0267 × 10 −^25
B^2
nTLundquist number (p.381)
S=μ 0 vAL
ηCollisions, resistivity, and runawaysElectron-electron collision rate (p.21)
νee=4× 10 −^12nlnΛ
TeV^3 /^2s−^1wherelnΛ∼ 10 , electron-ion rate same magnitude, ion-ion slower by
√
me/miSpitzer resistivity (p.394)
η=1. 03 × 10 −^4ZlnΛ
Te^3 /^2Ohm-m