The Coulomb collision effect on the bounce-resonance dissipation is conside
red for toroidal magnetized plasmas. The solution of the Vlasov equation wi
th a simplified Fokker-Planck collision operator is presented. The parallel
components of the dielectric tensor are obtained. A collisionless limit of
wave dissipation is found. (C) 1999 Published by Elsevier Science B.V.