In cosmological first-order phase transitions, the microscopic interaction of
the phase transition fronts with non-equilibrium plasma particles manifests
itself macroscopically as friction forces. In general, it is a nontrivial
problem to compute these forces, and only two limits have been studied, namely,
that of very slow walls and, more recently, ultra-relativistic walls which run
away. In this paper we consider ultra-relativistic velocities and show that
stationary solutions still exist when the parameters allow the existence of
runaway walls. Hence, we discuss the necessary and sufficient conditions for
the fronts to actually run away. We also propose a phenomenological model for
the friction, which interpolates between the non-relativistic and
ultra-relativistic values. Thus, the friction depends on two friction
coefficients which can be calculated for specific models. We then study the
velocity of phase transition fronts as a function of the friction parameters,
the thermodynamic parameters, and the amount of supercooling.Comment: 34 pages, 7 figures. v2: minor correction