The effect of a temperature gradient on neoclassical ideal internal m
= 1 kink modes is studied theoretically. The ideal MHD instability of
these modes is assumed to be suppressed by the effects of the finite i
on Larmor radius. A study is made of the growth (or damping) of these
modes caused by collisional dissipation due to circulating ions. The m
ode with a frequency close to that of the ion drift, which is unstable
in the case of a uniform temperature of the plasma, is shown to damp
when the ion-temperature gradient is not too small. It is noted that t
his mode is similar to the fishbone oscillations excited by the energe
tic ions.