Abstract

Micropolar fluid and magneto-micropolar fluid systems are systems of equations with distinctive feature in its applicability and also mathematical difficulty. The purpose of this work is to follow the approach of [ 8 ] and show that another general class of systems of equations, that includes the two-dimensional micropolar and magneto-micropolar fluid systems, is well-posed and satisfies the Laplace principle, and consequently the large deviation principle, with the same rate function.

Highlights

  • The theory of large deviations is an important direction of research and has been studied by many (e.g. [13, 20], Chapter 12 [12], [7])

  • The authors in [16] developed an approach to this theory through proving the convergence of solutions to variational problems, based on the fact that the large deviation principle (LDP) in a Polish space is equivalent to Laplace principle

  • The work in [8] covered many models that include the NavierStokes equations (NSE), magnetohydrodynamics (MHD) system, Benard problem, magnetic Benard problem, Leray ↵- model and shell models of turbulence; we refer to its accompanying paper [9] for Wong-Zakai approximation results

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Summary

Department of Mathematics University of Rochester

Micropolar fluid and magneto-micropolar fluid systems are sysAbstract. tems of equations with distinctive feature in its applicability and mathematical di culty. Micropolar fluid and magneto-micropolar fluid systems are sysAbstract. Tems of equations with distinctive feature in its applicability and mathematical di culty. The purpose of this work is to follow the approach of [8] and show that another general class of systems of equations, that includes the twodimensional micropolar and magneto-micropolar fluid systems, is well-posed and satisfies the Laplace principle, and the large deviation principle, with the same rate function

Introduction
Vi with k
It holds that for all
Now we estimate
Now for
Sh weakly in
Now we let
Zt p
Then KM is a compact
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