Vorticity equation on surfaces with arbitrary topology

TL;DR

This paper derives the vorticity equation for incompressible fluids on surfaces with arbitrary topology, exploring Hamiltonian structures and two formulations of the diffusion operator considering surface curvature.

Contribution

It introduces a novel derivation of the vorticity equation on complex surfaces and compares two approaches for modeling diffusion incorporating surface curvature effects.

Findings

Conserved surface energy and enstrophy identified in the inviscid limit.

Two diffusion operators formulated: one standard on Riemannian manifolds, one curvature-based.

Diffusive equilibria minimize dissipation considering surface curvature.

Abstract

We derive the vorticity equation for an incompressible fluid on a 2-dimensional surface with arbitrary topology embedded in 3-dimensional Euclidean space by using a tailored Clebsch parametrization of the flow. In the inviscid limit, we identify conserved surface energy and enstrophy, and obtain the corresponding noncanonical Hamiltonian structure. We then discuss the formulation of the diffusion operator on the surface by examining two alternatives. In the first case, we follow the standard approach for the Navier-Stokes equations on a Riemannian manifold and calculate the diffusion operator by requiring that flows corresponding to Killing fields of the Riemannian metric are not subject to dissipation. For an embedded surface, this leads to a diffusion operator including derivatives of the stream function across the surface. In the second case, using an analogy with the Poisson equation for the Newtonian gravitational potential in general relativity, we construct a diffusion operator taking into account the Ricci scalar curvature of the surface. The resulting vorticity equation is 2-dimensional, and the corresponding diffusive equilibria minimize dissipation under the constraint of curvature energy.