A two-layer, deformation-forced, semigeostrophic frontogenesis model i
s presented in which the lower and upper layers represent the troposph
ere and stratosphere, respectively. The evolution of an upper-troposph
eric front and associated tropopause fold is examined after the format
ion of a discontinuity at the lower boundary. Recently developed metho
ds for extending the model beyond the time of surface frontal collapse
are used to obtain a physically consistent discontinuous solution in
the lower troposphere. The tropopause folds thus obtained are compared
to those that evolve when the model is integrated beyond the time of
collapse at the surface without regard to the unphysical nature of the
solution at low levels, Differences between the two solutions in the
vicinity of the tropopause appear to be minimal even when the upper- a
nd lower-tropospheric fronts are connected by common isentropes. This
suggests that upper-tropospheric frontogenesis is a process largely in
dependent of surface-based dynamics within the framework of the model
presented here. The related issue of the differences in lower-troposph
eric dynamics between a one-layer rigid-lid model and the two-layer mo
del is also discussed. It is found that subsidence of the tropopause i
n the two-layer model is responsible for an enhanced cross-front ageos
trophic flow at low levels. This result indicates the significance of
the upper boundary condition in SG simulations of lower-tropospheric f
rontogenesis.