The magnetoconductivity sigma(B) of a classical 2D electron crystal on
superfluid He-4 is non-linear. Experimentally we find a contribution
to sigma(B) which, at constant field, gives sigma(B) proportional to J
(x), the current density, while at constant current, sigma(B) proporti
onal to 1/B. In this region the Hall velocity v(H) slowly approaches t
he ripplon velocity v(1) at the first reciprocal lattice vector, due t
o strong electron-ripplon interactions with the helium. The magnetocon
ductivity decreases sharply for v(H) > v(1). Fluctuations in sigma(B)
are seen above the melting temperature.