We consider a new concept of weak solutions to the phase-field equations wi
th a small parameter epsilon characterizing the length of interaction. For
the standard situation of a single free interface, this concept tin contras
t with the common one) leads to the well-known Stefan-Gibbs-Thomson problem
as epsilon--> 0. For the case of a large number M(epsilon) (M(epsilon) -->
infinity as epsilon--> 0) Of free interfaces, which corresponds to the 'wa
ve-train' interpretation of a 'mushy region', this concept allows us to obt
ain the limit problem as epsilon --> 0.