A theory is developed for the plasma rotation in a rippled-field tokam
ak under the conditions corresponding to the banana regime. In contras
t with the previous study by Mikhailovskii [4], it is assumed that the
fast-ion beam that gives rise to the plasma rotation is absent. In th
is case, the plasma rotation is shown to be governed by the ripple-ind
uced thermal force, i.e., by the temperature-gradient dependent compon
ent of the frictional force related to collisions between the circulat
ing and locally trapped ions. The drift kinetic equation is used to de
rive analytical expressions both for the ripple-induced thermal force
and for the ''velocity'' component of this frictional force, i.e., for
the component that is proportional to the difference between the mean
velocities of the circulating and locally trapped ions. From the cond
ition that this component of the frictional force is equal to zero an
expression for the equilibrium toroidal velocity of the plasma is obta
ined.