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\reffig{arctic_topog}. It is carved out from, and obtains open |
\reffig{arctic_topog}. It is carved out from, and obtains open |
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boundary conditions from, the global cubed-sphere configuration |
boundary conditions from, the global cubed-sphere configuration |
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described above. The horizontal domain size is 420 by 384 grid boxes. |
described above. The horizontal domain size is 420 by 384 grid boxes. |
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\begin{figure} |
\begin{figure*} |
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\centerline{{\includegraphics*[width=0.44\linewidth]{\fpath/topography}}} |
\includegraphics*[width=0.44\linewidth]{\fpath/topography} |
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\caption{Bathymetry and domain boudaries of Arctic |
\includegraphics*[width=0.46\linewidth]{\fpath/archipelago} |
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Domain. The letters label sections in the Canadian Archipelago, |
\caption{Left: Bathymetry and domain boudaries of Arctic |
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where ice transport is evaluated. |
Domain; the dashed line marks the boundaries of the inset on the |
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|
right hand side. The letters in the inset label sections in the |
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Canadian Archipelago, where ice transport is evaluated: |
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A: Nares Strait; % |
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B: \ml{Meighen Island}; % |
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C: Prince Gustaf Adolf Sea; % |
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D: \ml{Brock Island}; % |
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E: McClure Strait; % |
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F: Amundsen Gulf; % |
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G: Lancaster Sound; % |
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H: Barrow Strait \ml{W.}; % |
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I: Barrow Strait \ml{E.}; % |
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J: Barrow Strait \ml{N.}. % |
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\label{fig:arctic_topog}} |
\label{fig:arctic_topog}} |
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\end{figure} |
\end{figure*} |
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|
|
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The main dynamic difference from cube sphere is that it does not use |
The main dynamic difference from cube sphere is that it does not use |
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rescaled vertical coordinates (z$^\ast$) and the surface boundary |
rescaled vertical coordinates (z$^\ast$) and the surface boundary |
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conditions for freshwater input are different, because those features |
conditions for freshwater input are different, because those features |
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are not supported by the open boundary code. |
are not supported by the open boundary code. |
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|
|
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Open water, dry ice, wet ice, dry snow, and wet snow albedo are, respectively, 0.15, 0.85, |
Open water, dry ice, wet ice, dry snow, and wet snow albedo are, |
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0.76, 0.94, and 0.8. |
respectively, 0.15, 0.85, 0.76, 0.94, and 0.8. |
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|
|
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The model is integrated from January, 1992 to March \ml{[???]}, 2000, |
The model is integrated from January, 1992 to March \ml{[???]}, 2000, |
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with three different dynamical solvers and two different boundary |
with three different dynamical solvers and two different boundary |
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|
|
285 |
The difference in ice volume and ice drift velocities between the |
The difference in ice volume and ice drift velocities between the |
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different experiments has consequences for the ice transport out of |
different experiments has consequences for the ice transport out of |
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the Arctic. Although the main export of ice goes through the Fram |
the Arctic. Although the most exported ice drifts through the Fram |
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Strait, a considerable amoung of ice is exported through the Canadian |
Strait (approximately $2300\pm610\text{\,km$^3$\,y$^{-1}$}$), a |
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Archipelago \citep{???}. \reffig{archipelago} shows a time series of |
considerable amount (order $160\text{\,km$^3$\,y$^{-1}$}$) ice is |
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\ml{[maybe smooth to longer time scales:] daily averaged} ice |
exported through the Canadian Archipelago \citep[and references |
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transport through various straits in the Canadian Archipelago and the |
therein]{serreze06}. \reffig{archipelago} shows a time series of |
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Fram Strait for the different model solutions. Generally, the |
\ml{[maybe smooth to different time scales:] daily averaged, smoothed |
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C-EVP-ns solution has highest maximum (export out of the Artic) and |
with monthly running means,} ice transports through various straits |
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minimum (import into the Artic) fluxes as the drift velocities are |
in the Canadian Archipelago and the Fram Strait for the different |
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largest in this solution \ldots |
model solutions. The export through Fram Strait is too high in all |
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|
model (annual averages ranges from $3324$ to |
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|
$3931\text{\,km$^3$\,y$^{-1}$}$) solutions, while the export through |
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Lancaster Sound is lower (annual averages are $41$ to |
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$201\text{\,km$^3$\,y$^{-1}$}$) than compared to observations. |
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Generally, the C-EVP solutions have highest maximum (export out of the |
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Artic) and minimum (import into the Artic) fluxes as the drift |
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velocities are largest in this solution. In the extreme, both B- and |
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C-grid LSOR solvers have practically no ice transport through the |
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Nares Strait, which is only a few grid points wide, while the C-EVP |
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solutions allow up to 500\,km$^3$\,y$^{-1}$ in summer. |
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\begin{figure} |
\begin{figure} |
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\centerline{{\includegraphics*[width=0.6\linewidth]{\fpath/Jan1992xport}}} |
%\centerline{{\includegraphics*[width=0.6\linewidth]{\fpath/Jan1992xport}}} |
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|
\centerline{{\includegraphics*[width=0.6\linewidth]{\fpath/ice_export}}} |
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\caption{Transport through Canadian Archipelago for different solver |
\caption{Transport through Canadian Archipelago for different solver |
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flavors. The letters refer to the labels of the sections in |
flavors. The letters refer to the labels of the sections in |
311 |
\reffig{arctic_topog}. |
\reffig{arctic_topog}; positive values are flux out of the Arctic. |
312 |
\label{fig:archipelago}} |
\label{fig:archipelago}} |
313 |
\end{figure} |
\end{figure} |
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|