This paper presents a simplified model of the process through which a
geostrophic flow enhances the vertical propagation of near-inertial ac
tivity from the mixed layer into the deeper ocean. The geostrophic flo
w is idealized as steady and barotropic with a sinusoidal dependence o
n the north-south coordinate; the corresponding streamfunction takes t
he form psi = -Psi cos(2 alpha y). Near-inertial oscillations are cons
idered in linear theory and disturbances are decomposed into horizonta
l and vertical normal modes. For this particular flow, the horizontal
modes are given in terms of Mathieu functions. The initial-value probl
em can then be solved by projecting onto this set of normal modes. A d
etailed solution is presented for the case in which the mixed layer is
set into motion as a slab. There is no initial horizontal structure i
n the model mixed layer; rather, horizontal structure, such as enhance
d near-inertial energy in regions of negative vorticity, is impressed
on the near-inertial fields by the pre-existing geostrophic flow. Many
details of the solution, such as the rate at which near-inertial acti
vity in the mixed layer decays, are controlled by the nondimensional n
umber, Upsilon = 4 Psi f(0)/(HmixNmix2)-N-2, where f(0) is the inertia
l frequency, H-mix is the mixed layer depth, and N-mix is the buoyancy
frequency immediately below the base of the mixed layer. When Upsilon
is large, near-inertial activity in the mixed layer decays on a time-
scale HmixNmix/alpha(2) Psi(3/2)f(0)(1/2). When Upsilon is small, near
-inertial activity in the mixed layer decays on a time-scale proportio
nal to (NmixHmix2)-H-2/alpha(2) Psi(2)f(0).