Non-autonomous 2D Navier-Stokes system with a simple global attractor and some averaging problems. (English) Zbl 1068.35089
Summary: We study the global attractor of the non-autonomous 2D Navier-Stokes system with time-dependent external force \(g(x,t)\). We assume that \(g(x,t)\) is a translation compact function and the corresponding Grashof number is small. Then the global attractor has a simple structure: it is the closure of all the values of the unique bounded complete trajectory of the Navier-Stokes (NS) system. In particular, if \(g(x,t)\) is a quasiperiodic function with respect to \(t\), then the attractor is a continuous image of a torus. Moreover the global attractor attracts all the solutions of the NS system with exponential rate, that is, the attractor is exponential. We also consider the 2D Navier-Stokes system with rapidly oscillating external force \(g(x,t,t/\varepsilon )\), which has the average as \(\varepsilon \rightarrow 0+\). We assume that the function \(g(x,t,z)\) has a bounded primitive with respect to \(z\) and the averaged NS system has a small Grashof number that provides a simple structure of the averaged global attractor. Then we prove that the distance from the global attractor of the original NS system to the attractor of the averaged NS system is less than a small power of \(\varepsilon \).
MSC:
35Q30 | Navier-Stokes equations |
37L30 | Attractors and their dimensions, Lyapunov exponents for infinite-dimensional dissipative dynamical systems |
34C29 | Averaging method for ordinary differential equations |
35B40 | Asymptotic behavior of solutions to PDEs |
35B41 | Attractors |
37N10 | Dynamical systems in fluid mechanics, oceanography and meteorology |
76D05 | Navier-Stokes equations for incompressible viscous fluids |
Keywords:
time averaging; Navier-Stokes system with rapidly oscillating external force; averaged NS system; small Grashof number; averaged global attractorReferences:
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