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Averaging of 2D Navier-Stokes equations with singularly oscillating forces

机译:具有奇异振荡力的二维Navier-Stokes方程的平均

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摘要

For rho is an element of[0, 1) and epsilon > 0, the nonautonomous 2D Navier-Stokes equations with singularly oscillating external force partial derivative(t)u - upsilon Delta u + (u . del)u = -del p + g(0)(t) + epsilon(-rho) g(1) (t/epsilon), del . u = 0 are considered, together with the averaged equations partial derivative(t)u - upsilon Delta u + (u . del)u = -del p + g(0)(t) del . u = 0 formally corresponding to the limiting case epsilon = 0. Under suitable assumptions on the external force, the uniform boundedness of the related uniform global attractors A(epsilon) is established, as well as the convergence of the attractors A e of the first system to the attractor A(0) of the second one as epsilon -> 0(+). When the Grashof number of the averaged equations is small, the convergence rate of A(epsilon) to A(0) is controlled by K epsilon(1-rho)
机译:因为rho是[0,1)的元素并且epsilon> 0,所以非自治二维Navier-Stokes方程具有奇异振荡的外力偏导数(t)u -upsilon Delta u +(u。del)u = -del p + g(0)(t)+ epsilon(-rho)g(1)(t / epsilon),del。考虑u = 0以及平均方程的偏导数(t)u -upsilonδu +(u.del)u = -del p + g(0)(t)del。 u = 0正式对应于极限情况epsilon =0。在适当的外力假设下,建立了相关均匀全局吸引子A(epsilon)的一致有界性,以及第一个吸引子A e的收敛系统到第二个吸引子A(0)的epsilon-> 0(+)。当平均方程的Grashof数小时,A(ε)到A(0)的收敛速度由K epsilon(1-rho)控制

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