Energy and helicity conservation for the generalized quasi-geostrophic equation

preprint2022arXivOpen access

Abstract

In this paper, we consider the 2-D generalized surface quasi-geostrophic equation with the velocity vv determined by v=R⊥Λγ−1θv=\mathcal{R}^{\perp}Λ^{γ-1}θ. It is shown that the LpL^p type energy norm of weak solutions is conserved provided θ∈Lp+1(0,T;Bp+1,c(N)γ3)θ\in L^{p+1}(0,T; {B}^{\fracγ{3}}_{p+1, c(\mathbb{N})}) for 0<γ<320<γ<\frac32 or θ∈Lp+1(0,T;Bp+1,∞α) for any γ−1<α<1 with 32≤γ<2θ\in L^{p+1}(0,T; {B}^α_{p+1,\infty})~\text{for any}~γ-1<α<1 \text{ with} ~\frac{3}{2}\leq γ<2. Moreover, we also prove that the helicity of weak solutions satisfying ∇θ∈L3(0,T;B˙3,c(N)γ3)\nablaθ\in L^{3}(0,T;\dot{B}_{3,c(\mathbb{N})}^{\fracγ{3}}) for 0<γ<320<γ<\frac32 or ∇θ∈L3(0,T;B˙3,∞α) for any γ−1<α<1 with 32≤γ<2\nablaθ\in L^{3}(0,T; \dot{B}^α_{3,\infty})~\text{for any}~γ-1<α<1 \text{ with} ~\frac{3}{2}\leq γ<2 is invariant. Therefore, the accurate relationships between the critical regularity for the energy (helicity) conservation of the weak solutions and the regularity of velocity in 2-D generalized quasi-geostrophic equation are presented.

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