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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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during the <strong>AIDJEX</strong> main experiment could be simulated (Colony, 1975).<br />

addition to simulations <strong>of</strong> observed conditions, numerous calculations have<br />

been performed using idealized driving forces (Pritchard and Schwaegler,<br />

1975; Pritchard and Colony, 1974; Schwaegler and Pritchard, 1977). Complete<br />

simulations during special time periods in the 1975-76 <strong>AIDJEX</strong> main experiment<br />

also allowed a test <strong>of</strong> the model under realistic driving forces.<br />

last cases the model response was compared with observed response <strong>of</strong> the ice<br />

cover. These results were reported by Coon et al. (1976, 1977) and by<br />

Pritchard et al. (1976, 1977).<br />

In<br />

In these<br />

While the aforementioned calculations have increased understanding <strong>of</strong><br />

how the model responds to a given set <strong>of</strong> conditions, they have also raised<br />

some questions.<br />

The lack <strong>of</strong> answers is <strong>of</strong>ten caused by the difficulty <strong>of</strong><br />

understanding how each physical property affects response, 'and this diffi-<br />

culty is enhanced by nonlinearities <strong>of</strong> the model.<br />

are requi.red, it is particularly difficult to determine accurately special<br />

local features <strong>of</strong> the response, such as velocity discontinuities. Because<br />

<strong>of</strong> these difficulties, the present work was undertaken.<br />

out that the jump conditions that must be satisfied when discontinuities <strong>of</strong><br />

various kinds are present were discussed by Nye (1975).<br />

Since numerical solutions<br />

It should be pointed<br />

That analysis, how-<br />

ever, did not address the question <strong>of</strong> when or where discontinuites might<br />

arise or how solutions might vary along discontinuities.<br />

It is known that<br />

characteristics play a dominant role in the nature <strong>of</strong> the solutions <strong>of</strong> cer-<br />

tain systems <strong>of</strong> partial differential equations (Courant an& Hilbert, 1962).<br />

For example, discontinuities may exist in solutions only along characteris-<br />

tic curves. Since some partial differential equations do not admit real<br />

characteristic curves, these systems eliminate the possibility <strong>of</strong> a discont<br />

inuity .<br />

Satellite images <strong>of</strong> the ice cover (both NOAA-4 and Landsat) have shown<br />

that deformations are <strong>of</strong>ten concentrated in narrow bands that could be well<br />

approximated as velocity discontinuities on time scales <strong>of</strong> a day. Between<br />

these discontinuities, deformations <strong>of</strong> lower magnitudes also occur. It is<br />

our feeling that these features can be represented by a plastic ice model.<br />

Therefore, it is important to understand how, when, and where discontinui-<br />

ties may arise. Since discontinuities may arise in modeled stress fields<br />

111

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