Steadily propagating monopole vortex solutions to the eta(i)-mode equa
tions are investigated. A general condition for non-linear vortex solu
tions to be steadily propagating is derived by demanding that their ve
locity is outside the regime of linear-wave propagation. The velocity
of the vortex is determined by the ratio of the pressure perturbation
and the electrostatic potential. Numerical studies show that such vort
ices generally emerge from localized initial conditions. A new type of
vortex interaction is also revealed.