16 |
|
|
17 |
%---------------------------------------------------------------------- |
%---------------------------------------------------------------------- |
18 |
\subsubsection{Introduction |
\subsubsection{Introduction |
19 |
\label{sec:pkg:exf:intro}} |
\label{sec:pkg:seaice:intro}} |
20 |
|
|
21 |
|
|
22 |
Package ``seaice'' provides a dynamic and thermodynamic interactive |
Package ``seaice'' provides a dynamic and thermodynamic interactive |
58 |
no additional CPP options are required. |
no additional CPP options are required. |
59 |
% |
% |
60 |
\end{itemize} |
\end{itemize} |
61 |
(see Section \ref{sect:buildingCode}). |
(see Section \ref{sec:buildingCode}). |
62 |
|
|
63 |
Parts of the SEAICE code can be enabled or disabled at compile time |
Parts of the SEAICE code can be enabled or disabled at compile time |
64 |
via CPP preprocessor flags. These options are set in either |
via CPP preprocessor flags. These options are set in either |
65 |
\code{SEAICE\_OPTIONS.h} or in \code{ECCO\_CPPOPTIONS.h}. |
\code{SEAICE\_OPTIONS.h} or in \code{ECCO\_CPPOPTIONS.h}. |
66 |
Table \ref{tab:pkg:seaice:cpp} summarizes these options. |
Table \ref{tab:pkg:seaice:cpp} summarizes these options. |
67 |
|
|
68 |
\begin{table}[h!] |
\begin{table}[!ht] |
69 |
\centering |
\centering |
70 |
\label{tab:pkg:seaice:cpp} |
\label{tab:pkg:seaice:cpp} |
71 |
{\footnotesize |
{\footnotesize |
127 |
~ \\ |
~ \\ |
128 |
% |
% |
129 |
Table~\ref{tab:pkg:seaice:runtimeparms} lists most run-time parameters. |
Table~\ref{tab:pkg:seaice:runtimeparms} lists most run-time parameters. |
130 |
\input{part6/seaice-parms.tex} |
\input{s_phys_pkgs/text/seaice-parms.tex} |
131 |
|
|
132 |
\paragraph{Input fields and units\label{sec:pkg:seaice:fields_units}} |
\paragraph{Input fields and units\label{sec:pkg:seaice:fields_units}} |
133 |
\begin{description} |
\begin{description} |
531 |
\phantom{=}& \phantom{\frac{1}{A_{i,j}^w} \biggl\{} |
\phantom{=}& \phantom{\frac{1}{A_{i,j}^w} \biggl\{} |
532 |
+ (\Delta{x}_1\sigma_{21})_{i,j+1}^Z - (\Delta{x}_1\sigma_{21})_{i,j}^Z |
+ (\Delta{x}_1\sigma_{21})_{i,j+1}^Z - (\Delta{x}_1\sigma_{21})_{i,j}^Z |
533 |
\biggr\} |
\biggr\} |
534 |
\intertext{with} |
\end{align} |
535 |
|
with |
536 |
|
\begin{align} |
537 |
(\Delta{x}_2\sigma_{11})_{i,j}^C =& \phantom{+} |
(\Delta{x}_2\sigma_{11})_{i,j}^C =& \phantom{+} |
538 |
\Delta{y}_{i,j}^{F}(\zeta + \eta)^{C}_{i,j} |
\Delta{y}_{i,j}^{F}(\zeta + \eta)^{C}_{i,j} |
539 |
\frac{u_{i+1,j}-u_{i,j}}{\Delta{x}_{i,j}^{F}} \\ \notag |
\frac{u_{i+1,j}-u_{i,j}}{\Delta{x}_{i,j}^{F}} \\ \notag |
575 |
\phantom{=}& \phantom{\frac{1}{A_{i,j}^s} \biggl\{} |
\phantom{=}& \phantom{\frac{1}{A_{i,j}^s} \biggl\{} |
576 |
+ (\Delta{x}_1\sigma_{22})_{i,j}^C - (\Delta{x}_1\sigma_{22})_{i,j-1}^C |
+ (\Delta{x}_1\sigma_{22})_{i,j}^C - (\Delta{x}_1\sigma_{22})_{i,j-1}^C |
577 |
\biggr\} |
\biggr\} |
578 |
\intertext{with} |
\end{align} |
579 |
|
with |
580 |
|
\begin{align} |
581 |
(\Delta{x}_1\sigma_{12})_{i,j}^Z =& \phantom{+} |
(\Delta{x}_1\sigma_{12})_{i,j}^Z =& \phantom{+} |
582 |
\Delta{y}_{i,j}^{U}\overline{\eta}^{Z}_{i,j} |
\Delta{y}_{i,j}^{U}\overline{\eta}^{Z}_{i,j} |
583 |
\frac{u_{i,j}-u_{i,j-1}}{\Delta{y}_{i,j}^{U}} |
\frac{u_{i,j}-u_{i,j-1}}{\Delta{y}_{i,j}^{U}} |
674 |
diffusive terms for quantities $X=(c\cdot{h}), c, (c\cdot{h}_{s})$. |
diffusive terms for quantities $X=(c\cdot{h}), c, (c\cdot{h}_{s})$. |
675 |
% |
% |
676 |
From the various advection scheme that are available in the MITgcm, we |
From the various advection scheme that are available in the MITgcm, we |
677 |
choose flux-limited schemes \citep[multidimensional 2nd and 3rd-order |
recommend flux-limited schemes \citep[multidimensional 2nd and |
678 |
advection scheme with flux limiter][]{roe:85, hundsdorfer94} to |
3rd-order advection scheme with flux limiter][]{roe:85, hundsdorfer94} |
679 |
preserve sharp gradients and edges that are typical of sea ice |
to preserve sharp gradients and edges that are typical of sea ice |
680 |
distributions and to rule out unphysical over- and undershoots |
distributions and to rule out unphysical over- and undershoots |
681 |
(negative thickness or concentration). These scheme conserve volume |
(negative thickness or concentration). These schemes conserve volume |
682 |
and horizontal area and are unconditionally stable, so that we can set |
and horizontal area and are unconditionally stable, so that we can set |
683 |
$D_{X}=0$. Run-timeflags: \code{SEAICEadvScheme} (default=2), |
$D_{X}=0$. Run-timeflags: \code{SEAICEadvScheme} (default=2, is the |
684 |
\code{DIFF1} (default=0.004). |
historic 2nd-order, centered difference scheme), \code{DIFF1} |
685 |
|
(default=0.004). |
686 |
|
|
687 |
There is considerable doubt about the reliability of a ``zero-layer'' |
There is considerable doubt about the reliability of a ``zero-layer'' |
688 |
thermodynamic model --- \citet{semtner84} found significant errors in |
thermodynamic model --- \citet{semtner84} found significant errors in |
774 |
Available output fields are summarized in |
Available output fields are summarized in |
775 |
Table \ref{tab:pkg:seaice:diagnostics}. |
Table \ref{tab:pkg:seaice:diagnostics}. |
776 |
|
|
777 |
\begin{table}[h!] |
\begin{table}[!ht] |
778 |
\centering |
\centering |
779 |
\label{tab:pkg:seaice:diagnostics} |
\label{tab:pkg:seaice:diagnostics} |
780 |
{\footnotesize |
{\footnotesize |
839 |
|
|
840 |
%%% Local Variables: |
%%% Local Variables: |
841 |
%%% mode: latex |
%%% mode: latex |
842 |
%%% TeX-master: "../manual" |
%%% TeX-master: "../../manual" |
843 |
%%% End: |
%%% End: |