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import OAI.MathematicalPhysics.NavierStokes.ForcedComputation.Programs.CompactRapidEmbedding
namespace OAI
/-! The similarity has length scale 1/8. Thus viscosity 64ν before the
similarity gives viscosity ν afterwards. All identities are proved directly
from the coordinate derivatives used in the rapid construction. -/
noncomputable section
open Set
open scoped BigOperators
namespace RapidForcing.CompactEmbedding
theorem spatialD_field {u : Field Space} {t : ℝ}
(hu : Differentiable ℝ (u t)) (i : Fin 3) (x : Space) :
spatialD i (field u) t x = (8 * coordinateSign i) •
linear (spatialD i u t (unembed x)) := by
have hd := linear.hasFDerivAt.comp x
((hu (unembed x)).hasFDerivAt.comp x (unembed_hasFDerivAt x))
simp only [Function.comp_def] at hd
change fderiv ℝ (fun y => linear (u t (unembed y))) x (basis i) = _
rw [hd.fderiv]
simp only [ContinuousLinearMap.comp_apply, inverseLinear_basis, map_smul, spatialD]
theorem divergence_field {u : Field Space} {t : ℝ}
(hu : Differentiable ℝ (u t)) (x : Space) :
divergence (field u) t x = divergence u t (unembed x) := by
unfold divergence
apply Finset.sum_congr rfl
intro i _
rw [spatialD_field hu, PiLp.smul_apply, linear_apply]
by_cases hi : i = 0
all_goals simp [coordinateSign, hi]
all_goals ring
theorem advection_field {u : Field Space} {t : ℝ}
(hu : Differentiable ℝ (u t)) (x : Space) :
advection (field u) t x = linear (advection u t (unembed x)) := by
unfold advection
rw [map_sum]
apply Finset.sum_congr rfl
intro i _
rw [spatialD_field hu, field, linear_apply, smul_smul, map_smul]
congr 1
by_cases hi : i = 0 <;> simp [coordinateSign, hi] <;> ring
theorem spatialD_const_smul {u : Field Space} {t : ℝ}
(hu : Differentiable ℝ (u t)) (a : ℝ) (i : Fin 3) (x : Space) :
spatialD i (fun t x => a • u t x) t x = a • spatialD i u t x := by
change fderiv ℝ (a • u t) x (basis i) = _
rw [((hu x).hasFDerivAt.const_smul a).fderiv]
rfl
theorem spatialD_field_differentiable {u : Field Space} {t : ℝ}
(hu : Differentiable ℝ (u t)) : Differentiable ℝ (field u t) :=
linear.differentiable.comp (hu.comp (unembed_contDiff.differentiable (by simp)))
theorem spatialD_twice_field {u : Field Space} {t : ℝ}
(hu : Differentiable ℝ (u t))
(hdu : ∀ i, Differentiable ℝ (spatialD i u t)) (i : Fin 3) (x : Space) :
spatialD i (spatialD i (field u)) t x =
(64 : ℝ) • linear (spatialD i (spatialD i u) t (unembed x)) := by
have he : spatialD i (field u) t =
fun y => (8 * coordinateSign i) • field (spatialD i u) t y := by
funext y
exact spatialD_field hu i y
change fderiv ℝ (spatialD i (field u) t) x (basis i) = _
rw [he]
change spatialD i (fun s y => (8 * coordinateSign i) • field (spatialD i u) s y) t x = _
rw [spatialD_const_smul (spatialD_field_differentiable (hdu i)),
spatialD_field (hdu i), smul_smul]
congr 1
by_cases hi : i = 0 <;> norm_num [coordinateSign, hi]
theorem laplace_field {u : Field Space} {t : ℝ}
(hu : Differentiable ℝ (u t))
(hdu : ∀ i, Differentiable ℝ (spatialD i u t)) (x : Space) :
laplace (field u) t x = (64 : ℝ) • linear (laplace u t (unembed x)) := by
unfold laplace
rw [map_sum, Finset.smul_sum]
exact Finset.sum_congr rfl (fun i _ => spatialD_twice_field hu hdu i x)
theorem timeD_field {u : Field Space} {t : ℝ} (ht : 0 ≤ t) (x : Space)
(hu : DifferentiableWithinAt ℝ (fun s => u s (unembed x)) (Ici 0) t) :
timeD (field u) t x = linear (timeD u t (unembed x)) := by
have hd := linear.hasFDerivAt.comp_hasDerivWithinAt t hu.hasDerivWithinAt
exact hd.derivWithin (uniqueDiffOn_Ici 0 t ht)
theorem residual_field {u : Field Space} {t : ℝ} (ht : 0 ≤ t)
(hu : Differentiable ℝ (u t))
(hdu : ∀ i, Differentiable ℝ (spatialD i u t))
(htime : ∀ x, DifferentiableWithinAt ℝ (fun s => u s x) (Ici 0) t)
(ν : ℝ) (x : Space) :
residual ν (field u) t x = linear (residual (64 * ν) u t (unembed x)) := by
unfold residual
rw [timeD_field ht x (htime _), advection_field hu, laplace_field hu hdu,
map_sub, map_add, map_smul, smul_smul]
congr 1
congr 1
ring
theorem navierStokes_field {u f : Field Space} (ν : ℝ)
(hNS : NavierStokes (64 * ν) f u (fun _ _ => 0))
(hu : ∀ t, 0 ≤ t → Differentiable ℝ (u t))
(hdu : ∀ t, 0 ≤ t → ∀ i, Differentiable ℝ (spatialD i u t))
(htime : ∀ t, 0 ≤ t → ∀ x,
DifferentiableWithinAt ℝ (fun s => u s x) (Ici 0) t) :
NavierStokes ν (field f) (field u) (fun _ _ => 0) := by
refine ⟨?_, ?_, ?_⟩
· intro t ht x
have hres : residual (64 * ν) u t (unembed x) = f t (unembed x) := by
have he := hNS.1 t ht (unembed x)
simp [gradient, spatialD] at he
unfold residual
rw [he]
abel
have he := residual_field ht (hu t ht) (hdu t ht) (htime t ht) ν x
rw [hres] at he
change timeD (field u) t x + advection (field u) t x = _
simp only [gradient, spatialD, fderiv_const_apply, zero_apply,
zero_smul, Finset.sum_const_zero, neg_zero, zero_add]
change timeD (field u) t x + advection (field u) t x =
ν • laplace (field u) t x + linear (f t (unembed x))
unfold residual at he
rw [← he]
abel
· intro t ht x
rw [divergence_field (hu t ht)]
exact hNS.2.1 t ht (unembed x)
· intro x
simp [field, hNS.2.2]
end RapidForcing.CompactEmbedding
end
end OAI