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AIDJEX Bulletin #40 - Polar Science Center - University of Washington

AIDJEX Bulletin #40 - Polar Science Center - University of Washington

AIDJEX Bulletin #40 - Polar Science Center - University of Washington

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fc is the Coriolis parameter,<br />

- k is a unit vector normal to the earth's surface;<br />

To study the quasi-steady problem, we should not neglect mg, but instead<br />

write:<br />

where & = ag/ag is the velocity gradient. The model is then written in an<br />

Eulerian description.<br />

Now it is meaningful to neglect av_/at so that time<br />

dependence may be ignored. With these assumptions in mind, we may write the<br />

Cartesian components <strong>of</strong> momentum balance as<br />

where Cartesian components <strong>of</strong> all tensors are introduced:<br />

and the water stress law may include any nonlinear algebraic response that<br />

depends only on the ice velocity relative to geostrophic ocean currents<br />

(McPhee, 1975).<br />

The constitutive law used to simulate sea ice dynamics is elasticplastic<br />

(Coon et al., 1974; Coon and Pritchard, 1974; Pritchard, 1975).<br />

However, the elastic response is included primarily to help obtain a numerical<br />

solution. A rigid-plastic material law is thought to be as reasonable<br />

from a physical standpoint. Our analysis <strong>of</strong> characteristics to date has<br />

treated only the rigid-plastic model. Therefore, we must exercise care when<br />

the results <strong>of</strong> this analysis are used to interpret possible discontinuities<br />

in numerically calculated results. But we shall study the mathematical<br />

properties <strong>of</strong> the rigid-plastic model, and from these results we expect to<br />

117

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