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import OAI.MathematicalPhysics.NavierStokes.ForcedComputation.Detector.CylinderCompactCalculus
import Mathlib.MeasureTheory.Integral.IntervalIntegral.FundThmCalculus
namespace OAI
/-! Integration of first derivatives in the horizontal directions and
over one vertical period. Only C¹ regularity is needed. -/
noncomputable section
namespace ForcedComputation.VelocityDetector.CylinderLocalCalculus
open ShearFlows Set MeasureTheory Filter
open scoped ContDiff Topology
theorem plane_integral_derivative_zero {g : Plane → ℝ} (hg : ContDiff ℝ 1 g)
(hc : HasCompactSupport g) (j : Fin 2) :
(∫ x, fderiv ℝ g x (PlanarHamiltonian.basis j)) = 0 := by
have hD : Integrable (fun x => fderiv ℝ g x (PlanarHamiltonian.basis j)) :=
((hg.continuous_fderiv (by norm_num)).clm_apply continuous_const).integrable_of_hasCompactSupport
(hc.fderiv_apply ℝ (PlanarHamiltonian.basis j))
have hI : Integrable g := hg.continuous.integrable_of_hasCompactSupport hc
have h := integral_mul_fderiv_eq_neg_fderiv_mul_of_integrable
(μ := (volume : Measure Plane)) (f := fun _ : Plane => (1 : ℝ)) (g := g)
(v := PlanarHamiltonian.basis j) (by simp)
(by simpa only [one_mul] using hD) (by simpa only [one_mul] using hI)
(fun _ _ => differentiableAt_const 1)
(fun x _ => hg.differentiable (by norm_num) x)
simpa only [one_mul, fderiv_const_apply, zero_apply, zero_mul, integral_zero,
neg_zero] using h
theorem vertical_integral_derivative_zero {g : ℝ → ℝ} (hg : ContDiff ℝ 1 g)
(hp : g 1 = g 0) : (∫ z, deriv g z ∂verticalPeriodMeasure) = 0 := by
have h := intervalIntegral.integral_eq_sub_of_hasDerivAt
(a := (0 : ℝ)) (b := 1)
(fun z _ => (hg.differentiable (by norm_num) z).hasDerivAt)
((hg.continuous_deriv (by norm_num)).intervalIntegrable 0 1)
rw [hp, sub_self] at h
simpa only [verticalPeriodMeasure, intervalIntegral.integral_of_le zero_le_one,
integral_Icc_eq_integral_Ioc] using h
theorem atHeight_smooth : ContDiff ℝ ∞ (fun y : Plane × ℝ => atHeight y.1 y.2) := by
apply contDiff_pi.mpr
intro j
fin_cases j <;> dsimp [atHeight] <;> fun_prop
theorem scalarSpatialD_horizontal_support {g : Space → ℝ} {K : Set Plane}
(hK : IsClosed K) (hs : ∀ x, horizontal x ∉ K → g x = 0)
(j : Fin 3) (x : Space) (hx : horizontal x ∉ K) : scalarSpatialD j g x = 0 := by
have hn : ∀ᶠ y in 𝓝 x, horizontal y ∉ K :=
(hK.isOpen_compl.preimage (show Continuous horizontal from by
apply continuous_pi
intro j
fin_cases j <;> dsimp [horizontal] <;> fun_prop)).mem_nhds hx
have he : g =ᶠ[𝓝 x] (fun _ => 0) := hn.mono (fun y hy => hs y hy)
simp only [scalarSpatialD, he.fderiv_eq, fderiv_const_apply]
rfl
theorem scalarSpatialD_cylinder_integrable {g : Space → ℝ} (hg : ContDiff ℝ 1 g)
{K : Set Plane} (hK : IsCompact K) (hs : ∀ x, horizontal x ∉ K → g x = 0)
(j : Fin 3) :
Integrable (fun y => scalarSpatialD j g (atHeight y.1 y.2)) cylinderMeasure := by
apply integrable_horizontal_compact
(((hg.continuous_fderiv (by norm_num)).clm_apply continuous_const).comp
atHeight_smooth.continuous) hK
intro y hy
apply scalarSpatialD_horizontal_support hK.isClosed hs
simpa only [atHeight_horizontal] using hy
theorem integral_horizontal_scalarD_zero {g : Space → ℝ} (hg : ContDiff ℝ 1 g)
{K : Set Plane} (hK : IsCompact K) (hs : ∀ x, horizontal x ∉ K → g x = 0)
(j : Fin 2) :
(∫ y, scalarSpatialD j.castSucc g (atHeight y.1 y.2) ∂cylinderMeasure) = 0 := by
rw [cylinderMeasure, integral_prod_symm _ (scalarSpatialD_cylinder_integrable hg hK hs _)]
have hz (z : ℝ) : (∫ x : Plane, scalarSpatialD j.castSucc g (atHeight x z)) = 0 := by
have hi : ContDiff ℝ 1 (fun x : Plane => atHeight x z) := by
apply contDiff_pi.mpr
intro i
fin_cases i <;> dsimp [atHeight] <;> fun_prop
have hcs : HasCompactSupport (fun x : Plane => g (atHeight x z)) := by
apply HasCompactSupport.intro hK
intro x hx
apply hs
simpa only [atHeight_horizontal] using hx
have he (x : Plane) : scalarSpatialD j.castSucc g (atHeight x z) =
fderiv ℝ (fun X : Plane => g (atHeight X z)) x (PlanarHamiltonian.basis j) := by
have hd := (hg.differentiable (by norm_num) (atHeight x z)).hasFDerivAt.comp x
(atHeight_hasFDerivAt x z)
change HasFDerivAt (fun X : Plane => g (atHeight X z)) _ x at hd
rw [hd.fderiv]
simp only [ContinuousLinearMap.comp_apply, planeInclusion_basis, scalarSpatialD]
simp_rw [he]
exact plane_integral_derivative_zero (hg.comp hi) hcs j
simp only [hz, integral_zero]
theorem integral_vertical_scalarD_zero {g : Space → ℝ} (hg : ContDiff ℝ 1 g)
{K : Set Plane} (hK : IsCompact K) (hs : ∀ x, horizontal x ∉ K → g x = 0)
(hp : VerticallyPeriodic g) :
(∫ y, scalarSpatialD 2 g (atHeight y.1 y.2) ∂cylinderMeasure) = 0 := by
rw [cylinderMeasure, integral_prod _ (scalarSpatialD_cylinder_integrable hg hK hs _)]
have hz (x : Plane) :
(∫ z, scalarSpatialD 2 g (atHeight x z) ∂verticalPeriodMeasure) = 0 := by
have hi : ContDiff ℝ 1 (fun z : ℝ => atHeight x z) := by
apply contDiff_pi.mpr
intro i
fin_cases i <;> dsimp [atHeight] <;> fun_prop
have he (z : ℝ) : scalarSpatialD 2 g (atHeight x z) =
deriv (fun Z : ℝ => g (atHeight x Z)) z := by
have hmap : HasDerivAt (fun Z : ℝ => atHeight x Z) (basis 2) z := by
apply hasDerivAt_pi.mpr
intro i
fin_cases i
· simpa [atHeight, basis] using hasDerivAt_const z (x 0)
· simpa [atHeight, basis] using hasDerivAt_const z (x 1)
· change HasDerivAt (fun z : ℝ => z) 1 z
exact (hasFDerivAt_id (𝕜 := ℝ) z).hasDerivAt
exact ((hg.differentiable (by norm_num) _).hasFDerivAt.comp_hasDerivAt z hmap).deriv.symm
have heq : atHeight x 1 = atHeight x 0 + (1 : ℝ) • basis 2 := by
ext i
fin_cases i <;> simp [atHeight, basis]
have hperiod : g (atHeight x 1) = g (atHeight x 0) := by
rw [heq]
simpa only [Int.cast_one] using hp (atHeight x 0) 1
simp_rw [he]
exact vertical_integral_derivative_zero (hg.comp hi) hperiod
simp only [hz, integral_zero]
end ForcedComputation.VelocityDetector.CylinderLocalCalculus
end
end OAI