next up previous contents
Next: 42.3.0.4 Small angle approximation Up: 42.3 Isopycnal diffusion Previous: 42.3.0.2 Orthonormal isopycnal frame

42.3.0.3 z-level frame

The orthogonal isopycnal frame allowed for a simple prescription of the isopycnal diffusion process. In order to describe such a diffusion process in other frames of reference, the components of Kmust be transformed. Such rules of transformation are standard (e.g., Aris 1962). The diagonal components $K^{\overline{m} \overline{n}}$from the orthogonal isopycnal frame are transformed to the z-level frame through

 \begin{displaymath}K^{m n} = \Lambda^{m}_{\;\; \overline{m}}
K^{\overline{m}\overline{n}}
\Lambda^{n}_{\;\; \overline{n}},
\end{displaymath} (42.48)

where the transformation matrix is given by equation (B.44). Written as matrices with $\Lambda$ having components $\Lambda^{n}_{\;\; \overline{n}}$, this transformation takes the form $K = \Lambda {\overline K} \Lambda^{T}$, where ${\overline K}$ has the diagonal form given in equation (B.45). Performing the matrix multiplication

\begin{displaymath}K^{m n} =
\left( \begin{array}{ccc}
{S_{y} \over S}
&
...
...+S^{2}}}
&
{1 \over \sqrt{1+S^{2}}}
\end{array}
\right),
\end{displaymath} (42.49)

yields the components of the diffusion tensor in the z-level system given by Redi (1982)

 \begin{displaymath}K^{m n} =
{A_{I} \over (1+S^{2})}
\left( \begin{array}{ccc...
... \over \rho_{z}}
&
\epsilon + S^{2}
\end{array}
\right),
\end{displaymath} (42.50)

which can also be written

\begin{displaymath}K^{m n} = {A_{I} \over (1+S^{2})}
\left( \begin{array}{ccc}...
...1-\epsilon)S_{y}
&
\epsilon + S^{2}
\end{array}
\right).
\end{displaymath} (42.51)

Note that Redi uses the symbol $\delta$ instead of S in her expression. The ratio of the diapycnal to isopycnal diffusivities defines the typically small number $\epsilon = A_{D}/A_{I} \approx
10^{-7}$. An equivalent form is suggested by writing the tensor in the orthonormal isopycnal frame as

\begin{displaymath}K^{\overline{m} \overline{n}} = A_{I}
\left( \begin{array}{c...
...& 0 \\
0 & 0 & 0 \\
0 & 0 & 1 \\
\end{array}
\right),
\end{displaymath} (42.52)

which separates the effects of the anisotropy between the along and across isopycnal directions. This expression can be written in the compact form

 \begin{displaymath}K^{ \overline{m} \overline{n} } =
K_{ \overline{m} \overline...
...})_{\overline{m}}(\vec{e}_{\overline{3}})_{\overline{n}} \; ,
\end{displaymath} (42.53)

as noted in equation (B.46). Transforming to the z-level frame yields

\begin{displaymath}K^{m n} = A_{I}
\left( \begin{array}{ccc}
1 & 0 & 0 \\
0 ...
...{z} & \rho_{y}\rho_{z} & \rho_{z}^{2}
\end{array}
\right),
\end{displaymath} (42.54)

which can also be written

 \begin{displaymath}K^{m n} = K_{m n} = A_{I} \delta_{m n} +
A_{I}(\epsilon-1)
...
...\rho}_{m}\hat{\rho}_{n})
+A_{D}\hat{\rho}_{m}\hat{\rho}_{n},
\end{displaymath} (42.55)

where $\hat{\rho}_{m}=\partial_{m}\rho/\vert\nabla \rho\vert$ are the components of the diapycnal unit vector ${\vec{e}}_{\overline{3}}$written in the z-level frame [see equation (B.43)]. Note that equation (B.55) could have been written down immediately once equation (B.53) was hypothesized, and the unit vectors (B.41), (B.42), and (B.43) were determined.


next up previous contents
Next: 42.3.0.4 Small angle approximation Up: 42.3 Isopycnal diffusion Previous: 42.3.0.2 Orthonormal isopycnal frame
RC Pacanowski and SM Griffies, GFDL, Jan 2000