Spatial tails of regularized Leray solutions #
The local energy identity and the uniform global energy bounds control the
velocity outside large balls, as in lem:reg-tails.
The positive-time spacetime measure is the product of spatial volume and one-dimensional volume restricted to positive times.
noncomputable def
CKN.Leray.regTailsPositiveGradientExtension
(D : Foundation.Parabolic.ParabolicPoint → Fin 3 → Foundation.Parabolic.Vec3)
:
Extending the spatial gradient by zero off positive spacetime preserves measurability, so the global dissipation can be integrated by slices.
Equations
Instances For
theorem
CKN.Leray.regTails_positiveGradientExtension_measurable
(D : Foundation.Parabolic.ParabolicPoint → Fin 3 → Foundation.Parabolic.Vec3)
(hDcont :
∀ (i j : Fin 3),
ContinuousOn (fun (z : Foundation.Parabolic.ParabolicPoint) => D z i j) (spaceTimeSet Set.univ (Set.Ioi 0)))
:
theorem
CKN.Leray.regTails_scalarTimeProduct_test
(q : Foundation.Parabolic.Vec3 → ℝ)
(hq : ContDiff ℝ (↑⊤) q)
(hqc : HasCompactSupport q)
(η : ℝ → ℝ)
(hη : ContDiff ℝ (↑⊤) η)
(hηc : HasCompactSupport η)
(hηI : tsupport η ⊆ Set.Ioi 0)
:
(fun (z : Foundation.Parabolic.Vec3 × ℝ) => q z.1 * η z.2) ∈ spaceTimeTestFunction Set.univ (Set.Ioi 0)
A product of compact smooth spatial and positive-time tests is an admissible scalar space-time test.
theorem
CKN.Leray.regTails_energy_bounds
(ρ : RegMollifierProfile)
(ε : ℝ)
(hε : 0 < ε)
(a : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3)
(u : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3)
(D : Foundation.Parabolic.ParabolicPoint → Fin 3 → Foundation.Parabolic.Vec3)
(hR5 :
∀ (t : ℝ),
0 ≤ t →
MeasureTheory.eLpNorm (regUniformVelocitySlice u t) 2 MeasureTheory.volume ^ 2 + 2 * regUniformDissipation u D t = MeasureTheory.eLpNorm (regMollifyVector ρ ε hε (regUniformSpatialField a)) 2 MeasureTheory.volume ^ 2)
(ha : MeasureTheory.MemLp a 2 MeasureTheory.volume)
(hDcont :
∀ (i j : Fin 3),
ContinuousOn (fun (z : Foundation.Parabolic.ParabolicPoint) => D z i j) (spaceTimeSet Set.univ (Set.Ioi 0)))
(hU : ∀ (t : ℝ), 0 ≤ t → MeasureTheory.MemLp (fun (x : Foundation.Parabolic.Vec3) => u (x, t)) 2 MeasureTheory.volume)
(hSpatialC1 : ∀ (t : ℝ), 0 < t → ∀ (i : Fin 3), ContDiff ℝ ↑1 fun (x : Foundation.Parabolic.Vec3) => u (x, t) i)
(hDerivative :
∀ (t : ℝ),
0 < t →
∀ (x : Foundation.Parabolic.Vec3) (i j : Fin 3),
(fderiv ℝ (fun (y : Foundation.Parabolic.Vec3) => u (y, t) i) x) (basisVec j) = D (x, t) i j)
:
(∀ (t : ℝ),
0 ≤ t →
MeasureTheory.eLpNorm (regUniformVelocitySlice u t) 2 MeasureTheory.volume ^ 2 ≤ MeasureTheory.eLpNorm (regUniformSpatialField a) 2 MeasureTheory.volume ^ 2) ∧ 2 * ∫⁻ (z : Foundation.Parabolic.ParabolicPoint), ENNReal.ofReal (spatialGradientSq u D z) ∂regUniformPositiveTimeMeasure ≤ MeasureTheory.eLpNorm (regUniformSpatialField a) 2 MeasureTheory.volume ^ 2 ∧ ∀ᵐ (t : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioi 0), ∃ (h : Fin 3 → H1Function Set.univ),
(∀ (i : Fin 3) (x : Vec 3), (h i).toFun x = u (x, t) i) ∧ ∀ (i : Fin 3) (x : Vec 3) (j : Fin 3), (h i).grad x j = D (x, t) i j
Slice energy, finite total dissipation, and almost every positive-time H¹
slice follow from the R5 identity in lem:reg-tails. The gradient is extended
measurably from positive time before applying the global energy estimate.