/[MITgcm]/MITgcm_contrib/articles/ceaice_split_version/ceaice_part2/ceaice_concl.tex
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Wed Mar 25 13:43:18 2009 UTC (16 years, 4 months ago) by mlosch
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comment out the text, as it is just a place holder (a copy from early
versions of part1)

1 heimbach 1.1 \section{Discussion and conclusion}
2     \label{sec:concl}
3    
4 mlosch 1.2 % Recommendations
5     % \begin{itemize}
6     % \item use the LSOR or another implicit solver, because EVP tends to
7     % have too weak ice, and is much slower for the recommended time step
8     % choices ($\frac{1}{120}$ of the model time step). Linearization does
9     % not appear to be an issue for the short time steps used in this
10     % study ($\Delta{t} = 20\text{\,min}$), and the LSOR-solver converges
11     % quickly (only a few iterations) at each time step, because the
12     % forcing changes only slowly within 20\,min.
13     % \item thermodynamics appears to thave the second largest effect (after
14     % EVP vs.\ LSOR)
15     % \item use a flux limited scheme without explicit diffusion for
16     % advecting thermodynamic variables
17     % \item use no slip boundary conditions, they make more sense
18     % \item TEM has little effect on the solution, other rheologies that
19     % differ more from the elliptic yield curve may have bigger effects
20     % \item the effects of \citet{hibler87}'s stress formulation on both ice
21     % and ocean model need further exploration
22     % \end{itemize}
23 heimbach 1.1
24     %%% Local Variables:
25     %%% mode: latex
26     %%% TeX-master: "ceaice"
27     %%% End:

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