We calculate the velocity and thickness of a bubble wall at the electr
oweak phase transition in the minimal standard model. We model the wal
l with semiclassical equations of motion and show that friction arises
from the deviation of massive particle populations from thermal equil
ibrium. We treat these with Boltzmann equations in a fluid approximati
on. Our technique allows us to account for particle transport, and to
determine the wall thickness dynamically. We find that the wall is sig
nificantly thicker than at phase equilibrium, and that the velocity is
fairly high, upsilon(W) similar or equal to 0.6c for m(H) = 50 GeV.