2015
DOI: 10.1137/140987833
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Inertial Manifolds for Certain Subgrid-Scale $\alpha$-Models of Turbulence

Abstract: Abstract. In this note we prove the existence of an inertial manifold, i.e., a global invariant, exponentially attracting, finite-dimensional smooth manifold, for two different sub-grid scale α-models of turbulence: the simplified Bardina model and the modified Leray-α model, in two-dimensional space. That is, we show the existence of an exact rule that parameterizes the dynamics of small spatial scales in terms of the dynamics of the large ones. In particular, this implies that the long-time dynamics of these… Show more

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Cited by 19 publications
(24 citation statements)
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“…In reproducing the argument used in Hamed to prove point (i) in Hamed,, proposition 3 (see also Hamed, proposition 9), ie, the “cone invariance property,” which is stated in Proposition (i) below, we introduce the following truncated nonlinearities: rightscriptF1(V):=χϱ(DN1/2V)[scriptR1(V)ϑlefte2],scriptF2(V):=χϱ(DN1/2V)[scriptR2(V)f],andrightrightF:left=(scriptF1,scriptF2). Here, χ is a smooth cutoff function outside the ball of radius ρ =2 in (L 2 (Ω)) 3 . Indeed, let χ:R+false[0,1false] with χ ( r )=1 for 0≤ r ≤1, χ ( r )=0 for r ≥2, and | χ ′ ( r )|≤2 for r ≥0 (which is null outside the ball of radius ρ=2trueϱ˜).…”
Section: Existence Of An Inertial Manifoldmentioning
confidence: 99%
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“…In reproducing the argument used in Hamed to prove point (i) in Hamed,, proposition 3 (see also Hamed, proposition 9), ie, the “cone invariance property,” which is stated in Proposition (i) below, we introduce the following truncated nonlinearities: rightscriptF1(V):=χϱ(DN1/2V)[scriptR1(V)ϑlefte2],scriptF2(V):=χϱ(DN1/2V)[scriptR2(V)f],andrightrightF:left=(scriptF1,scriptF2). Here, χ is a smooth cutoff function outside the ball of radius ρ =2 in (L 2 (Ω)) 3 . Indeed, let χ:R+false[0,1false] with χ ( r )=1 for 0≤ r ≤1, χ ( r )=0 for r ≥2, and | χ ′ ( r )|≤2 for r ≥0 (which is null outside the ball of radius ρ=2trueϱ˜).…”
Section: Existence Of An Inertial Manifoldmentioning
confidence: 99%
“…Proof of Proposition Let V 1 =( V 1 , ϑ 1 ) and V 2 =( v 2 , ϑ 2 ) be 2 solutions of to . To show the cone invariance, ie, the condition given in Proposition (i) (see also Hamed, proposition 3‐(i)), it is enough to show that ()centerarraybold-italicV1(t)arraybold-italicV2(t)=()centerarray(bold-italicv1(t),ϑ1(t))array(bold-italicv2(t),ϑ2(t)) cannot pass through the boundary of the cone if the dynamics starts inside the cone. More precisely, we will prove that ddt()false‖DN1false/2Qn()V1false(tfalse)V2false(tfalse)false‖γfalse‖DN1false/2Pn()V1false(tfalse)V2false(tfalse)false‖<0 whenever ()centerarraybold-italicV1(t)arraybold-italicV2(t)trueΓ˜n,γ, where trueΓ˜n,γ stands for the boundary of the cone trueΓ˜n,γ.…”
Section: Existence Of An Inertial Manifoldmentioning
confidence: 99%
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