We present a new class of exact solutions of the steady axisymmetric M
HD equations relevant for stellar winds. The geometry of the streamlin
es and fieldlines is helicoidal. All quantities depend both on distanc
e to the central object and on latitude. A technique based on a nonlin
ear separation of variables yields the most general solution which dep
ends on latitude vis three anisotropy parameters. These are related to
typical values of the different quantities st the base of the outflow
. We are thus able to model a wide range of winds from almost spherica
lly symmetric to highly anisotropic ones. Topologically, there are two
critical points present in the solution for the radial dependence of
the outflow speed. One appears at the familiar star-point Alfvenic sin
gularity while the other is at the X-type singularity where the radial
how speed equals the fast MHD wave speed in the radial direction. A u
nique solution corresponding to zero pressure at infinity must pass th
rough both these two points. For the wind to be able to accelerate to
large distances, the density at the equator must exceed the density at
the pole. In these circumstances, the polar speed is always greater t
han the equatorial one. This trend is confirmed by the Ulysses data on
the heliolatitudinal dependence of the solar wind as well by interpla
netary scintillation data.