A new formulation of the toroidal, finite beta, resistive tearing stab
ility problem is presented. As in standard tearing mode theory, the mo
de structure throughout most of the configuration is deter-mined by an
ideal, inertia-free model. Thus, it is very closely related to that o
btained from standard ideal magnetohydrodynamic (MHD) numerical stabil
ity programs that depend on an energy principle. The effects of inerti
a, resistivity, and any other plasma properties are important only in
thin layers enclosing resonant surfaces. These surfaces are distinguis
hed by the fact that they are composed of closed field lines. Instabil
ity growth rates are obtained from the condition of matching between t
he inner and outer regions. The data needed from the outer region for
matching are conventionally reduced to a quantity DELTA', but in toroi
dally coupled axisymmetric systems the relevant quantity is a matrix.
A previous paper [Pletzer and Dewar, J. Plasma Phys. 45, 427 (1991)] p
resented a relation between an extension of the ideal energy and the i
nformation from the outer region that is needed in matching to the inn
er layers. Here, this is used to construct a relation for the tearing
mode growth rates directly in terms of an extension of the ideal energ
y matrix. This demonstrates a convenient way to extend the numerical p
rograms for ideal stability to include stability against tearing modes
.