Abstract

This paper is devoted to the large time behavior and especially to the regularity of the global attractor of the second grade fluid equations in the two-dimensional torus. We first recall that, for any size of the material coefficient α > 0 , these equations are globally well posed and admit a compact global attractor A α in ( H 3 ( T 2 ) ) 2 . We prove that, for any α > 0 , there exists β ( α ) > 0 , such that A α belongs to ( H 3 + β ( α ) ( T 2 ) ) 2 if the forcing term is in ( H 1 + β ( α ) ( T 2 ) ) 2 . We also show that this attractor is contained in any Sobolev space ( H 3 + m ( T 2 ) ) 2 provided that α is small enough and the forcing term is regular enough. These arguments lead also to a new proof of the existence of the compact global attractor A α . Furthermore we prove that on A α , the second grade fluid system can be reduced to a finite-dimensional system of ordinary differential equations with an infinite delay. Moreover, the existence of a finite number of determining modes for the equations of the second grade fluid is established.

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