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Add lean source and binary files (part 90)
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import OAI.MathematicalPhysics.NavierStokes.ForcedComputation.Flow.PlanarCompactLift
namespace OAI
/-! A rational volume-independent coordinate change for the Euclidean cube
observer. The velocity is pushed forward; the force is subsequently defined
by its Navier--Stokes residual, so anisotropic diffusion causes no restriction. -/
noncomputable section
namespace ForcedComputation.BalancedStretch
open ShearFlows Set
open scoped ContDiff BigOperators
def coefficient (j : Fin 3) : ℝ := if j = 1 then 16 else 1
def linear : Space →L[ℝ] Space :=
ContinuousLinearMap.pi (fun j => coefficient j •
(ContinuousLinearMap.proj j : Space →L[ℝ] ℝ))
def inverseLinear : Space →L[ℝ] Space :=
ContinuousLinearMap.pi (fun j => (coefficient j)⁻¹ •
(ContinuousLinearMap.proj j : Space →L[ℝ] ℝ))
@[simp] theorem linear_apply (x : Space) (j : Fin 3) :
linear x j = coefficient j * x j := rfl
@[simp] theorem inverseLinear_apply (x : Space) (j : Fin 3) :
inverseLinear x j = (coefficient j)⁻¹ * x j := rfl
theorem coefficient_ne (j : Fin 3) : coefficient j ≠ 0 := by
simp only [coefficient]
split_ifs <;> norm_num
def stretch : Space ≃L[ℝ] Space :=
{ toLinearEquiv :=
{ toFun := linear
invFun := inverseLinear
left_inv := by
intro x
ext j
simp [coefficient_ne]
right_inv := by
intro x
ext j
simp [coefficient_ne]
map_add' := linear.map_add
map_smul' := linear.map_smul }
continuous_toFun := linear.continuous
continuous_invFun := inverseLinear.continuous }
@[simp] theorem stretch_apply (x : Space) (j : Fin 3) :
stretch x j = coefficient j * x j := rfl
@[simp] theorem stretch_symm_apply (x : Space) (j : Fin 3) :
stretch.symm x j = (coefficient j)⁻¹ * x j := rfl
@[simp] theorem stretch_symm_basis (j : Fin 3) :
stretch.symm (basis j) = (coefficient j)⁻¹ • basis j := by
ext k
by_cases h : k = j
· subst k
simp [basis]
· simp [basis, Pi.single_eq_of_ne h]
def push (a : Space → Space) (x : Space) : Space := stretch (a (stretch.symm x))
def velocity (V : Velocity) : Velocity := fun y => push (fun x => V (y.1, x)) y.2
theorem push_smooth {a : Space → Space} (ha : ContDiff ℝ ∞ a) :
ContDiff ℝ ∞ (push a) :=
stretch.contDiff.comp (ha.comp stretch.symm.contDiff)
theorem velocity_smooth {V : Velocity} (hV : ContDiff ℝ ∞ V) :
ContDiff ℝ ∞ (velocity V) :=
stretch.contDiff.comp
(hV.comp (contDiff_fst.prodMk (stretch.symm.contDiff.comp contDiff_snd)))
theorem push_derivative (a : Space → Space) (x : Space) (j : Fin 3) :
derivative (push a) j x =
(coefficient j)⁻¹ • stretch (derivative a j (stretch.symm x)) := by
change fderiv ℝ (stretch ∘ (a ∘ stretch.symm)) x (basis j) = _
rw [stretch.comp_fderiv, stretch.symm.comp_right_fderiv]
simp only [ContinuousLinearMap.comp_apply, ContinuousLinearEquiv.coe_coe,
stretch_symm_basis, map_smul, derivative]
theorem push_divergence (a : Space → Space) (x : Space) :
divergence (push a) x = divergence a (stretch.symm x) := by
unfold divergence
apply Finset.sum_congr rfl
intro j _
rw [push_derivative]
simp only [Pi.smul_apply, smul_eq_mul, stretch_apply]
rw [← mul_assoc, inv_mul_cancel₀ (coefficient_ne j), one_mul]
theorem velocity_divergence {V : Velocity}
(hV : ∀ t x, divergence (fun y => V (t, y)) x = 0) (t : ℝ) (x : Space) :
divergence (fun y => velocity V (t, y)) x = 0 := by
exact (push_divergence _ _).trans (hV _ _)
theorem push_zero_iff (a : Space → Space) (x : Space) :
push a x = 0 ↔ a (stretch.symm x) = 0 := by
change stretch _ = 0 ↔ _
exact stretch.map_eq_zero_iff
theorem push_support {a : Space → Space} {K : Set Space}
(hK : IsClosed K) (ha : tsupport a ⊆ K) :
tsupport (push a) ⊆ stretch '' K := by
apply closure_minimal
· intro x hx
refine ⟨stretch.symm x, ha ?_, by simp⟩
exact subset_tsupport _ ((push_zero_iff a x).not.mp hx)
· exact stretch.toHomeomorph.isClosedMap _ hK
theorem push_compact {a : Space → Space} (ha : HasCompactSupport a) :
HasCompactSupport (push a) :=
(ha.image stretch.continuous).of_isClosed_subset (isClosed_tsupport _)
(push_support (isClosed_tsupport _) (Subset.refl _))
theorem trajectory {V : Velocity} {γ : ℝ → Space} {a t : ℝ}
(hγ : HasDerivAt γ (V (a + t, γ t)) t) :
HasDerivAt (fun s => stretch (γ s))
(velocity V (a + t, stretch (γ t))) t := by
apply hasDerivAt_pi.mpr
intro j
simpa only [velocity, push, stretch_apply, ContinuousLinearEquiv.symm_apply_apply]
using ((hasDerivAt_pi.mp hγ) j).const_mul (coefficient j)
/-- The cube used by the balanced Euclidean main result. -/
def observer : Set Space := {x | ∀ j : Fin 3, -1 < x j ∧ x j < 2}
theorem nonhalting_outside {x : Plane} (hx : 3 / 16 ≤ x 1) :
stretch (atHeight x 0) ∉ observer := by
intro h
have h₁ := (h (1 : Fin 3)).2
change coefficient 1 * x 1 < 2 at h₁
norm_num [coefficient] at h₁
linarith
theorem halting_inside {x : Plane} (hx : 0 < x 0 ∧ x 0 < 1)
(hy : 1 / 16 ≤ x 1 ∧ x 1 ≤ 3 / 32) :
stretch (atHeight x 0) ∈ observer := by
intro j
fin_cases j <;> simp only [stretch_apply, coefficient, atHeight]
· norm_num
constructor <;> linarith [hx.1, hx.2]
· norm_num
constructor <;> linarith [hy.1, hy.2]
· norm_num
/-- A straight loading path stays outside the cube whenever its endpoint
satisfies `x₀+x₁≥4`. This lets the body use a fixed machine-only normalization. -/
theorem loading_outside {p : Space} (hp : 4 ≤ p 0 + p 1)
{θ : ℝ} (hθ : θ ∈ Icc (0 : ℝ) 1) :
(1 - θ) • ![4, 0, 0] + θ • p ∉ observer := by
intro h
have h₀ := (h (0 : Fin 3)).2
have h₁ := (h (1 : Fin 3)).2
simp only [Pi.add_apply, Pi.smul_apply, smul_eq_mul,
Matrix.cons_val_zero, Matrix.cons_val_one, mul_zero, zero_add] at h₀ h₁
have hs : 4 ≤ (1 - θ) * 4 + θ * p 0 + θ * p 1 := by
nlinarith [mul_nonneg hθ.1 (sub_nonneg.mpr hp)]
linarith
end ForcedComputation.BalancedStretch
end
end OAI