openAI-math-dataset / lean /OAI /Analysis /Conductivity /Flux /PhysicalTensorPatch.lean
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Add lean source and binary files (part 15)
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import Mathlib
import OAI.Analysis.Conductivity.Branching.AttachedFlatTransport
namespace OAI
noncomputable section
namespace ScalarConductivity
open Set MeasureTheory Matrix
open scoped Matrix.Norms.Elementwise
local instance physicalTensorPatchMeasurableSpace :
MeasurableSpace (Matrix (Fin 3) (Fin 3) ℝ) := borel _
local instance physicalTensorPatchBorelSpace : BorelSpace (Matrix (Fin 3) (Fin 3) ℝ) := ⟨rfl⟩
def sourceFlatPatch (i j : Fin 4) : Set (Fin 3 → ℝ) :=
sourceCollarPiece i j '' sourceExtendedBox (-(1:ℝ)/100) (1/100)
lemma isCompact_sourceFlatPatch (i j : Fin 4) : IsCompact (sourceFlatPatch i j) :=
isCompact_Icc.image (sourceCollarPiece_contDiff i j).continuous
lemma continuousAt_sourceCollarInverse_patch (i j : Fin 4) {y : Fin 3 → ℝ}
(hy : y∈sourceFlatPatch i j) : ContinuousAt (sourceCollarInverse i j) y := by
obtain ⟨x,hx,rfl⟩ := hy
obtain ⟨ht,hi,hj⟩ := mem_sourceExtendedBox.mp hx
have hr : 0<sourceCollarRadius j (x 0) (x 2) :=
(by norm_num : (0:ℝ)<1/50).trans_le (sourceCollarRadius_extended j ht hj).1
have hrad := sourceCollarPiece_radial_pos i j hr.le hi
have htime := sourceCollarPiece_time_pos i j hr.le (by linarith [ht.2] : x 0≤1) hi hj
have hc : Continuous sourceCollarTime := by
unfold sourceCollarTime sourceCrossCoordinates sourceRadial
fun_prop
have hcR : Continuous sourceRadial := by unfold sourceRadial; fun_prop
have hcX : Continuous sourceCrossCoordinates := by
unfold sourceCrossCoordinates sourceRadial
fun_prop
unfold sourceCollarInverse
apply continuousAt_pi.mpr
intro k
fin_cases k
· exact hc.continuousAt
· apply ContinuousAt.div
· unfold squareFaceParameter
fun_prop
· exact hcR.continuousAt
· rw [hrad]
exact hr.ne'
· apply ContinuousAt.div
· exact ((show Continuous (squareFaceParameter j) by
unfold squareFaceParameter; fun_prop).comp hcX).continuousAt
· exact continuousAt_const.sub hc.continuousAt
· rw [htime]
linarith [ht.2]
lemma continuousOn_attachedPhysicalFlatTensor (s : Fin 3 → ℝ) {a : ℝ} (ha : a≠0)
(i j : Fin 4) : ContinuousOn (attachedPhysicalFlatTensor s a i j) (sourceFlatPatch i j) := by
apply (continuousOn_attachedFlatTensor s ha i j).comp
(fun y hy => (continuousAt_sourceCollarInverse_patch i j hy).continuousWithinAt)
rintro _ ⟨x,hx,rfl⟩
simpa only [sourceCollarInverse_extended i j (le_refl _) (le_refl _) hx] using hx
def attachedPatchTensor (s : Fin 3 → ℝ) (a : ℝ) (i j : Fin 4)
(y : Fin 3 → ℝ) : Matrix (Fin 3) (Fin 3) ℝ :=
by classical exact if y∈sourceFlatPatch i j then attachedPhysicalFlatTensor s a i j y else 1
lemma measurable_attachedPatchTensor (s : Fin 3 → ℝ) {a : ℝ} (ha : a≠0)
(i j : Fin 4) : Measurable (attachedPatchTensor s a i j) := by
classical
exact (continuousOn_attachedPhysicalFlatTensor s ha i j).measurable_piecewise
continuousOn_const (isCompact_sourceFlatPatch i j).isClosed.measurableSet
lemma attachedPatchTensor_symmetric (s : Fin 3 → ℝ) (a : ℝ) (i j : Fin 4)
(y : Fin 3 → ℝ) : (attachedPatchTensor s a i j y)ᵀ=attachedPatchTensor s a i j y := by
classical
unfold attachedPatchTensor
split_ifs
· exact attachedPhysicalFlatTensor_symmetric s a i j y
· exact Matrix.transpose_one
end ScalarConductivity
end
noncomputable section
namespace ScalarConductivity
open Set MeasureTheory Matrix
open scoped Matrix.Norms.Elementwise
local instance attachedFaceTensorListMeasurableSpace :
MeasurableSpace (Matrix (Fin 3) (Fin 3) ℝ) := borel _
local instance attachedFaceTensorListBorelSpace : BorelSpace (Matrix (Fin 3) (Fin 3) ℝ) := ⟨rfl⟩
def attachedFaceTensorList (s : Fin 3 → ℝ) (a : ℝ) (ks : List (Fin 4 × Fin 4))
(y : Fin 3 → ℝ) : Matrix (Fin 3) (Fin 3) ℝ := by
classical
exact ks.foldr (fun k A => if y∈sourceFlatPatch k.1 k.2 then
attachedPatchTensor s a k.1 k.2 y else A) 1
lemma attachedFaceTensorList_cons (s : Fin 3 → ℝ) (a : ℝ)
(k : Fin 4 × Fin 4) (ks : List (Fin 4 × Fin 4)) (y : Fin 3 → ℝ) :
attachedFaceTensorList s a (k::ks) y=
(by classical exact if y∈sourceFlatPatch k.1 k.2 then attachedPatchTensor s a k.1 k.2 y
else attachedFaceTensorList s a ks y) := by
classical
rfl
lemma attachedFaceTensorList_measurable (s : Fin 3 → ℝ) {a : ℝ} (ha : a≠0)
(ks : List (Fin 4 × Fin 4)) : Measurable (attachedFaceTensorList s a ks) := by
classical
induction ks with
| nil => exact measurable_const
| cons k ks ih =>
exact Measurable.ite (isCompact_sourceFlatPatch k.1 k.2).isClosed.measurableSet
(measurable_attachedPatchTensor s ha k.1 k.2) ih
lemma attachedFaceTensorList_symmetric (s : Fin 3 → ℝ) (a : ℝ)
(ks : List (Fin 4 × Fin 4)) (y : Fin 3 → ℝ) :
(attachedFaceTensorList s a ks y)ᵀ=attachedFaceTensorList s a ks y := by
classical
induction ks with
| nil => exact Matrix.transpose_one
| cons k ks ih =>
simp only [attachedFaceTensorList_cons]
split_ifs
· exact attachedPatchTensor_symmetric s a k.1 k.2 y
· exact ih
lemma identity_matrix_energy_bounds : ∃ c C : ℝ,0<c ∧ c<C ∧ ∀ v : Fin 3 → ℝ,
c*‖v‖^2≤v ⬝ᵥ ((1 : Matrix (Fin 3) (Fin 3) ℝ)*ᵥv) ∧
v ⬝ᵥ ((1 : Matrix (Fin 3) (Fin 3) ℝ)*ᵥv)≤C*‖v‖^2 := by
have hp (u : Unit) (_ : u∈({()} : Set Unit)) (v : Fin 3 → ℝ) (hv : v≠0) :
0<v ⬝ᵥ ((1 : Matrix (Fin 3) (Fin 3) ℝ)*ᵥv) := by
rw [Matrix.one_mulVec]
exact lt_of_le_of_ne (Finset.sum_nonneg (fun k _ => mul_self_nonneg (v k)))
(Ne.symm (mt dotProduct_self_eq_zero.mp hv))
obtain ⟨c,C,hc,hcC,h⟩ := compact_matrix_energy_bounds isCompact_singleton
(fun _ : Unit => (1 : Matrix (Fin 3) (Fin 3) ℝ)) continuousOn_const hp
exact ⟨c,C,hc,hcC,h () (mem_singleton ())⟩
lemma attachedFaceTensorList_elliptic (s : Fin 3 → ℝ)
(hs : ∀ x y : ℝ,(1/2)*(x^2+y^2) ≤ s 0*x^2+2*s 1*x*y+s 2*y^2)
{a : ℝ} (ha : a≠0) (ks : List (Fin 4 × Fin 4)) :
∃ c C : ℝ,0<c ∧ c<C ∧ ∀ y (v : Fin 3 → ℝ),
c*‖v‖^2≤v ⬝ᵥ (attachedFaceTensorList s a ks y*ᵥv) ∧
v ⬝ᵥ (attachedFaceTensorList s a ks y*ᵥv)≤C*‖v‖^2 := by
classical
induction ks with
| nil =>
obtain ⟨c,C,hc,hcC,h⟩ := identity_matrix_energy_bounds
exact ⟨c,C,hc,hcC,fun _ => h⟩
| cons k ks ih =>
obtain ⟨c,C,hc,hcC,h⟩ := ih
obtain ⟨d,D,hd,hdD,hk⟩ := attachedPhysicalFlatTensor_elliptic s hs ha k.1 k.2
refine ⟨min c d,max C D,lt_min hc hd,
lt_of_le_of_lt (min_le_left _ _) (hcC.trans_le (le_max_left _ _)),?_⟩
intro y v
simp only [attachedFaceTensorList_cons]
by_cases hy : y∈sourceFlatPatch k.1 k.2
· simp only [ite_eq_left hy,attachedPatchTensor]
exact ⟨(mul_le_mul_of_nonneg_right (min_le_right _ _) (sq_nonneg _)).trans
(hk y hy v).1,
(hk y hy v).2.trans (mul_le_mul_of_nonneg_right (le_max_right _ _) (sq_nonneg _))⟩
· simp only [ite_eq_right hy]
exact ⟨(mul_le_mul_of_nonneg_right (min_le_left _ _) (sq_nonneg _)).trans
(h y v).1,
(h y v).2.trans (mul_le_mul_of_nonneg_right (le_max_left _ _) (sq_nonneg _))⟩
lemma attachedFaceTensorList_outside (s : Fin 3 → ℝ) (a : ℝ)
(ks : List (Fin 4 × Fin 4)) (y : Fin 3 → ℝ)
(hy : ∀ k∈ks,y∉sourceFlatPatch k.1 k.2) : attachedFaceTensorList s a ks y=1 := by
classical
induction ks with
| nil => rfl
| cons k ks ih =>
simpa only [attachedFaceTensorList,List.foldr_cons,ite_eq_right (hy k (List.mem_cons_self))]
using ih (fun l hl => hy l (List.mem_cons_of_mem k hl))
lemma attachedFaceTensorList_local (s : Fin 3 → ℝ) (a : ℝ)
(ks : List (Fin 4 × Fin 4)) (y : Fin 3 → ℝ)
(hy : ∃ k∈ks,y∈sourceFlatPatch k.1 k.2) :
∃ k∈ks,y∈sourceFlatPatch k.1 k.2 ∧
attachedFaceTensorList s a ks y=attachedPhysicalFlatTensor s a k.1 k.2 y := by
classical
induction ks with
| nil => simp at hy
| cons k ks ih =>
by_cases hk : y∈sourceFlatPatch k.1 k.2
· refine ⟨k,List.mem_cons_self,hk,?_⟩
simp only [attachedFaceTensorList,List.foldr_cons,ite_eq_left hk,attachedPatchTensor]
· obtain ⟨l,hl,hy⟩ := hy
obtain ⟨l,hl,hly,he⟩ := ih ⟨l,(List.mem_cons.mp hl).resolve_left
(fun e => hk (e ▸ hy)),hy⟩
refine ⟨l,List.mem_cons_of_mem k hl,hly,?_⟩
simpa only [attachedFaceTensorList,List.foldr_cons,ite_eq_right hk] using he
def attachedCollarTensor (s : Fin 3 → ℝ) (a : ℝ) :
(Fin 3 → ℝ) → Matrix (Fin 3) (Fin 3) ℝ :=
attachedFaceTensorList s a (Finset.univ : Finset (Fin 4 × Fin 4)).toList
theorem attachedCollarTensor_properties (s : Fin 3 → ℝ)
(hs : ∀ x y : ℝ,(1/2)*(x^2+y^2) ≤ s 0*x^2+2*s 1*x*y+s 2*y^2)
{a : ℝ} (ha : a≠0) :
Measurable (attachedCollarTensor s a) ∧
(∀ y,(attachedCollarTensor s a y)ᵀ=attachedCollarTensor s a y) ∧
(∃ c C : ℝ,0<c ∧ c<C ∧ ∀ y (v : Fin 3 → ℝ),
c*‖v‖^2≤v ⬝ᵥ (attachedCollarTensor s a y*ᵥv) ∧
v ⬝ᵥ (attachedCollarTensor s a y*ᵥv)≤C*‖v‖^2) ∧
(∀ y,(∀ i j,y∉sourceFlatPatch i j) → attachedCollarTensor s a y=1) ∧
(∀ y,(∃ i j,y∈sourceFlatPatch i j) → ∃ i j,y∈sourceFlatPatch i j ∧
attachedCollarTensor s a y=attachedPhysicalFlatTensor s a i j y) := by
refine ⟨attachedFaceTensorList_measurable s ha _,
attachedFaceTensorList_symmetric s a _,attachedFaceTensorList_elliptic s hs ha _,?_,?_⟩
· intro y hy
exact attachedFaceTensorList_outside s a _ y (fun k _ => hy k.1 k.2)
· rintro y ⟨i,j,hy⟩
obtain ⟨k,_,hk,he⟩ := attachedFaceTensorList_local s a
(Finset.univ : Finset (Fin 4 × Fin 4)).toList y ⟨(i,j),by simp,hy⟩
exact ⟨k.1,k.2,hk,he⟩
end ScalarConductivity
end
end OAI