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Geometry of shallow-water dynamics with thermodynamics

Published 15 Jun 2021 in nlin.CD, physics.ao-ph, and physics.flu-dyn | (2106.08268v1)

Abstract: We review the geometric structure of the IL$0$PE model, a rotating shallow-water model with variable buoyancy, thus sometimes called ``thermal'' shallow-water model. We start by discussing the Euler--Poincar\'e equations for rigid body dynamics and the generalized Hamiltonian structure of the system. We then reveal similar geometric structure for the IL$0$PE. We show, in particular, that the model equations and its (Lie--Poisson) Hamiltonian structure can be deduced from Morrison and Greene's (1980) system upon ignoring the magnetic field ($\vec{\mathrm B} = 0$) and setting $U(\rho,s) = \frac{1}{2}\rho s$, where $\rho$ is mass density and $s$ is entropy per unit mass. These variables play the role of layer thickness ($h$) and buoyancy ($\t$) in the IL$0$PE, respectively. Included in an appendix is an explicit proof of the Jacobi identity satisfied by the Poisson bracket of the system.

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