It is shown that besides the ion orbit loss mechanism, which occurs in
a region a - epsilon(t) rho(p) < r < a, the drift-orbit transport flu
x driven by the collisionless helically trapped particles can also dri
ve the poloidal (E) over right arrow x (B) over right arrow velocity i
n a region r < a - epsilon(t) rho(p) in stellarators. Here, r(a) is th
e minor (plasma) radius, epsilon(t) is the toroidal amplitude of the m
agnetic field spectrum, (E) over right arrow((B) over right arrow) is
the electric (magnetic) field, and rho(p) is the poloidal ion gyroradi
us. The transport flux-driven (E) over right arrow x (B) over right ar
row velocity can be triggered most efficiently by an increase of the i
on temperature gradient. The theory is applied to the high-mode phenom
enon observed in stellarators.