Divergence free range of the mild Stokes integral #
The closed Leray data space is preserved by the time-integrated Stokes term in lem:reg-local-mild.
The continuous identification of Hilbert vectors with coordinate triples for the mild integral.
Equations
- CKN.Leray.mildIntegralCoordinateEquiv = PiLp.continuousLinearEquiv 2 ℝ fun (x : Fin 3) => ℝ
Instances For
theorem
CKN.Leray.mildIntegralWeakPairing_integrable
(a : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3)
(ha : IsWeakDivFreeL2 a)
(ψ : WeakTestFunction Set.univ)
:
MeasureTheory.Integrable (fun (x : Foundation.Parabolic.Vec3) => ∑ i : Fin 3, a x i * ψ.partialDeriv i x)
MeasureTheory.volume
The subspace of L² velocities satisfying the regularized mild integral J condition.
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
CKN.Leray.regularizedMildJData_sub
{u v : ↥RealVectorL2}
(hu : RegularizedMildJData u)
(hv : RegularizedMildJData v)
:
RegularizedMildJData (u - v)
The real Leray data used in the regularized mild flow are closed under subtraction.
theorem
CKN.Leray.regularizedMildStokesIntegral_isInJ
(F : ℝ → ↥RealTensorL2)
(hF : Continuous F)
(C T t : ℝ)
(hFC : ∀ (s : ℝ), ‖F s‖ ≤ C)
(hC : 0 ≤ C)
(hT : 0 ≤ T)
(hTpos : 0 < T)
(ht : 0 ≤ t)
(htT : t ≤ T)
:
The Stokes time integral takes values in the closed divergence free space used for trajectories in lem:reg-local-mild.