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The model domain consists of an approximately 3
km square by 1 km deep box of initially
unstratified, resting fluid. The domain is doubly periodic.
The experiment has 20 levels in the vertical, each of equal thickness
50
m (the horizontal resolution is also 50 m). The fluid is initially unstratified with a
uniform reference potential temperature
20
C. The equation of state
used in this experiment is linear
 |
(3.75) |
which is implemented in the model as a density anomaly equation
 |
(3.76) |
with
and
. Integrated forward in
this configuration the model state variable theta is equivalent to
either in-situ temperature,
, or potential temperature,
. For
consistency with other examples, in which the equation of state is
non-linear, we use
to represent temperature here. This is
the quantity that is carried in the model core equations.
As the fluid in the surface layer is cooled (at a mean rate of 800 Wm
), it becomes
convectively unstable and
overturns, at first close to the grid-scale, but, as the flow matures, on larger scales
(figures 3.13 and 3.14), under the influence of
rotation (
s
) .
Model parameters are specified in file input/data. The grid dimensions are
prescribed in code/SIZE.h. The forcing (file input/Qsurf.bin) is specified
in a binary data file generated using the Matlab script input/gendata.m.
Next: 3.15.2 Equations solved
Up: 3.15 Surface Driven Convection
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