Definition
Weak Navier–Stokes solution
Locally square-integrable velocity and locally integrable pressure satisfying momentum and incompressibility against tests.
On an open space-time cylinder , a weak Navier–Stokes solution with viscosity and locally integrable force is a pair , satisfying the integral identities
for all compactly supported smooth vector tests and scalar tests . Here the outer product has entries , and . The indicated local integrability makes these products meaningful. These are the distributional momentum and incompressibility equations.
Here uses Lebesgue square integrability on compact subsets. The tests are from the smooth test-function space; , , and are the spatial gradient, divergence, and Laplacian.
Initial data and pressure elimination
On , initial datum is imposed by allowing tests supported in and adding 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 the energy class, Leray–Hopf solutions, and suitable weak solutions.