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Next: 35.1.6 gent_mcwilliams Up: 35.1.5 redi_diffusion Previous: 35.1.5.2 Meridional isoneutral diffusion

   
35.1.5.3 Vertical isoneutral diffusion flux

The component of the isoneutral diffusive flux through the bottom face of a T cell $diff\_fbt^{iso}_{i,k,j}$ is broken into two parts: the K33i,k,j component and the off diagonal component $diff\_fbiso_{i,k,j}$ which contains K31i,k,j and K32i,k,j pieces. The vertical diffusion operator term for tracers is also broken into two parts for isoneutral diffusion. First, the part containing $diff\_fbiso_{i,k,j}$ is solved explicitly with all other explicit components. Second, the part containing the K33i,k,j component is solved implicitly along with any other vertical diffusivity piece arising from dianeutral diffusion. The use of an implicit solver for the K33i,k,j term allows for steeper neutral direction slopes to be handled within the constraints of the linear diffusion equation stability (see Cox 1987 and Griff ies et al. 1997 for details). In the model, the vertical component is written

    $\displaystyle -F^{z}_{i,k,j} =
K^{33}_{i,k,j}\delta_{z}T_{i,k,j} + \diff\_fbiso_{i,k,j} =
K^{33}_{i,k,j}\delta_{z}T_{i,k,j}$  
  + $\displaystyle {1 \over 4 dxt_{i} \; dht_{i,k,j} } \;
\sum_{ip=0}^{1}
dxu_{i-1+i...
...lta^{(i-1+ip,k,j)}_{(i-1+ip,k+kr,j)}
\;
Ax^{(i,k+kr)}_{(i-1+ip,k+kr \vert i,k)}$  
    $\displaystyle \times \;
Sx^{(i,k+kr)}_{(i-1+ip,k+kr \vert i,k)} \; \delta_{x}T_{i-1+ip,k+kr}$  
  + $\displaystyle {1 \over 4 \cos\phi^{T}_{j} dyt_{j} \; dht_{i,k,j} } \;
\sum_{jq=...
...lta^{(i,k,j-1+jq)}_{(i,k+kr,j-1+jq)}
\; Ay^{(k+kr,j)}_{(k+kr,j-1+jq \vert k,j)}$  
    $\displaystyle \times \;
Sy^{(k+kr,j)}_{(k+kr,j-1+jq \vert k,j)} \; \delta_{y}T_{k+kr,j-1+jq}.$ (35.8)

where the non-negative diagonal component to the small angle isoneutral diffusion tensor is given by
$\displaystyle K^{33 \; small}_{i,k,j}$ = $\displaystyle {1 \over 4 dxt_{i} \; dht_{i,k,j} } \;
\sum_{ip=0}^{1}
dxu_{i-1+ip}
\times$  
    $\displaystyle \sum_{kr=0}^{1}
\Delta^{(i-1+ip,k,j)}_{(i-1+ip,k+kr,j)}
\;
Ax^{(i,k+kr)}_{(i-1+ip,k+kr \vert i,k)}
\; (Sx^{(i,k+kr)}_{(i-1+ip,k+kr \vert i,k)})^{2}$  
  + $\displaystyle {1 \over 4 \cos\phi^{T}_{j} dyt_{j} \; dht_{i,k,j} } \;
\sum_{jq=0}^{1}
\cos\phi^{U}_{j-1+jq} dyu_{j-1+jq}
\times$  
    $\displaystyle \sum_{kr=0}^{1}
\Delta^{(i,k,j-1+jq)}_{(i,k+kr,j-1+jq)}
\; Ay^{(k...
...j)}_{(k+kr,j-1+jq \vert k,j)}
\; (Sy^{(k+kr,j)}_{(k+kr,j-1+jq \vert k,j)})^{2},$ (35.9)

The contribution of this flux to the diffusion operator is given by
$\displaystyle R^{z}(T)_{i,k,j} =
\delta_{z} (\diff\_fbt^{iso}_{i,k-1,j}).$     (35.10)

Note that certain irrelevant longitudinal i and latitudinal jlabels were omitted for brevity.


next up previous contents
Next: 35.1.6 gent_mcwilliams Up: 35.1.5 redi_diffusion Previous: 35.1.5.2 Meridional isoneutral diffusion
RC Pacanowski and SM Griffies, GFDL, Jan 2000