The strong equation with its time derivative, and solenoidality #
For a strong solution in the class of prop:lps-local-strong, integrating the term
-u · ∂ₜφ of the weak momentum equation by parts in time gives the equation with the
weak time derivative ∂ₜu tested against φ, and every time slice being weakly
solenoidal gives ∑ᵢ ∂ᵢuᵢ = 0 almost everywhere on the slab. Both are inputs of the
difference-quotient argument of prop:lps-smoothing.
Integrability, against a space-time test field, of the integrand of the weak momentum
equation written with a time-derivative field A, a flux F, a gradient field G and
a pressure q (prop:lps-smoothing). Only F is merely integrable.
The weak momentum equation of a strong solution, with the term -u · ∂ₜφ integrated
by parts in time against a weak time derivative Dtu of u (prop:lps-smoothing).
The gradient of a strong solution is trace free almost everywhere on the slab: every
time slice lies in J (prop:lps-local-strong, used in prop:lps-smoothing).