We discuss Einstein's field equations in the presence of signature cha
nge using variational methods, obtaining a generalization of the Lancz
os equation relating the distributional term in the stress tensor to t
he discontinuity of the extrinsic curvature. In particular, there is n
o distributional term in the stress tensor, and hence no surface layer
, precisely when the extrinsic curvature is continuous, in agreement w
ith the standard result for constant signature. (C) 1996 American Inst
itute of Physics.