The energy estimate for the smooth forced heat response #
Testing the forced heat equation with the response itself gives, for every
t₁ ≥ 0,
‖Z(t₁)‖₂² + ∫₀^{t₁} ‖∇Z‖₂² ≤ ∫₀^{t₁} ‖g‖₂²,
the smooth-data form of eq:pv-stokes-energy in lem:pv-stokes.
theorem
ESS.response_sq_window_integrable
{g : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ}
(hg : ∀ (i j : Fin 3), ContDiff ℝ (↑⊤) (g i j))
(hgc : ∀ (i j : Fin 3), HasCompactSupport (g i j))
(a b : ℝ)
:
MeasureTheory.Integrable
(fun (p : CKN.Foundation.Parabolic.Vec3 × ℝ) => ∑ i : Fin 3, ∑ j : Fin 3, responseGrad g j p i ^ 2)
(MeasureTheory.volume.prod (MeasureTheory.volume.restrict (Set.Ioc a b))) ∧ MeasureTheory.Integrable (fun (p : CKN.Foundation.Parabolic.Vec3 × ℝ) => ∑ i : Fin 3, ∑ j : Fin 3, g i j p ^ 2)
(MeasureTheory.volume.prod (MeasureTheory.volume.restrict (Set.Ioc a b))) ∧ MeasureTheory.Integrable
(fun (p : CKN.Foundation.Parabolic.Vec3 × ℝ) =>
∑ i : Fin 3, ∑ j : Fin 3, responseGrad g j p i * (responseGrad g j p i + g i j p))
(MeasureTheory.volume.prod (MeasureTheory.volume.restrict (Set.Ioc a b)))
The response and its spatial gradient have space-time integrable squares on each finite window, and the squared tensor is integrable there.
theorem
ESS.response_energy_le
{g : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ}
(hg : ∀ (i j : Fin 3), ContDiff ℝ (↑⊤) (g i j))
(hgc : ∀ (i j : Fin 3), HasCompactSupport (g i j))
(hgpos : ∀ (i j : Fin 3), tsupport (g i j) ⊆ {p : CKN.Foundation.Parabolic.Vec3 × ℝ | 0 < p.2})
{t₁ : ℝ}
(ht₁ : 0 ≤ t₁)
:
(∫ (x : CKN.Foundation.Parabolic.Vec3), ∑ i : Fin 3, responseVec g (x, t₁) i ^ 2) + ∫ (p : CKN.Foundation.Parabolic.Vec3 × ℝ), ∑ i : Fin 3,
∑ j : Fin 3,
responseGrad g j p i ^ 2 ∂MeasureTheory.volume.prod (MeasureTheory.volume.restrict (Set.Ioc 0 t₁)) ≤ ∫ (p : CKN.Foundation.Parabolic.Vec3 × ℝ), ∑ i : Fin 3, ∑ j : Fin 3, g i j p ^ 2 ∂MeasureTheory.volume.prod (MeasureTheory.volume.restrict (Set.Ioc 0 t₁))
The energy estimate for the smooth forced heat response: for every t₁ ≥ 0,
‖Z(t₁)‖₂² + ∫_{(0,t₁]} ‖∇Z‖₂² ≤ ∫_{(0,t₁]} ‖g‖₂².