Difference between revisions of "Kohout, Alison"
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considerable idealisation is required. One aspect which is critical to understand is the | considerable idealisation is required. One aspect which is critical to understand is the | ||
decay of wave energy through the Marginal Ice Zone (MIZ). | decay of wave energy through the Marginal Ice Zone (MIZ). | ||
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A number of models for wave propagation in the marginal ice zone have been presented. The | A number of models for wave propagation in the marginal ice zone have been presented. The | ||
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a series of experiments which were performed by \citet{sakai_hanai02} using floating plastic sheets | a series of experiments which were performed by \citet{sakai_hanai02} using floating plastic sheets | ||
in a two-dimensional wave tank. We are therefore confident that the numerical | in a two-dimensional wave tank. We are therefore confident that the numerical | ||
| − | solution presented here is correct | + | solution presented here is correct. |
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Revision as of 23:40, 23 April 2006
Alison Kohout (PHD student)
Research topic: Two dimensional wave scattering in the MIZ
The sea-ice which forms in the polar oceans plays a key role in driving the world's oceanic circulatory system and hence the world's climatic system. It is therefore important to understand the processes which influence the extent of this sea-ice. \citet{squire95,wadhams00} have evidence suggesting that ocean waves play a major role in the fracturing of ice-covered seas. The analysis of this phenomena involves many complicated variables and considerable idealisation is required. One aspect which is critical to understand is the decay of wave energy through the Marginal Ice Zone (MIZ).
A number of models for wave propagation in the marginal ice zone have been presented. The most sophisticated were the fully three dimensional models using a coupling of solutions for individual ice floes with a transport equation \citep{Masson_Le,jgrrealism}. These models, which were derived separately, have been recently shown to be almost identical \citep{ocean_modelling06}. Another three-dimensional model was developed by \citet{dixon_squire01} based on the coherent potential approximation. We present here a much simpler model based on a two-dimensional solution. Although much simpler, this model has a number of advantages over the three-dimensional models, the most important being that it is much less computationally demanding. We also believe that a simple model is the best place to begin to make comparisons with data and to test and debug the more sophisticated models.
The two-dimensional solution is based on a matched eigenfunction expansion. The model is described in detail in \citet{elastic_plates06} where the solution is carefully analysed for energy conservation, compared with previous results and compared to a series of experiments which were performed by \citet{sakai_hanai02} using floating plastic sheets in a two-dimensional wave tank. We are therefore confident that the numerical solution presented here is correct.
