57A034
A new modelling framework for sea-ice mechanics based on
elasto-brittle rheology
Lucas Girard, Sylvain Bouillon, Jérôme Weiss,
David Amitrano, Vincent Legat
Corresponding author: Lucas Girard –
lgirard@lgge.obs.ujf-grenoble.fr
We present a new and original modelling framework for
sea-ice mechanics based on elasto-brittle (EB) behavior. Sea-ice deformation
plays a key role in air–ice–ocean interactions as well as the global
dynamics of the ice cover, but it is crudely represented in current sea-ice
models which are based mainly in the viscous-plastic (VP) rheology. The aim of
the framework we present is to capture the statistical and scaling properties of
sea-ice deformation. Sea ice is considered as a continuous elastic plate
encountering progressive damage, represented as a reduction of the elastic
modulus at the local (element) scale and reflecting the increase of crack and
lead density. The damage threshold is determined using the Coulomb criterion. As
the result of long-range interactions, the stress relaxation following a damage
event can induce an avalanche of damage. Damage propagates in narrow linear
features, resulting in a very heterogeneous strain field. A second criterion is
implemented to account for the formation of pressure ridges taking place under
high confining stress states. Simulations over short timescales (~48 hours) are
performed with a finite element application of the model over the Arctic Ocean.
Sea ice is considered as quasi-static (no advection) forced by wind stress
fields derived from ECMWF analysis. The simulated ice deformation fields compare
well with strain-rate estimates derived from RGPS observations: deformation
strongly localizes into quasi-linear features, and the statistical and scaling
properties of the fields are in striking agreement with observations. For
comparison, similar simulations are performed with the VP rheology implemented
in the finite element version of the Louvain-la-Neuve ice model (LIM). We show
that the EB model considerably improves the representation of sea-ice
deformation. These results motivate the implementation of the EB model in a
global dynamic–thermodynamic sea-ice model.
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