Abstract
It is shown that, for a Tokamak plasma with fixed boundary, the toroidal contributions to the shear are sufficiently important to modify the j-kink instability. Assuming that β is small and using the energy principle, δW is calculated to order (rR)6 and the toroidal corrections are shown to change the sign of the destabilizing term. One consequence is that the range of rotational transform angles for which the m=1, ν=1 instability will occur, when the shear is weak, is below the Kruskal-Shafranov limit and not above it. Also, the new terms have an important stabilizing effect for the screw pinch.