2 Plasma current density in terms of Ψ and g

When the displacement current term is neglectable (the case we consider in this note), the conductive current is just another representation of the magnetic field. Specifically, the current density can be written in terms of the magnetic field as (Ampère’s law):

                                    (           )
μ0J = ∇ ×B  = − ∂B-ϕˆR + 1-∂(RB-ϕ)ˆZ + ∂BR- − ∂BZ-  ˆϕ.
                ∂Z     R   ∂R         ∂Z    ∂R
(49)

  2.1 Poloidal current density
  2.2 Toroidal current density