On an open space-time cylinder QRn×RQ\subset\mathbb R^n\times\mathbb R, a weak Navier–Stokes solution with viscosity ν>0\nu>0 and locally integrable force ff is a pair uLloc2(Q)u\in L^2_{\rm loc}(Q), pLloc1(Q)p\in L^1_{\rm loc}(Q) satisfying the

Q(utϕ+(uu):ϕ+νuΔϕ+pdivϕ+fϕ)=0,Quψ=0\int_Q\bigl(u\cdot\partial_t\phi+(u\otimes u):\nabla\phi +\nu u\cdot\Delta\phi+p\,\operatorname{div}\phi+f\cdot\phi\bigr)=0, \qquad \int_Q u\cdot\nabla\psi=0

for all compactly supported smooth vector tests ϕ\phi and scalar tests ψ\psi. Here the has entries uiuju_i u_j, and (uu):ϕ=i,juiujjϕi(u\otimes u):\nabla\phi=\sum_{i,j}u_i u_j\partial_j\phi_i. The indicated makes these products meaningful. These are the distributional .

Here Lloc2L^2_{\rm loc} uses on compact subsets. The tests are from the ; \nabla, div\operatorname{div}, and Δ\Delta are the spatial , , and .

Initial data and pressure elimination

On Rn×(0,T)\mathbb R^n\times(0,T), initial datum u0u_0 is imposed by allowing tests supported in [0,T)[0,T) and adding u0(x)ϕ(x,0)dx\int u_0(x)\cdot\phi(x,0)\,dx to the first identity. Restricting to divergence-free vector tests removes the pressure term. Recovering a pressure from that restricted formulation is a separate assertion depending on the domain and function spaces.

Energy conditions

This definition alone imposes neither finite global energy nor an energy inequality. See , , and .

References