Some results established in [1-4] for autonomous reversible systems ar
e extended to periodic systems that are reversible under the substitut
ion t --> -t, x --> M(-t)x, M2(t) = E (where E is the identity matrix)
, both in the non-resonant case and in the case of internal resonance.
A complete solution of the problem of stability in the first approxim
ation is derived for single-frequency resonances, which have no analog
ue in autonomous systems. It turns out that a system with one degree o
f freedom is either unstable or stable to any finite order. It is show
n that the known conditions 15] do in fact guarantee formal stability
in the rolling of a heavy, homogeneous, almost symmetric ellipsoid in
the principal plane.