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List of Tables
7.1
Ohmic conductivity as function of the e-e collision model
7.2
Ohmic conductivity as function of the effective charge using the linearized e-e collision model
7.3
Runaway rate as function of the effective charge using the Maxwellian e-e collision model
7.4
Runaway rate as function of the collision model. Calculations are performed with bounce-averaging, which reduce
Γ
R
by 21% as compared to data given in Table 7.3, for similar plasma parameters.
7.5
Lower Hybrid current drive efficiencies
η
LH
in a pure hydrogen plasma from various 2
-
D
relativistic Fokker-Planck codes
7.6
Lower Hybrid current drive efficiencies (
A
⋅
m∕W
) in a pure hydrogen plasma from various 2
-
D
relativistic Fokker-Planck codes
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