44 |
Traditionally, probably for historical reasons and the ease of |
Traditionally, probably for historical reasons and the ease of |
45 |
treating the Coriolis term, most standard sea-ice models are |
treating the Coriolis term, most standard sea-ice models are |
46 |
discretized on Arakawa-B-grids \citep[e.g.,][]{hibler79, harder99, |
discretized on Arakawa-B-grids \citep[e.g.,][]{hibler79, harder99, |
47 |
kreyscher00, zhang98, hunke97}. From the perspective of coupling a |
kreyscher00, zhang98, hunke97}, although there are sea ice models |
48 |
sea ice-model to a C-grid ocean model, the exchange of fluxes of heat |
diretized on a C-grid \citep[e.g.,][]{ip91, tremblay97, |
49 |
and fresh-water pose no difficulty for a B-grid sea-ice model |
lemieux09}. % |
50 |
\citep[e.g.,][]{timmermann02a}. However, surface stress is defined at |
\ml{[there is also MI-IM, but I only found this as a reference: |
51 |
velocities points and thus needs to be interpolated between a B-grid |
\url{http://retro.met.no/english/r_and_d_activities/method/num_mod/MI-IM-Documentation.pdf}]} |
52 |
sea-ice model and a C-grid ocean model. Smoothing implicitly |
From the perspective of coupling a sea ice-model to a C-grid ocean |
53 |
associated with this interpolation may mask grid scale noise and may |
model, the exchange of fluxes of heat and fresh-water pose no |
54 |
contribute to stabilizing the solution. On the other hand, by |
difficulty for a B-grid sea-ice model \citep[e.g.,][]{timmermann02a}. |
55 |
smoothing the stress signals are damped which could lead to reduced |
However, surface stress is defined at velocities points and thus needs |
56 |
variability of the system. By choosing a C-grid for the sea-ice model, |
to be interpolated between a B-grid sea-ice model and a C-grid ocean |
57 |
we circumvent this difficulty altogether and render the stress |
model. Smoothing implicitly associated with this interpolation may |
58 |
coupling as consistent as the buoyancy coupling. |
mask grid scale noise and may contribute to stabilizing the solution. |
59 |
|
On the other hand, by smoothing the stress signals are damped which |
60 |
|
could lead to reduced variability of the system. By choosing a C-grid |
61 |
|
for the sea-ice model, we circumvent this difficulty altogether and |
62 |
|
render the stress coupling as consistent as the buoyancy coupling. |
63 |
|
|
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A further advantage of the C-grid formulation is apparent in narrow |
A further advantage of the C-grid formulation is apparent in narrow |
65 |
straits. In the limit of only one grid cell between coasts there is no |
straits. In the limit of only one grid cell between coasts there is no |
66 |
flux allowed for a B-grid (with no-slip lateral boundary counditions), |
flux allowed for a B-grid (with no-slip lateral boundary counditions), |
67 |
and models have used topographies artificially widened straits to |
and models have used topographies with artificially widened straits to |
68 |
avoid this problem \citep{holloway07}. The C-grid formulation on the |
avoid this problem \citep{holloway07}. The C-grid formulation on the |
69 |
other hand allows a flux of sea-ice through narrow passages if |
other hand allows a flux of sea-ice through narrow passages if |
70 |
free-slip along the boundaries is allowed. We demonstrate this effect |
free-slip along the boundaries is allowed. We demonstrate this effect |
73 |
Talk about problems that make the sea-ice-ocean code very sensitive and |
Talk about problems that make the sea-ice-ocean code very sensitive and |
74 |
changes in the code that reduce these sensitivities. |
changes in the code that reduce these sensitivities. |
75 |
|
|
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This paper describes the MITgcm sea ice |
This paper describes the MITgcm sea ice model; it presents example |
77 |
model; it presents example Arctic and Antarctic results from a realistic, |
Arctic and Antarctic results from a realistic, eddy-permitting, global |
78 |
eddy-permitting, global ocean and sea-ice configuration; it compares B-grid |
ocean and sea-ice configuration; it compares B-grid and C-grid dynamic |
79 |
and C-grid dynamic solvers in a regional Arctic configuration; and it presents |
solvers and investigates further aspects of sea ice modeling in a |
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example results from coupled ocean and sea-ice adjoint-model integrations. |
regional Arctic configuration; and it presents example results from |
81 |
|
coupled ocean and sea-ice adjoint-model integrations. |
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