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

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

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MATHEMATICAL CHARACTERISTICS OF A PLASTIC MODEL<br />

OF SEA ICE DYNAMICS<br />

Robert S. Pritchard and R. Reimer<br />

<strong>AIDJEX</strong><br />

ABSTRACT<br />

A plastic sea ice model developed by the <strong>AIDJEX</strong> modeling group is<br />

analyzed to determine the conditions under which real characteristic<br />

curves exist. For this analysis, inertia and material<br />

hardening are assumed negligible. We show that the characteristics<br />

at each point where the material is plastic can be real and<br />

distinct (hyperbolic equations), coincident (parabolic equations),<br />

or imaginary (elliptic equations). There may also be elastic<br />

regions. The characteristics enable one to see which parts <strong>of</strong><br />

the boundary affect which parts <strong>of</strong> the solution region, and<br />

thereby they show where discontinuities in the solution may be<br />

expected.<br />

The characteristic curves do not depend on advection, air stress,<br />

water drag, Coriolis force, sea surface tilt, or yield strength<br />

gradients except as these terms affect the stress state. At each<br />

point the direction taken by the characteristic curves is determined<br />

as a function <strong>of</strong> the stress state. The curves are<br />

symmetric about the principal stress axes, while the angle<br />

between them depends on the position <strong>of</strong> the stress on the yield<br />

curve. The governing set <strong>of</strong> partial differential equations are<br />

transformed into ordinary differential equations along the characteristic<br />

curves. These equations have been determined for an<br />

arbitrary isotrspic yield surface and a non-normal flow rule when<br />

advection is included.<br />

The analytical difficulties that arise when a normal flow rule<br />

and advection are simultaneously considered are discussed. It<br />

has been conjectured that in many cases the large-scale lead<br />

patterns in the ice cover are related to the characteristic<br />

curves. Since velocity discontinuities are anticipated across<br />

leads it is the velocity characteristics at which we look. Along<br />

these curves there is no stretching. This physical property<br />

neither provides a physical explanation for the correspondence<br />

between leads and characteristics nor refutes such a possibility.<br />

Further observations are required. The characteristic analysis<br />

improves our understanding <strong>of</strong> the effect <strong>of</strong> yield surface and<br />

flow rule on ice response. The characteristic equations will be<br />

109

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