A.7 Density limit

The maximum density that can be obtained in stable plasma operations (without disruption) is empirically given by

ne ≈ 1.5nG,
(543)

where nG is the Greenwalt density, which is given by

         I
nG = 1014--p2
        πa
(544)

where Ip is the plasma current, a is the minor radius, all physical quantities are in SI units. The 1.5nG gives the density limit that can be achieved for a tokamak operation scenario with plasma current Ip and plasma minor radius a. The Greenwalt density limit is an empirical one, which, like other empirical limits, can be exceeded in practice. Equation (544) indicates that the Greenwalt density is proportional to the current density. Therefore the ability to operate in large plasma current density means the ability to operate with high plasma density.

Note that neither the pressure limit nor the density limit is determined by the force-balance constraints. They are determined by the stability of the equilibrium. On the other hand, since the stability of the equilibrium is determined by the equilibrium itself, the pressure and density limit is determined by the equilibrium.