In this work a complex coupled shallow ice model which governs the thermal, hydrodynamic and mechanical processes in the dynamics of large ice masses is proposed and solved by means of efficient numerical techniques.
The mathematical modelAfter that shallow ice approximation has been performed in the mass, momentum and energy conservation equations on a 2-D ice mass section (x, z) [1], the PDE system governing the upper ice sheet profile η, the velocity field v = (u, v), the temperature T and the basal magnitudes (velocity u b and stress τ b ) is provided by a set of coupled problems. The upper profile of the ice sheet section is an unknown and that is the reason why we consider a large enough fixed rectangular domainwhere z max is a large enough value. The set Ω G includes not only a longitudinal section of the ice sheet}, but also the part of the atmosphere above the ice mass. So, for any time t, the inclusion Ω I (t) ⊂ Ω G holds. Therefore, we can write the relation between domains as Ω G = Ω I (t) ∪ Ω A (t), where Ω A is the 2-D section of the atmosphere.Profile problem: the ice layer longitudinal extent is not a priori known, so that the interval (S − (t) , S + (t)) ⊂ (−1, 1) is an additional unknown. Thus, the moving boundary profile problem is posed over the fixed domain Ω = (−1, 1). For this, let t max > 0 be a large enough time instant and let a : (0, t max ) × Ω → R be the given accumulation-ablation rate and η 0 : Ω → R be the given initial profile. Then, following [4], for t ∈ [0, t max ], the formulation can be written as:where γ and ν are dimensionless parameters. The basal ice velocity u b depends on the basal temperature according to (6).Ice velocity problem: the velocity field computation is based on an original velocity model in the framework of the shallow ice approach proposed in [5]. In this asymptotic approximation, an expression for the z-derivative of the horizontal velocity can be deduced and next, by integrating the obtained expression of basal velocity from 0 to z and taking into account the velocity values at the upper profile and at the base, we obtain the expression of the horizontal velocity:where e γT is associated to viscous dissipation thermal effects and γ = 11.3 is a dimensionless parameter. Next, we can extend to the whole domain the stream function ψ associated to the ice velocity field and we can obtain the vertical velocity from ψ as follows