“…In these equations, L| is the length of the field line (L| = 7rRo/m + £ d and L| = 7rRoq/m + £ d /sin<£ in the poloidal and toroidal configurations, respectively; for limiter discharges, £ d need not be added), xi is the coefficient of longitudinal heat conductivity (we assume the classical Spitzer coefficient xi = 2 x 10 20 T s 5/2 ), X, = 2 X 10 12 T 2 /n s is the path length of the electrons, the coefficient a (the flux limit factor [20], a ~ 3-10) describes the drop in heat flux for X|/L| > 1, T d is the plasma temperature at the divertor plates, 0 ~ 1.6 is a coefficient to allow for the distortion of the distribution function near the plates [17,21], S s = 27rRo27rak is the area of the magnetic surface bounded by the separatrix, Xx = 7D Bohm , 7 is a coefficient of ~3 -8 , Wj is the fraction of energy lost through ionization in the divertor channel and W ;i is the fraction of energy lost through ionization at the plates. W takes into account both losses through ionization of the main gas, which for hydrogen and deuterium can be estimated by the formula (see Ref.…”