A neoclassical theory of poloidal rotation in tokamaks is developed for rf-
heated plasmas. It is based on a moment expansion but, in contrast to the u
sual neoclassical theory, which takes into account the strong deformation o
f the local equilibrium distribution function due to rf heating. This distr
ibution function is the solution, in the banana regime, of the drift kineti
c equation, which includes both collisional diffusion and quasilinear rf di
ffusion operators. The set of closed, self-consistent transport and rotatio
n equations is obtained in a form similar to its usual neoclassical counter
part. The parallel components of the generalized stress tensors are calcula
ted. This allows us to solve the transport equations for the poloidal rotat
ion that is obtained in explicit form. Modifications of the poloidal rotati
on due to the rf heating are also discussed. (C) 2001 American Institute of
Physics.