An averaged Navier–Stokes model is

ut=νΔu+B~(u,u),div⁡u=0,u_t=\nu\Delta u+\widetilde B(u,u),\qquad\operatorname{div}u=0,

where, on divergence-free H10(R3)H^{10}(\mathbb R^3) fields, the BB is replaced through

⟨B~(u,v),w⟩=E⟨B(A1u,A2v),A3w⟩.\langle\widetilde B(u,v),w\rangle =\mathbb E\langle B(A_1u,A_2v),A_3w\rangle.

Set Ai=mi(D)Rot⁡RiDil⁡λiA_i=m_i(D)\operatorname{Rot}_{R_i}\operatorname{Dil}_{\lambda_i}, with

Rot⁡Ru(x)=Ru(R−1x),Dil⁡λu(x)=λ3/2u(λx).\operatorname{Rot}_R u(x)=Ru(R^{-1}x),\qquad \operatorname{Dil}_\lambda u(x)=\lambda^{3/2}u(\lambda x).

The RiR_i are random , the mim_i are real , and E\mathbb E is . Require C−1≤λi≤CC^{-1}\leq\lambda_i\leq C almost surely and E∏iMki(mi)<∞\mathbb E\prod_iM_{k_i}(m_i)<\infty for every triple of orders. Pairings use the L2L^2 duality on the indicated .

Energy cancellation

Energy-preserving models additionally require ⟨B~(u,u),u⟩=0\langle\widetilde B(u,u),u\rangle=0. Arbitrary choices of the three transformations do not guarantee this identity. Results for a specified B~\widetilde B concern that modified equation.

References