A new exact solution is obtained for an axisymmetric MHD configuration
with stationary plasma flows. The solution is found under the assumpt
ion that the dependence of velocity potential G (or Mach number M-a) o
n magnetic potential Psi has a general form, i.e., it is an arbitrary
differentiable function G(Psi). As in the static case, the solution fo
und is self-similar because of the self-similar variable of the form t
= r(2)/omega(z). It is shown that stationary plasma flows do not affe
ct the geometric shape of the magnetic surfaces; however, they do affe
ct the radial magnetic-field distribution: B-z similar to B-r similar
to 1/root\1 - M-a(2)\. Possible applications of the solution obtained,
in particular, to sunspots, are discussed.