Statistical mechanics of Fofonoff flows in an oceanic basin (original) (raw)

2011, The European Physical Journal B

We study the minimization of potential enstrophy at fixed circulation and energy in an oceanic basin with arbitrary topography. For illustration, we consider a rectangular basin and a linear topography h = by which represents either a real bottom topography or the β-effect appropriate to oceanic situations. Our minimum enstrophy principle is motivated by different arguments of statistical mechanics reviewed in the article. It leads to steady states of the quasigeostrophic (QG) equations characterized by a linear relationship between potential vorticity q and stream function ψ. For low values of the energy, we recover Fofonoff flows [J. Mar. Res. 13, 254 (1954)] that display a strong westward jet. For large values of the energy, we obtain geometry induced phase transitions between monopoles and dipoles similar to those found by Chavanis & Sommeria [J. Fluid Mech. 314, 267 (1996)] in the absence of topography. In the presence of topography, we recover and confirm the results obtained by Venaille & Bouchet [Phys. Rev. Lett. 102, 104501 (2009)] using a different formalism. In addition, we introduce relaxation equations towards minimum potential enstrophy states and perform numerical simulations to illustrate the phase transitions in a rectangular oceanic basin with linear topography (or β-effect). PACS numbers: 05.20.-y Classical statistical mechanics -05.45.-a Nonlinear dynamics and chaos -05.90.+m Other topics in statistical physics, thermodynamics, and nonlinear dynamical systems -47.10.-g General theory in fluid dynamics -47.15.ki Inviscid flows with vorticity -47.20.-k Flow instabilities -47.32.-y Vortex dynamics; rotating fluids

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Statistical mechanics of two-dimensional Euler flows and minimum enstrophy states

The European Physical Journal B, 2010

A simplified thermodynamic approach of the incompressible 2D Euler equation is considered based on the conservation of energy, circulation and microscopic enstrophy. Statistical equilibrium states are obtained by maximizing the Miller-Robert-Sommeria (MRS) entropy under these sole constraints. We assume that these constraints are selected by properties of forcing and dissipation. We find that the vorticity fluctuations are Gaussian while the mean flow is characterized by a linear ω − ψ relationship. Furthermore, we prove that the maximization of entropy at fixed energy, circulation and microscopic enstrophy is equivalent to the minimization of macroscopic enstrophy at fixed energy and circulation. This provides a justification of the minimum enstrophy principle from statistical mechanics when only the microscopic enstrophy is conserved among the infinite class of Casimir constraints. Relaxation equations towards the statistical equilibrium state are derived. These equations can serve as numerical algorithms to determine maximum entropy or minimum enstrophy states. We use these relaxation equations to study geometry induced phase transitions in rectangular domains. In particular, we illustrate with the relaxation equations the transition between monopoles and dipoles predicted by Chavanis & Sommeria [J. Fluid. Mech. 314, 267 (1996)]. We take into account stable as well as metastable states and show that metastable states are robust and have negative specific heats. This is the first evidence of negative specific heats in that context. We also argue that saddle points of entropy can be long-lived and play a role in the dynamics because the system may not spontaneously generate the perturbations that destabilize them. PACS numbers: 05.20.-y Classical statistical mechanics -05.45.-a Nonlinear dynamics and chaos -05.90.+m Other topics in statistical physics, thermodynamics, and nonlinear dynamical systems -47.10.-g General theory in fluid dynamics -47.15.ki Inviscid flows with vorticity -47.20.-k Flow instabilities -47.32.-y Vortex dynamics; rotating fluids

Nonlinear stability and statistical mechanics of flow over topography

The stability properties and stationary statistics of inviscid barotropic flow over topography are examined. Minimum enstrophy states have potential vorticity proportional to the streamfunction and are nonlinearly stable ; correspondingly, canonical equilibrium based on energy and enstrophy conservation predicts mean potential vorticity is proportional to the mean streamfunction. It is demonstrated that in the limit of infinite resolution the canonical mean state is statistically sharp, that is, without any eddy energy on any scale, and is identical to the nonlinearly stable minimum enstrophy state. Special attention is given to the interaction between small scales and a dynamically evolving large-scale flow. On the b-plane, these stable flows have a westward large-scale component. Possibilities for a general relation between inviscid statistical equilibrium and nonlinear stability theory are examined. of two-dimensional turbulence.

Statistical mechanics of quasi-geostrophic flows on a rotating sphere

Journal of Statistical Mechanics: Theory and Experiment, 2012

Statistical mechanics provides an elegant explanation to the appearance of coherent structures in two-dimensional inviscid turbulence: while the fine-grained vorticity field, described by the Euler equation, becomes more and more filamented through time, its dynamical evolution is constrained by some global conservation laws (energy, Casimir invariants). As a consequence, the coarse-grained vorticity field can be predicted through standard statistical mechanics arguments (relying on the Hamiltonian structure of the two-dimensional Euler flow), for any given set of the integral constraints.

Statistical mechanics of the shallow-water system with an a priori potential vorticity distribution

Comptes Rendus Physique, 2006

We adapt the statistical mechanics of the shallow-water equations to the case where the flow is forced at small scales. We assume that the statistics of forcing is encoded in a prior potential vorticity distribution which replaces the specification of the Casimir constraints in the case of freely evolving flows. This determines a generalized entropy functional which is maximized by the coarse-grained PV field at statistical equilibrium. Relaxation equations towards equilibrium are derived which conserve the robust constraints (energy, mass and circulation) and increase the generalized entropy.

Evolution and decay of a rotating flow over random topography

The evolution and decay of a homogeneous flow over random topography in a rotating system is studied by means of numerical simulations and theoretical considerations. The analysis is based on a quasi-two-dimensional shallow-water approximation, in which the horizontal divergence is explicitly different from zero, and topographic variations are not restricted to be much smaller than the mean depth, as in quasigeostrophic dynamics. The results are examined by comparing the evolution of a turbulent flow over different random bottom topographies characterized by a specific horizontal scale, or equivalently, a given mean slope. As in two-dimensional turbulence, the energy of the flow is transferred towards larger scales of motion; after some rotation periods, however, the process is halted as the flow pattern becomes aligned along the topographic contours with shallow water to the right. The quasisteady state reached by the flow is characterized by a nearly linear relationship between potential vorticity and transport function in most parts of the domain, which is justified in terms of minimum-enstrophy arguments. It is found that global energy decays faster for topographies with shorter horizontal length scales due to more effective viscous dissipation. In addition, some comparisons between simulations based on the shallow-water and quasi-geostrophic formulations are carried out. The role of solid boundaries is also examined: it is shown that vorticity production at no-slip walls contributes for a slight disorganization of the flow.

Non-linear dynamics and statistical theories for basic geophysical flows

2006

Preface page xi 1 Barotropic geophysical flows and two-dimensional fluid flows: elementary introduction 1.1 Introduction 1.2 Some special exact solutions t 8 1.3 Conserved quantities 1.4 Barotropic geophysical flows in a channel domain-an important physical model 1.5 Variational derivatives and an optimization principle for elementary geophysical solutions 1.6 More equations for geophysical flows References 2 The response to large-scale forcing \ 2.1 Introduction 2.2 Non-linear stability with Kolmogorov forcing 2.3 Stability of flows with generalized Kolmogorov forcing References 3 The selective decay principle for basic geophysical flows 3.1 Introduction 3.2 Selective decay states and their invariance 3.3 Mathematical formulation of the selective decay principle 3.4 Energy-enstrophy decay 3.5 Bounds on the Dirichlet quotient, A(t) 3.6 Rigorous theory for selective decay 3.7 Numerical experiments demonstrating facets of selective decay References vi Contents A.l Stronger controls on A(?) A.2 The proof of the mathematical form of the selective decay principle in the presence of the beta-plane effect 4 Non-linear stability of steady geophysical flows 4.1 Introduction 4.2 Stability of simple steady states 4.3 Stability for more general steady states 4.4 Non-linear stability of zonal flows on the beta-plane 4.5 Variational characterization of the steady states References 5 Topographic mean flow interaction, non-linear instability, and chaotic dynamics 5.1 Introduction 5.2 Systems with layered topography 5.3 Integrable behavior 5.4 A limit regime with chaotic solutions 5.5 Numerical experiments • References Appendix 1 Appendix 2

Large-scale behavior and statistical equilibria in rotating flows

Physical Review E, 2011

We examine long-time properties of the ideal dynamics of three-dimensional flows, in the presence or not of an imposed solid-body rotation and with or without helicity (velocity-vorticity correlation). In all cases the results agree with the isotropic predictions stemming from statistical mechanics. No accumulation of excitation occurs in the large scales, even though in the dissipative rotating case anisotropy and accumulation, in the form of an inverse cascade of energy, are known to occur. We attribute this latter discrepancy to the linearity of the term responsible for the emergence of inertial waves. At intermediate times, inertial energy spectra emerge that differ somewhat from classical wave-turbulence expectations, and with a trace of large-scale excitation that goes away for long times. These results are discussed in the context of partial two-dimensionalization of the flow undergoing strong rotation as advocated by several authors.

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