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Next: 35.1.4 Some caveats and Up: 35.1 Basic isoneutral schemes Previous: 35.1.2 Summary of the

35.1.3 Summary of the options and namelist parameters

Option isoneutralmix is referred to as a hybrid mixing scheme since it only mixes tracers, not momentum. One basic horizontal mixing scheme (e.g. option consthmix) and one basic vertical mixing scheme (e.g. option constvmix) must also be enabled for use with option isoneutralmix. Optionsredi_diffusion, gent_mcwilliams, and biharmonic_rm are the three main sub-options to option isoneutralmix. Enabling either of these three sub-options will automatically enable isoneutralmix. There is one other sub-option, diff_nonconstant, which is described in Section 34.2.

For conceptual orientation, the combined mixing tensor which defines the default tracer fluxes arising from redi_diffusion, gent_mcwilliams, and biharmonic_rm takes the form

 
$\displaystyle J^{mn} =
\left( \begin{array}{ccc}
A_{I} & 0 & (A_{I}-\kappa + B ...
...a -B \, \nabla_{h}^{2}) \, S_{y} &
(A_{I} \, S^{2} + A_{D})
\end{array}\right),$     (35.1)

where AI is the along isoneutral diffusivity, $\kappa$ is the GM90 diffusivity, B is the RM98 biharmonic diffusivity, Sx and Sy are the isoneutral slopes in the x and y directions, respectively, S2 = Sx2 + Sy2, AD is the dianeutral diffusivity, approximated here as vertical diffusion, and $\nabla_{h}^{2}$ is the horizontal Laplacian operator. This tensor represents the sum of the symmetric small angle isoneutral diffusion tensor, the anti-symmetric GM90 tensor, and the anti-symmetric RM98 tensor. The central goals of the numerical algorithms are to discretize the tracer fluxes arsing from this tensor in a numerically stable and physically consistent fashion. It is believed that the current algorithms in MOM provide a workable approximation to these two goals.

1.
Option redi_diffusion enables the Redi isoneutral diffusion process. There are two sub-options for  redi_diffusion.

For the small tensor, and for most parameter ranges of the full tensor, some form of tapering is required in order to scale to zero the along isoneutral diffusivity as the slope increases. There are two options for implementing this tapering.

If one uses a mixed layer scheme such as option kppvmix (Section 32.2.3), it might be useful to compute horizontal tracer fluxes within the boundary layer using the same horizontal diffusivity as used to compute vertical tracer fluxes. Option isotropic_mixed (Section 34.1.9.3) enables this choice to be made in MOM.

The namelist parameters (refer to Section 14.4 for information on namelist variables) for  redi_diffusion are the following:

In order to obtain the standard small slope tensor using the Gerdes et al. (1991) form for tapering, the option redi_diffusion is all that is needed. Default options small_tensor and gkw_taper are automatically enabled. Setting the alternatives will override these defaults.

2.
Option gent_mcwilliams enables the GM90 adiabatic stirring process. There are two sub-options for gent_mcwilliams.

The namelist parameter for  gent_mcwilliams is the following:

Just as for the isoneutral diffusion scheme, it is necessary to scale the GM90 diffusivity to zero as the isoneutral slope increases. The same options, with the same maximum slope slmx, are used here as for isoneutral diffusion.

In order to obtain the standard gent_mcwilliams scheme, employing skew-fluxes and the Gerdes et al. (1991) form for tapering, the option gent_mcwilliams is all that is needed. Default options gm_skew and gkw_taper are automatically enabled. Setting the alternatives will override these defaults.

3.
Option biharmonic_rm (Section 34.1.8) enables the RM98 adiabatic biharmonic operator in terms of skew-fluxes. There are no sub-options for biharmonic_rm. The namelist parameter is

Just as for the isoneutral diffusion scheme, it is necessary to scale the RM98 diffusivity to zero as the isoneutral slope increases. The same options, with the same maximum slope slmx, are used here as for isoneutral diffusion.

4.
Option diff_nonconstant enables one of the mesoscale eddy closures for use in producing an eddy diffusivity which is a function of space and time. This option is described in Section 34.2.


next up previous contents
Next: 35.1.4 Some caveats and Up: 35.1 Basic isoneutral schemes Previous: 35.1.2 Summary of the
RC Pacanowski and SM Griffies, GFDL, Jan 2000