The natural structure for smectic-A liquid crystals arranged in a sample wi
th homogeneous boundary conditions is the so-called bookshelf structure wit
h uniform layers perpendicular to the sample cell plane. However, this stru
cture often deforms into the so-called chevron structure when the sample is
cooled. This deformation is usually thought to result from the mismatch be
tween bulk and surface layer thicknesses. In this paper we study the dynami
cs of chevron formation. Two possible scenarios are envisage. In one of the
se there is strong coupling between layer deformation and fluid flow, and i
n the other the fluid essentially does not move. In this paper we examine t
he first scenario, leaving the second, slower relaxation mode for another p
aper. Analytic solutions are found for near-critical deformations, and nume
rical solutions are found beyond the critical regime. [S1063-651X(98)06912-
8].