Effect of edge transport barrier on required toroidal field for ignition of elongated tokamak
Yang Cui-Kun1, 2, †, Chu Ming-Sheng1, Guo Wen-Feng1
       

Comparisons among variations of marginal BT required for all models at ignition relative to the ‘I’ model for an aspect ration A = 3 plasma, with edge parameter h (see Eqs. (10) and (12)). In order to accommodate all models in the same figure, we also used h to denote l ± 1 . (see Eq. (14)) for the ‘GB’ (broader) and ‘GP’ (more peaked) models. Panel (a) is the change of BT in unit of T, and panel (b) is the change relative to that of the ‘I’ model (see Eq. (4)).