By M. Holt

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**Sample text**

GW05] Thierry Gallay and C. Eugene Wayne. Global stability of vortex solutions of the twodimensional Navier-Stokes equation. Comm. Math. , 255(1):97–129, 2005. [Hal88] Jack K. Hale. Asymptotic behavior of dissipative systems, volume 25 of Mathematical Surveys and Monographs. American Mathematical Society, Providence, RI, 1988. [Hen81] Daniel Henry. Geometric theory of semilinear parabolic equations, volume 840 of Lecture Notes in Mathematics. Springer-Verlag, Berlin, 1981. [JT93] Don A. Jones and Edriss S.

Pd W/, the projection of W onto an d-dimensional subspace of the infinite dimensional phase space, and consider the maximum growth rate over all such projections. 78) In this estimate, the factor of 4 2 ı is just the area of the domain on which the equation evolves, and g is the forcing term in the equation for the velocity field, not the vorticity, and this force is assumed to be constant in time. Note that although the forcing function for the fluid velocity appears in the estimate of dimension, the actual estimates are done in the vorticity formulation which seems to yield sharper bounds on the attractor dimension than working directly with the velocity [CFT88].

T2ı /, then so are both components of the velocity field. 72), and take advantage of the fact that the external forcing is zero here, we see that all solutions will tend asymptotically to zero. We note here an important distinction between the Navier-Stokes equation on the torus and in the plane. t/ 2 L2 for any t > 0. However, in the present case, as noted just above, this implies that the system has finite energy and hence will decay to zero as t ! 1, rather than to an Oseen vortex, as in the previous section.