The evolution of a steady stratified along-isobath current flowing cyc
lonically (shallower water on the right looking downstream) over a slo
ping frictional bottom is examined using an idealized model. The flow
is assumed to consist of an inviscid vertically uniform geostrophic in
terior above a bottom boundary layer in which density is vertically we
ll mixed. Within the bottom boundary layer, vertical shear in the hori
zontal velocities is assumed to result only from horizontal density gr
adients. Density advection is included in the model, but momentum adve
ction is not. The downstream evolution of the current is described by
two coupled nonlinear partial differential equations for surface press
ure and boundary layer thickness, each of which is first order in the
along-isobath coordinate and can be easily integrated numerically. An
initially narrow along-isobath current over a uniformly sloping bottom
spreads and slows rapidly owing to the effects of bottom friction, mu
ch like the unstratified case. However, as the bottom boundary layer g
rows, the resulting horizontal density gradients reduce the bottom vel
ocity, which in turn, decreases both the transport in the bottom bound
ary layer and the spreading of the current. An equilibrium is reached
downstream in which the bottom velocity vanishes everywhere and the cu
rrent stops spreading. This equilibrium flow persists indefinitely des
pite the presence of a frictional bottom. The width of the equilibrium
current scales as W similar to (f/N alpha)(F-0/f)(1/2), where f is is
the Coriolis parameter, N the buoyancy frequency, alpha the bottom sl
ope, and F-0 the inflow volume flux per unit depth. The thickness of t
he bottom boundary layer scales as alpha W, while the along-isobath ve
locity scales as (N alpha/f)(F(0)f)(1/2). Surprisingly, the downstream
equilibrium flow is independent of the magnitude of bottom friction.
Good approximations for the equilibrium scales are obtained analytical
ly by imposing conservation of mass and buoyancy transports. Generaliz
ations to variable bottom slope, nonuniform stratification, and coasta
l currents are also presented.