A three magnetic field component sheared plasma sheet equilibrium mode
l is developed in the context of ideal magnetohydrodynamics (MHD). It
is argued that MHD stability theory may be sufficiently correct for a
thin sheet if the shear in the magnetic field is large enough. Using t
he model magnetic held, the ballooning eigenvalue equation is solved f
or several different values of equilibrium parameters. It is shown tha
t for sufficiently large values of the shear parameter, the model is u
nstable to symmetric ballooning modes with a growth rate on the order
of one tenth the Alfven rate.