  We review and extend to include the gauge fields our derivation of the
semiclassical limit of the collisionless quantum transport equations for the
fermions in presence of a CP-violating bubble wall at a first order electroweak
phase transition. We show how the (gradient correction modified) Lorenz-force
appears both in the Schwinger-Keldysh approach and in the semiclassical
WKB-treatment. In the latter approach the inclusion of gauge fields removes the
apparent phase reparametrization dependence of the intermediate calculations.
We also discuss setting up the fluid equations for practical calculations in
electroweak baryogenesis including the self-consistent (hyper)electric field
and the anomaly.
