Abstract:Gaussian measures of Gibbsian type are associated with some shell model of 3D turbulence; they are constructed by means of the energy, a conserved quantity for the 3D inviscid and unforced shell model. We prove the existence of a unique global flow for a stochastic viscous shell model and of a global flow for the deterministic inviscid shell model, with the property that these Gibbs measures are invariant for these flows.
“…[42] and [17]. It was shown in [14,Proposition 1] that the nonlinear term B(· , ·) for the GOY and Sabra shell models satisfies Assumption 2.2 with H = H. For more mathematical results related to shell models we refer to [3,5,6,14] and references therein.…”
Section: Goy and Sabra Shell Models Of Turbulencementioning
confidence: 99%
“…Their studies have generated many important results. We refer, for instance, to [5,20,[22][23][24]27,28,[38][39][40] and references therein for the results obtained and the advances that have been made so far.…”
Abstract:In this paper, we derive several results related to the long-time behavior of a class of stochastic semilinear evolution equations in a separable Hilbert space H:Here A is a positive self-adjoint operator and B is a bilinear map, and the driving noise L is basically a D(A −1/2 )-valued Lévy process satisfying several technical assumptions. By using a density transformation theorem type for Lévy measure, we first prove a support theorem and an irreducibility property of the Ornstein-Uhlenbeck processes associated to the nonlinear stochastic problem. Second, by exploiting the previous results we establish the irreducibility of the nonlinear problem provided that for a certain γUsing a coupling argument, the exponential ergodicity is also proved under the stronger assumption that B is continuous on H × H. While the latter condition is only satisfied by the nonlinearities of GOY and Sabra shell models, the assumption under which the irreducibility property holds is verified by several hydrodynamical systems such as the 2D Navier-Stokes, Magnetohydrodynamics equations, the 3D Leray-α model, the GOY and Sabra shell models.
“…[42] and [17]. It was shown in [14,Proposition 1] that the nonlinear term B(· , ·) for the GOY and Sabra shell models satisfies Assumption 2.2 with H = H. For more mathematical results related to shell models we refer to [3,5,6,14] and references therein.…”
Section: Goy and Sabra Shell Models Of Turbulencementioning
confidence: 99%
“…Their studies have generated many important results. We refer, for instance, to [5,20,[22][23][24]27,28,[38][39][40] and references therein for the results obtained and the advances that have been made so far.…”
Abstract:In this paper, we derive several results related to the long-time behavior of a class of stochastic semilinear evolution equations in a separable Hilbert space H:Here A is a positive self-adjoint operator and B is a bilinear map, and the driving noise L is basically a D(A −1/2 )-valued Lévy process satisfying several technical assumptions. By using a density transformation theorem type for Lévy measure, we first prove a support theorem and an irreducibility property of the Ornstein-Uhlenbeck processes associated to the nonlinear stochastic problem. Second, by exploiting the previous results we establish the irreducibility of the nonlinear problem provided that for a certain γUsing a coupling argument, the exponential ergodicity is also proved under the stronger assumption that B is continuous on H × H. While the latter condition is only satisfied by the nonlinearities of GOY and Sabra shell models, the assumption under which the irreducibility property holds is verified by several hydrodynamical systems such as the 2D Navier-Stokes, Magnetohydrodynamics equations, the 3D Leray-α model, the GOY and Sabra shell models.
“…But, they retain many important features of the true hydrodynamical models. Instead of dealing with complex valued unknowns we deal with the real and imaginary part of each component of the scalar velocity field (for the basic settings we follow [4]); this defines a sequence {u n } n with u n ∈ R 2 . For x = (x 1 , x 2 ) ∈ R 2 we set |x| 2 = x 2 1 + x 2 2 and the scalar product in R 2 is x · y = x 1 y 1 + x 2 y 2 .…”
Section: An Example: Shell Models Of Turbulencementioning
confidence: 99%
“…We set k n = √ λ n . The bilinear term B is defined by means of the components B n = (B n,1 , B n,2 ) as follows (see, e.g., [4]):…”
Section: An Example: Shell Models Of Turbulencementioning
confidence: 99%
“…We point out that the Gaussian invariant measure that we consider here is not the Gibbs measure of the enstrophy considered for the 2D stochastic NavierStokes or deterministic 2D Euler equation in previous papers [1,2,4,13,16], but has a more regular support. In particular, the support of this measure is a Sobolev space of non negative exponent.…”
Gaussian measures μ β,ν are associated to some stochastic 2D models of turbulence. They are Gibbs measures constructed by means of an invariant quantity of the system depending on some parameter β (related to the 2D nature of the fluid) and the viscosity ν. We prove the existence and the uniqueness of the global flow for the stochastic viscous system; moreover the measure μ β,ν is invariant for this flow and is the unique invariant measure. Finally, we prove that the deterministic inviscid equation has a μ β,ν -stationary solution (for any ν > 0).
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