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The viscous-plastic momentum equations for sea-ice dynamics are a model for the time evolution of the horizontal velocity field of a vertically homogeneous column of ice-pack continuum whose thickness and ice concentration vary in time and space. They constitute a highly nonlinear system of partial differential equations, and as such, both the mathematical analysis and numerical solution of its solution remain a challenge. To shed some light on this problem, we compared the performance of two known time discretization methods: the backward Euler (BE) and the Crank-Nicolson (CN) methods. Both methods are in theory unconditionally stable, but Euler's method is only first-order accurate while Crank-Nicolson is second-order. Centered finite differences were used for the spatial derivatives. This led to a nonlinear system of algebraic equations which was then solved using a Jacobian-free Newton-Krylov approach. First, the two methods were compared in terms of their ability to reproduce a synthetic solution to the viscous-plastic momentum equations when an artificial forcing is applied. The convergence of the two methods is assessed for a short time integration period of 12 hours and grid resolutions of
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