An averaged Navier–Stokes model is

ut=νΔu+B~(u,u),divu=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=EB(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)RotRiDilλiA_i=m_i(D)\operatorname{Rot}_{R_i}\operatorname{Dil}_{\lambda_i}, with

RotRu(x)=Ru(R1x),Dilλu(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 C1λiCC^{-1}\leq\lambda_i\leq C almost surely and EiMki(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