Option neptune implements the following. Based on statistical
mechanics arguments, Holloway (1992) proposed that interaction between
mesoscale eddies and topography results in a stress on the ocean with
two important consequences: first, the ocean is not driven towards a
state of rest and secondly, the resulting motion may have scales much
larger than the scale of the eddies. Somewhat suprisingly, this
interaction36.1 can generate coherent mean flows
on the scale of the topography. The magnitude of this topographic
stress is dependent on the correlation between pressure p and
topographic gradients
which is largely unknown but even if
the correlation is 0.1, the resulting topographic stress would be
comparable in magnitude to that of the surface wind.
If the view is taken that equations of motion are solved for moments of
probable flow (because of imperfect resolution) then those moments are
forced in part by derivatives of the distribution entropy with respect
to the realized moments. The entropy gradient is estimated as begin
proportional to a departure of the realized moments from a state in
which the entropy gradient is weak. This latter state is approximated
by a transport streamfunction
and maximum entropy velocity
given by
| = | (36.1) | ||
| = | (36.2) |
where f is the Coriolis term, H is depth, and
is O (10 km). If model resolution is coarse relative to the first
deformation radius,
is independent of depth. Instead of eddy
viscosity driving flow towards rest, flow is driven towards
using an eddy viscosity of the form
.
Note
that topographic influence on flow36.2 is not strongest near bottom topography. Instead, the flow
implied by
only approximates a maximum entropy system
given eddies and topography. Since this approximation is admittedly
crude, further refinements are open to researchers.
There is legitimate concern about the stepwise resolution of bottom topography in level models such as MOM and its predecessors. Option neptune is an attempt to instruct the model about physical consequences due to topography and eddies which are nearly unachievable even at the most ambitious resolutions. The hope is that if the model can be suitably informed about the effect of topography, it matters little if that topography is only ``approximately'' represented.