roseking's picture
Add lean source and binary files (part 90)
37bcf52 verified
Raw History Blame Contribute Delete
20 kB
import OAI.MathematicalPhysics.Elasticity.BoundaryEnergy
namespace OAI
section
/-! Strictly positive Gaussian-normal moments, without relying on a numerical
constant or an unproved nondegeneracy of the boundary limit. -/
noncomputable section
open Set MeasureTheory
open scoped BigOperators
namespace ElasticityBoundaryWeights
lemma weight_zero_of_nonpos (b : ℝ) {y : Y} (hy : y 2≤0) : weight b y=0 := by
simp [weight,Fin.prod_univ_three,factor,not_lt.mpr hy]
lemma weight_pos (b : ℝ) {y : Y} (hy : 0<y 2) : 0<weight b y := by
simp [weight,Fin.prod_univ_three,factor,hy,Real.exp_pos]
def normalMoment (n : ℕ) : ℝ := ∫ y : Y, (y 2)^n*weight 2 y
lemma normal_moment_integrable (n : ℕ) : Integrable (fun y : Y => (y 2)^n*weight 2 y) := by
apply (integrable_coordinate_moment (by norm_num : (0:ℝ)<2) 2 n).congr
exact Filter.Eventually.of_forall (fun y => by
dsimp only
by_cases hy : 0<y 2
· rw [abs_of_pos hy]
· rw [weight_zero_of_nonpos 2 (le_of_not_gt hy),mul_zero,mul_zero])
lemma normalMoment_pos (n : ℕ) : 0<normalMoment n := by
have hn (y : Y) : 0≤(y 2)^n*weight 2 y := by
by_cases hy : 0<y 2
· exact mul_nonneg (pow_nonneg hy.le n) (weight_nonneg 2 y)
· rw [weight_zero_of_nonpos 2 (le_of_not_gt hy),mul_zero]
apply (integral_pos_iff_support_of_nonneg hn (normal_moment_integrable n)).mpr
have ho : IsOpen ({y : Y | 0<y 2}) := isOpen_lt continuous_const (continuous_apply 2)
have hne : ({y : Y | 0<y 2}).Nonempty := ⟨fun _ => 1,by norm_num⟩
exact (ho.measure_pos volume hne).trans_le (measure_mono (fun y hy =>
(mul_pos (pow_pos hy _) (weight_pos 2 hy)).ne'))
lemma normalMoment_complex (n : ℕ) :
(∫ y : Y, weight 2 y • (y 2:ℂ)^n)=(normalMoment n:ℂ) := by
simp only [Complex.real_smul,← Complex.ofReal_pow,← Complex.ofReal_mul]
rw [integral_complex_ofReal]
congr 1
apply integral_congr_ae
exact Filter.Eventually.of_forall (fun y => mul_comm _ _)
end ElasticityBoundaryWeights
end
end
section
/-! The finite leading packet pairing is precisely the integrated Hermitian
isotropic density, against a strictly positive normal Gaussian moment. -/
noncomputable section
open Set Filter MeasureTheory
open scoped Topology BigOperators
namespace ElasticityBoundaryPacket
open Elasticity ElasticityBoundaryMVNormal ElasticityBoundaryMVCalculus
ElasticityBoundaryWeights ElasticityBoundaryOrderBound ElasticityBoundaryProfileBounds
ElasticityBoundaryLimit ElasticityBoundaryParameter ElasticityBoundaryEnergyLimit
ElasticityBoundaryCutoffBound
lemma polynomial_bound (p : MP) : OrderBound (fun _ y => value p y) 0 := by
obtain ⟨A,hA,n,h⟩ := polynomialGrowth p
exact ⟨A,hA,n,fun _ _ _ y => by simpa using h y⟩
lemma weighted_integrable {f : Y → ℂ} (hf : Continuous f)
(hF : OrderBound (fun _ => f) 0) {b : ℝ} (hb : 0<b) :
Integrable (fun y => weight b y • f y) := by
obtain ⟨A,hA,n,hB⟩ := hF
let g : Y → ℝ := fun y => (A*2^n)*(weight b y+‖y‖^n*weight b y)
have hg : Integrable g := ((integrable_weight hb).add (integrable_norm_moment hb n)).const_mul _
apply hg.mono' ((measurable_weight b).aestronglyMeasurable.smul hf.aestronglyMeasurable)
exact Eventually.of_forall (fun y => by
change ‖weight b y • f y‖≤g y
rw [norm_smul,Real.norm_eq_abs,abs_of_nonneg (weight_nonneg b y)]
have h := hB 1 (by norm_num) le_rfl y
simp only [pow_zero,mul_one] at h
calc
_ ≤ weight b y*(A*(1+‖y‖)^n) := mul_le_mul_of_nonneg_left h (weight_nonneg b y)
_ ≤ weight b y*(A*(2^n*(1+‖y‖^n))) :=
mul_le_mul_of_nonneg_left (mul_le_mul_of_nonneg_left (one_add_pow_le (norm_nonneg y) n) hA)
(weight_nonneg b y)
_ = g y := by dsimp [g]; ring)
lemma frozen_integrable (n : ℕ) (c : ℂ) (p q : MP) :
Integrable (fun y : Y => weight 2 y • ((y 2:ℂ)^n*c*value p y*star (value q y))) := by
apply weighted_integrable
· exact ((((Complex.continuous_ofReal.comp (continuous_apply 2)).pow n).mul continuous_const).mul
(smooth_value p).continuous).mul (smooth_value q).continuous.star
· have hc : OrderBound (fun (_ : ℝ) (_ : Y) => c) 0 := by
exact ⟨‖c‖,norm_nonneg _,0,fun _ _ _ _ => by simp⟩
exact (((normal_power_bound n).mul hc).mul (polynomial_bound p)).mul (OrderBound.conj (polynomial_bound q))
· norm_num
lemma frozenPair_integral (n : ℕ) (a : I → I → I → I → ℂ) (p q : W) :
frozenPair n a p q=∫ y : Y, weight 2 y • ((y 2:ℂ)^n*
tensorDensity a (fun i α => value (E₀ α (p i)) y) (fun j β => value (E₀ β (q j)) y)) := by
have hi (i α j β : I) := frozen_integrable n (a i α j β) (E₀ α (p i)) (E₀ β (q j))
have hfun (y : Y) : weight 2 y • ((y 2:ℂ)^n*
tensorDensity a (fun i α => value (E₀ α (p i)) y) (fun j β => value (E₀ β (q j)) y))=
∑ i, ∑ α, ∑ j, ∑ β, weight 2 y • ((y 2:ℂ)^n*a i α j β*
value (E₀ α (p i)) y*star (value (E₀ β (q j)) y)) := by
simp only [tensorDensity,Finset.mul_sum,Finset.smul_sum,mul_assoc]
simp_rw [hfun]
unfold frozenPair
symm
rw [integral_finsetSum _ (fun i _ => integrable_finsetSum _ (fun α _ =>
integrable_finsetSum _ (fun j _ => integrable_finsetSum _ (fun β _ => hi i α j β))))]
apply Finset.sum_congr rfl; intro i _
rw [integral_finsetSum _ (fun α _ => integrable_finsetSum _ (fun j _ =>
integrable_finsetSum _ (fun β _ => hi i α j β)))]
apply Finset.sum_congr rfl; intro α _
rw [integral_finsetSum _ (fun j _ => integrable_finsetSum _ (fun β _ => hi i α j β))]
apply Finset.sum_congr rfl; intro j _
exact integral_finsetSum _ (fun β _ => hi i α j β)
lemma frozenPair_constant (n : ℕ) (a : I → I → I → I → ℂ) (p q : W) (c : ℂ)
(h : ∀ y : Y, tensorDensity a (fun i α => value (E₀ α (p i)) y)
(fun j β => value (E₀ β (q j)) y)=c) :
frozenPair n a p q=(normalMoment n:ℂ)*c := by
rw [frozenPair_integral]
simp only [h,Complex.real_smul,← mul_assoc]
rw [integral_mul_const]
congr 1
exact normalMoment_complex n
end ElasticityBoundaryPacket
end
end
section
/-! Exact transverse and longitudinal frozen physical tests. Both are genuine
solutions of the normal isotropic elasticity equation. -/
noncomputable section
open scoped BigOperators Matrix
namespace ElasticityBoundaryLeading
open Elasticity ElasticityBoundarySymbol ElasticityBoundaryMVNormal
ElasticityBoundaryMVCalculus ElasticityBoundaryParameter ElasticityBoundaryLayerOperator
abbrev I := Fin 3
abbrev Y := I → ℝ
def leading (l m : ℂ) (f : F) : W := fun i => lift (homogeneousPolynomial l m f i)
def grad (p : W) (y : Y) : CMatrix := fun i α => value (E₀ α (p i)) y
lemma leading_normal (l m : ℂ) (hp : l+3*m≠0) (f : F) : normal l m (leading l m f)=0 := by
change normal l m (fun i => lift (homogeneousPolynomial l m f i))=0
rw [normal_lift,homogeneousPolynomial_physical l m hp]
ext i
simp
lemma leading_apply (l m : ℂ) (f : F) (i : I) :
leading l m f i=MvPolynomial.C (f i)+MvPolynomial.X 2*MvPolynomial.C (ElasticityBoundarySymbol.slope l m f i) := by
simp only [leading,homogeneousPolynomial,map_add,map_mul,lift_C,lift_X]
lemma grad_leading (l m : ℂ) (f : F) (y : Y) (i α : I) :
grad (leading l m f) y i α=
if α=0 then Complex.I*(f i+(y 2:ℂ)*ElasticityBoundarySymbol.slope l m f i)
else if α=1 then 0 else ElasticityBoundarySymbol.slope l m f i-f i-(y 2:ℂ)*ElasticityBoundarySymbol.slope l m f i := by
rw [grad,leading_apply]
fin_cases α <;> simp [E₀,value_smul] <;> ring
lemma tensorDensity_factor (D : ℂ) (a : I → I → I → I → ℂ) (P Q : CMatrix) :
tensorDensity (fun i α j β => D*a i α j β) P Q=D*tensorDensity a P Q := by
simp only [tensorDensity,Finset.mul_sum,mul_assoc]
lemma transverse_density (l₁ m₁ l₂ m₂ L M : ℂ) (y : Y) :
tensorDensity (elasticityTensor L M)
(grad (leading l₁ m₁ ![0,1,0]) y) (grad (leading l₂ m₂ ![0,1,0]) y)=2*M := by
rw [tensorDensity_isotropic]
simp only [sesquiDensity,Fin.sum_univ_three,grad_leading]
simp [ElasticityBoundarySymbol.slope]
ring
lemma longitudinal_trace (l m : ℂ) (hp : l+3*m≠0) (y : Y) :
(∑ i, grad (leading l m ![1,0,0]) y i i)=Complex.I*(2*m/(l+3*m)) := by
simp [Fin.sum_univ_three,grad_leading,ElasticityBoundarySymbol.slope]
have hp' : l+m*3≠0 := by simpa only [mul_comm] using hp
field_simp [hp,hp']
ring
lemma longitudinal_density (l₁ m₁ l₂ m₂ : ℂ) (hp₁ : l₁+3*m₁≠0) (hp₂ : l₂+3*m₂≠0)
(L : ℂ) (y : Y) :
tensorDensity (elasticityTensor L 0)
(grad (leading l₁ m₁ ![1,0,0]) y) (grad (leading l₂ m₂ ![1,0,0]) y)=
L*(Complex.I*(2*m₁/(l₁+3*m₁)))*star (Complex.I*(2*m₂/(l₂+3*m₂))) := by
rw [tensorDensity_isotropic]
simp only [sesquiDensity,zero_div,zero_mul,add_zero,longitudinal_trace l₁ m₁ hp₁,
longitudinal_trace l₂ m₂ hp₂]
lemma longitudinal_trace_ne (l m : ℂ) (hm : m≠0) (hp : l+3*m≠0) :
Complex.I*(2*m/(l+3*m))≠0 :=
mul_ne_zero Complex.I_ne_zero (div_ne_zero (mul_ne_zero (by norm_num) hm) hp)
end ElasticityBoundaryLeading
end
end
section
/-! Nondegenerate extraction of the two genuine isotropic scalar coefficients.
Tests are the actual frozen normal solutions, not arbitrary symbol data. -/
noncomputable section
open scoped Matrix BigOperators
namespace ElasticityBoundaryPacket
open Elasticity ElasticityBoundaryLeading ElasticityBoundaryWeights
ElasticityBoundarySymbol ElasticityBoundaryMVNormal ElasticityBoundaryParameter ElasticityBoundaryLayerOperator
lemma pair_separates (n : ℕ) (l₁ m₁ l₂ m₂ D L M : ℂ)
(hm₁ : m₁≠0) (hm₂ : m₂≠0) (hp₁ : l₁+3*m₁≠0) (hp₂ : l₂+3*m₂≠0)
(hD : D≠0)
(h : ∀ p q : W, normal l₁ m₁ p=0 → normal l₂ m₂ q=0 →
frozenPair n (fun i α j β => D*elasticityTensor L M i α j β) p q=0) : L=0 ∧ M=0 := by
have hmoment : (normalMoment n:ℂ)≠0 := Complex.ofReal_ne_zero.mpr (normalMoment_pos n).ne'
have hM : M=0 := by
have hh := h (leading l₁ m₁ ![0,1,0]) (leading l₂ m₂ ![0,1,0])
(leading_normal l₁ m₁ hp₁ _) (leading_normal l₂ m₂ hp₂ _)
have he := frozenPair_constant n (fun i α j β => D*elasticityTensor L M i α j β)
(leading l₁ m₁ ![0,1,0]) (leading l₂ m₂ ![0,1,0]) (D*(2*M)) (fun y => by
change tensorDensity _ (grad _ y) (grad _ y)=_
rw [tensorDensity_factor,transverse_density])
rw [he] at hh
exact (mul_eq_zero.mp ((mul_eq_zero.mp ((mul_eq_zero.mp hh).resolve_left hmoment)).resolve_left hD)).resolve_left
(by norm_num)
refine ⟨?_,hM⟩
have hh := h (leading l₁ m₁ ![1,0,0]) (leading l₂ m₂ ![1,0,0])
(leading_normal l₁ m₁ hp₁ _) (leading_normal l₂ m₂ hp₂ _)
have he := frozenPair_constant n (fun i α j β => D*elasticityTensor L M i α j β)
(leading l₁ m₁ ![1,0,0]) (leading l₂ m₂ ![1,0,0])
(D*(L*(Complex.I*(2*m₁/(l₁+3*m₁)))*star (Complex.I*(2*m₂/(l₂+3*m₂))))) (fun y => by
change tensorDensity _ (grad _ y) (grad _ y)=_
rw [hM,tensorDensity_factor,longitudinal_density l₁ m₁ l₂ m₂ hp₁ hp₂])
rw [he] at hh
have ht₁ := longitudinal_trace_ne l₁ m₁ hm₁ hp₁
have ht₂ : star (Complex.I*(2*m₂/(l₂+3*m₂)))≠0 := star_ne_zero.mpr
(longitudinal_trace_ne l₂ m₂ hm₂ hp₂)
exact (mul_eq_zero.mp ((mul_eq_zero.mp ((mul_eq_zero.mp
((mul_eq_zero.mp hh).resolve_left hmoment)).resolve_left hD)).resolve_right ht₂)).resolve_right ht₁
end ElasticityBoundaryPacket
end
end
section
/-! Boundary values of BOTH Lamé parameters from the literal physical DN map
on an arbitrary honest smooth domain. This is not a near-boundary assumption. -/
noncomputable section
open Set
open scoped Topology BigOperators
namespace ElasticityBoundaryPacket
open Elasticity ElasticityBoundaryLayerOperator
variable {Ω : Set X} {x : X}
lemma elasticityTensor_sub (l₁ m₁ l₂ m₂ : ℂ) (i α j β : I) :
elasticityTensor l₁ m₁ i α j β-elasticityTensor l₂ m₂ i α j β=
elasticityTensor (l₁-l₂) (m₁-m₂) i α j β := by
unfold elasticityTensor
ring
lemma admissible_frozen_ne {l m : X → ℝ} (ha : Admissible Ω l m) (hx : x∈closure Ω) :
(m x:ℂ)≠0 ∧ (l x:ℂ)+3*(m x:ℂ)≠0 := by
obtain ⟨hm,he⟩ := ha.2.2 x hx
constructor
· exact Complex.ofReal_ne_zero.mpr hm.ne'
· have hp : 0<l x+3*m x := by linarith
exact_mod_cast hp.ne'
lemma Setup.boundary_values (s : Setup Ω x) {l₁ m₁ l₂ m₂ : X → ℝ}
(hl₁ : ContDiff ℝ (⊤ : ℕ∞) l₁) (hm₁ : ContDiff ℝ (⊤ : ℕ∞) m₁)
(hl₂ : ContDiff ℝ (⊤ : ℕ∞) l₂) (hm₂ : ContDiff ℝ (⊤ : ℕ∞) m₂)
(ha₁ : Admissible Ω l₁ m₁) (ha₂ : Admissible Ω l₂ m₂)
(hO : IsOpen Ω) (hB : Bornology.IsBounded Ω) (hx : x∈closure Ω)
(hDN : DN Ω l₁ m₁=DN Ω l₂ m₂) : l₁ x=l₂ x ∧ m₁ x=m₂ x := by
obtain ⟨H₁,hH₁c,hH₁s,hH₁⟩ := s.compact_energy_coefficients
(Complex.ofRealCLM.contDiff.comp hl₁) (Complex.ofRealCLM.contDiff.comp hm₁)
obtain ⟨H₂,hH₂c,hH₂s,hH₂⟩ := s.compact_energy_coefficients
(Complex.ofRealCLM.contDiff.comp hl₂) (Complex.ofRealCLM.contDiff.comp hm₂)
let H := fun i α j β y => H₁ i α j β y-H₂ i α j β y
have hHc : ∀ i α j β, Continuous (H i α j β) := fun i α j β =>
(hH₁c i α j β).sub (hH₂c i α j β)
have hHs : ∀ i α j β, HasCompactSupport (H i α j β) := fun i α j β =>
(hH₁s i α j β).sub (hH₂s i α j β)
have hH (i α j β : I) (y : Y) (hy : WithLp.toLp 2 y∈s.K) :
s.rawCoeff (fun z => (l₁ z:ℂ)) (fun z => (m₁ z:ℂ)) i α j β y-
s.rawCoeff (fun z => (l₂ z:ℂ)) (fun z => (m₂ z:ℂ)) i α j β y=(y 2:ℂ)^0*H i α j β y := by
simp only [pow_zero,one_mul,H,hH₁ i α j β y hy,hH₂ i α j β y hy]
rfl
have hH0 : (fun i α j β => H i α j β 0)=
(fun i α j β => (s.jacobian 0:ℂ)*elasticityTensor
((l₁ x:ℂ)-(l₂ x:ℂ)) ((m₁ x:ℂ)-(m₂ x:ℂ)) i α j β) := by
funext i α j β
have h0 := hH i α j β 0 (by simpa using s.zero_mem)
simp only [pow_zero,one_mul] at h0
rw [← h0]
rw [s.rawCoeff_zero,s.rawCoeff_zero,← mul_sub,elasticityTensor_sub]
have hpair := pair_separates 0 (l₁ x) (m₁ x) (l₂ x) (m₂ x) (s.jacobian 0)
((l₁ x:ℂ)-(l₂ x:ℂ)) ((m₁ x:ℂ)-(m₂ x:ℂ))
(admissible_frozen_ne ha₁ hx).1 (admissible_frozen_ne ha₂ hx).1
(admissible_frozen_ne ha₁ hx).2 (admissible_frozen_ne ha₂ hx).2
(Complex.ofReal_ne_zero.mpr s.jacobian_pos.ne') (by
intro p q hp hq
rw [← hH0]
exact s.extract_normal hl₁ hm₁ hl₂ hm₂ ha₁ ha₂ hO hB hx hDN 0 H hHc hHs hH p q hp hq)
exact ⟨Complex.ofReal_injective (sub_eq_zero.mp hpair.1),
Complex.ofReal_injective (sub_eq_zero.mp hpair.2)⟩
lemma boundary_values_global {l₁ m₁ l₂ m₂ : X → ℝ}
(hS : SourceSmoothBoundary Ω) (hO : IsOpen Ω) (hB : Bornology.IsBounded Ω)
(hl₁ : ContDiff ℝ (⊤ : ℕ∞) l₁) (hm₁ : ContDiff ℝ (⊤ : ℕ∞) m₁)
(hl₂ : ContDiff ℝ (⊤ : ℕ∞) l₂) (hm₂ : ContDiff ℝ (⊤ : ℕ∞) m₂)
(ha₁ : Admissible Ω l₁ m₁) (ha₂ : Admissible Ω l₂ m₂)
(hDN : DN Ω l₁ m₁=DN Ω l₂ m₂) (hx : x∈frontier Ω) : l₁ x=l₂ x ∧ m₁ x=m₂ x := by
obtain ⟨s⟩ := setup_exists hS hx
exact s.boundary_values hl₁ hm₁ hl₂ hm₂ ha₁ ha₂ hO hB (frontier_subset_closure hx) hDN
end ElasticityBoundaryPacket
end
end
section
/-! Honest continuous normal Taylor quotients, obtained from the integral
remainder. These are actual functions of the coefficients, not assumed jets. -/
noncomputable section
open Set MeasureTheory
open scoped Topology BigOperators
namespace ElasticityBoundaryNormalTaylor
abbrev Y := Fin 3 → ℝ
def en : Y := Pi.single 2 1
def projection (y : Y) : Y := y-(y 2) • en
def travel (y : Y) (t : ℝ) : Y := projection y+t • ((y 2) • en)
@[simp] lemma en_apply_two : en 2=1 := by simp [en]
@[simp] lemma projection_two (y : Y) : projection y 2=0 := by simp [projection]
@[simp] lemma projection_zero : projection 0=0 := by simp [projection]
@[simp] lemma travel_zero (t : ℝ) : travel 0 t=0 := by simp [travel]
@[simp] lemma travel_one (y : Y) : travel y 1=y := by simp [travel,projection]
variable {F : Type*} [NormedAddCommGroup F] [NormedSpace ℝ F] [CompleteSpace F]
def normalJet (n : ℕ) (f : Y → F) (y : Y) : F :=
iteratedFDeriv ℝ n f y (fun _ => en)
def quotient (n : ℕ) (f : Y → F) (y : Y) : F :=
(n.factorial:ℝ)⁻¹ • ∫ t in (0:ℝ)..1, (1-t)^n • normalJet (n+1) f (travel y t)
omit [CompleteSpace F] in
lemma normalJet_continuous {f : Y → F} (hf : ContDiff ℝ (⊤ : ℕ∞) f) (n : ℕ) :
Continuous (normalJet n f) :=
(ContinuousMultilinearMap.apply ℝ (fun _ : Fin n => Y) F (fun _ => en)).continuous.comp
(hf.continuous_iteratedFDeriv (by exact_mod_cast le_top))
lemma travel_continuous : Continuous (fun z : Y × ℝ => travel z.1 z.2) := by
unfold travel projection
fun_prop
omit [CompleteSpace F] in
lemma quotient_continuous {f : Y → F} (hf : ContDiff ℝ (⊤ : ℕ∞) f) (n : ℕ) :
Continuous (quotient n f) := by
have hc : Continuous (Function.uncurry (fun y (t:ℝ) => (1-t)^n • normalJet (n+1) f (travel y t))) :=
((continuous_const.sub continuous_snd).pow n).smul
((normalJet_continuous hf (n+1)).comp travel_continuous)
have h := continuous_parametric_integral_of_continuous (μ := volume) hc (isCompact_Icc (a := (0:ℝ)) (b := 1))
have he (y : Y) : (∫ t in (0:ℝ)..1, (1-t)^n • normalJet (n+1) f (travel y t))=
∫ t in Icc (0:ℝ) 1, (1-t)^n • normalJet (n+1) f (travel y t) := by
rw [intervalIntegral.integral_of_le (by norm_num),integral_Icc_eq_integral_Ioc]
change Continuous (fun y : Y => (n.factorial:ℝ)⁻¹ • ∫ t in (0:ℝ)..1, (1-t)^n • normalJet (n+1) f (travel y t))
simp_rw [he]
exact (continuous_const : Continuous (fun _ : Y => (n.factorial:ℝ)⁻¹)).smul h
lemma normal_factor {f : Y → F} (hf : ContDiff ℝ (⊤ : ℕ∞) f) (n : ℕ) (y : Y)
(hz : ∀ k≤n, normalJet k f (projection y)=0) :
f y=(y 2)^(n+1) • quotient n f y := by
have h := map_add_eq_sum_add_integral_iteratedFDeriv
(f := f) (x := projection y) (y := (y 2) • en) (n := n)
(fun _ _ => hf.contDiffAt.of_le (by exact_mod_cast le_top))
have hv (k : ℕ) (z : Y) :
iteratedFDeriv ℝ k f z (fun _ => (y 2) • en)=(y 2)^k • normalJet k f z := by
rw [ContinuousMultilinearMap.map_smul_univ]
simp only [Finset.prod_const,Finset.card_univ,Fintype.card_fin,normalJet]
rw [show projection y+y 2 • en=y by simp [projection]] at h
rw [Finset.sum_eq_zero (fun k hk => by
have hk' : k<n+1 := Finset.mem_range.mp hk
rw [hv,hz k (by omega),smul_zero,smul_zero]),zero_add] at h
simp_rw [hv] at h
rw [show (fun t => (1-t)^n • ((y 2)^(n+1) • normalJet (n+1) f
(projection y+t • (y 2 • en))))=
(fun t => (y 2)^(n+1) • ((1-t)^n • normalJet (n+1) f (travel y t))) from by
funext t; rw [smul_comm]; rfl] at h
rw [intervalIntegral.integral_smul] at h
simpa only [quotient,smul_comm (n.factorial:ℝ)⁻¹] using h
lemma quotient_zero (n : ℕ) (f : Y → F) :
quotient n f 0=((n+1).factorial:ℝ)⁻¹ • normalJet (n+1) f 0 := by
simp only [quotient,travel_zero]
rw [intervalIntegral.integral_smul_const]
have hi : (∫ t in (0:ℝ)..1, (1-t)^n)=(n+1:ℝ)⁻¹ := by
rw [intervalIntegral.integral_comp_sub_left (fun t : ℝ => t^n) 1]
simp [integral_pow]
rw [hi,smul_smul]
congr 1
simp only [Nat.factorial_succ,Nat.cast_mul,Nat.cast_add,Nat.cast_one,mul_inv_rev]
end ElasticityBoundaryNormalTaylor
end
end
end OAI