Neutral atoms can significantly influence the physics of tokamak edge plasm
as, e.g., by affecting the radial electric field and plasma flow there, whi
ch may, in turn, be important for plasma confinement. Earlier work [Fulop ,
Phys. Plasmas 5, 3969 (1998)], assuming short mean-free path neutrals and
Pfirsch-Schluter ions, has shown that the ion-neutral coupling through char
ge-exchange affects the neoclassical flow velocity significantly. However,
the mean-free path of the neutrals is not always small in comparison with t
he radial scale length of densities and temperatures in the edge pedestal.
It is therefore desirable to determine what happens in the limit when the n
eutral mean-free path is comparable with the scale length. In the present w
ork a self-similar solution for the neutral distribution function allowing
for strong temperature and density variation is used, following the analysi
s of Helander and Krasheninnikov [Phys. Plasmas 3, 226 (1995)]. The self-si
milar solution is possible if the ratio of the mean-free path to the temper
ature and density scale length is constant throughout the edge plasma. The
resulting neutral distribution function is used to investigate the neutral
effects on the ion flow and electrostatic potential as this ratio varies fr
om much less than one to order unity. (C) 2001 American Institute of Physic
s.