We study turbulent transport of passive tracers by random wave fields of a
rather general nature. A formalism allowing for spatial inhomogeneity and a
nisotropy of an underlying velocity field (such as that caused by a latitud
inally varying Coriolis parameter) is developed, with the aim of treating p
roblems of large-scale ocean transport by long internal waves. For the spec
ial case of surface gravity waves on deep water, our results agree with the
earlier theory of Herterich & Hasselmann (1982), though even in that case
we discover additional, off-diagonal elements of the diffusion tensor emerg
ing in the presence of a mean drift. An advective diffusion equation includ
ing all components of the diffusion tensor D plus a mean, Stokes-type drift
u is derived and applied to the case of baroclinic inertia-gravity (BIG) w
aves. This application is of particular interest for ocean circulation and
climate modelling, as the mean drift, according to our estimates, is compar
able to ocean interior currents; Furthermore, while on the largest (100 km
and greater) scales, wave-induced diffusion is found to be generally small
compared to classical eddy-induced diffusion, the two become comparable on
scales below 10 km. These scales are near the present limit on the spatial
resolution of eddy-resolving ocean numerical models. Since we find that u(z
) and D-zz vanish identically, net vertical transport is absent in wave sys
tems of this type. However, for anisotropic wave spectra the diffusion tens
or can have non-zero off-diagonal vertical elements, D-xz and D-yz, and it
is shown that their presence leads to non-positive definiteness of D, and a
negative diffusion constant is found along a particular principal axis. Ho
wever, the simultaneous presence of a depth-dependent mean horizontal drift
rc(z) eliminates any potential unphysical behaviour.