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UKMO
GOSI
GOSI9esm
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9983cfc2
Commit
9983cfc2
authored
3 years ago
by
Stefania Ciliberti
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revised text for dynspg_exp and dynspg_ts
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doc/latex/NEMO/subfiles/chap_DYN.tex
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doc/latex/NEMO/subfiles/chap_DYN.tex
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9983cfc2
...
@@ -793,11 +793,11 @@ so that the update of the next velocities is done in module \mdl{dynspg\_flt} an
...
@@ -793,11 +793,11 @@ so that the update of the next velocities is done in module \mdl{dynspg\_flt} an
The form of the surface pressure gradient term depends on how the user wants to
The form of the surface pressure gradient term depends on how the user wants to
handle the fast external gravity waves that are a solution of the analytical equation (
\autoref
{
sec:MB
_
hor
_
pg
}
).
handle the fast external gravity waves that are a solution of the analytical equation (
\autoref
{
sec:MB
_
hor
_
pg
}
).
T
hree
formulations are available, all controlled by a CPP key (ln
\_
dynspg
\_
xxx
):
T
wo
formulations are available, all controlled by a CPP key (ln
\_
dynspg
\_
<method>
):
an explicit formulation which requires a small time step;
an explicit formulation which requires a small time step;
a filtered free surface formulation which allows a larger time step by
%
a filtered free surface formulation which allows a larger time step by
adding a filtering term into the momentum equation;
%
adding a filtering term into the momentum equation;
and
a split-explicit free surface formulation
, described below,
which also allows a larger time step.
a split-explicit free surface formulation which also allows a larger time step.
The extra term introduced in the filtered method is calculated implicitly, so that a solver is used to compute it.
The extra term introduced in the filtered method is calculated implicitly, so that a solver is used to compute it.
As a consequence the update of the
$
next
$
velocities is done in module
\mdl
{
dynspg
\_
flt
}
and not in
\mdl
{
dynnxt
}
.
As a consequence the update of the
$
next
$
velocities is done in module
\mdl
{
dynspg
\_
flt
}
and not in
\mdl
{
dynnxt
}
.
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