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% $Header$ |
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% $Name$ |
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\documentclass[12pt]{article} |
\documentclass[12pt]{article} |
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\usepackage[]{graphicx} |
\usepackage[]{graphicx} |
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both thickness $h$ and compactness (concentration) $c$: |
both thickness $h$ and compactness (concentration) $c$: |
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\begin{equation} |
\begin{equation} |
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P_{\max} = P^{*}c\,h\,e^{[C^{*}\cdot(1-c)]}, |
P_{\max} = P^{*}c\,h\,e^{[C^{*}\cdot(1-c)]}, |
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\label{icestrength} |
\label{eq:icestrength} |
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\end{equation} |
\end{equation} |
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with the constants $P^{*}$ and $C^{*}$. The nonlinear bulk and shear |
with the constants $P^{*}$ and $C^{*}$. The nonlinear bulk and shear |
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viscosities $\eta$ and $\zeta$ are functions of ice strain rate |
viscosities $\eta$ and $\zeta$ are functions of ice strain rate |
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\end{description} |
\end{description} |
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\ml{[We have not implemented the EVP solver on a B-grid.]} |
\ml{[We have not implemented the EVP solver on a B-grid.]} |
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\begin{figure*}[htbp] |
\begin{figure*}[htbp] |
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%GET \includegraphics[width=\widefigwidth]{\fpath/all_086280} |
\includegraphics[width=\widefigwidth]{\fpath/all_086280} |
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\caption{Ice concentration, effective thickness [m], and ice |
\caption{Ice concentration, effective thickness [m], and ice |
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velocities [m/s] |
velocities [m/s] |
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for 5 different numerical solutions.} |
for 5 different numerical solutions.} |
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time scale, resolution and EVP-time step, effectively allowing the |
time scale, resolution and EVP-time step, effectively allowing the |
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elastic waves to damp out more quickly \citep{hunke01}. |
elastic waves to damp out more quickly \citep{hunke01}. |
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\begin{figure*}[htbp] |
\begin{figure*}[htbp] |
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%GET \includegraphics[width=\widefigwidth]{\fpath/hun12days} |
\includegraphics[width=\widefigwidth]{\fpath/hun12days} |
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\caption{Ice flow, divergence and bulk viscosities of three |
\caption{Ice flow, divergence and bulk viscosities of three |
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experiments with \citet{hunke01}'s test case: C-LSRns (top), |
experiments with \citet{hunke01}'s test case: C-LSRns (top), |
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C-EVPns (middle), and C-EVPns with damping described in |
C-EVPns (middle), and C-EVPns with damping described in |
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which in turn can have a strong effect on solutions in the limit of |
which in turn can have a strong effect on solutions in the limit of |
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nearly rigid regimes (arching and blocking, not shown). |
nearly rigid regimes (arching and blocking, not shown). |
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\ml{[Say something about performance? This is tricky, as the |
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perfomance depends strongly on the configuration. A run with slowly |
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changing forcing is favorable for LSR, because then only very few |
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iterations are required for convergences while EVP uses its fixed |
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number of internal timesteps. If the forcing in changing fast, LSR |
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needs far more iterations while EVP still uses the fixed number of |
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internal timesteps. I have produces runs where for slow forcing LSR |
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is much faster than EVP and for fast forcing, LSR is much slower |
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than EVP. EVP is certainly more efficient in terms of vectorization |
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and MFLOPS on our SX8, but is that a criterion?]} |
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\subsection{C-grid} |
\subsection{C-grid} |
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\begin{itemize} |
\begin{itemize} |
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\item no-slip vs. free-slip for both lsr and evp; |
\item no-slip vs. free-slip for both lsr and evp; |
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helpful discussions. ML thanks Elizabeth Hunke for multiple explanations. |
helpful discussions. ML thanks Elizabeth Hunke for multiple explanations. |
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\bibliography{bib/journal_abrvs,bib/seaice,bib/genocean,bib/maths,bib/mitgcmuv,bib/fram} |
\bibliography{bib/journal_abrvs,bib/seaice,bib/genocean,bib/maths,bib/mitgcmuv,bib/fram} |
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%\bibliography{journal_abrvs,seaice,genocean,maths,mixing,mitgcmuv,bib/fram} |
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\end{document} |
\end{document} |
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