import Mathlib import OAI.Analysis.Conductivity.Sources.LocalPiola import OAI.Analysis.Conductivity.Variational.CompactSymmetricMoments import OAI.Analysis.Conductivity.Flux.CompactFluxDivergence namespace OAI noncomputable section namespace ScalarConductivity open Set MeasureTheory Matrix open scoped Matrix.Norms.Elementwise def symmetricSource (H : Coord3 → Mat3) (u : Coord3 → Fin 2 → ℝ) (j : Fin 2) : Coord3 → ℝ := coordinateDivergence (fun x => (H x*gradientColumns (fderiv ℝ u x)).col j) lemma symmetricFlux_smooth {H : Coord3 → Mat3} {u : Coord3 → Fin 2 → ℝ} (hH : ContDiff ℝ (↑(⊤ : ℕ∞)) H) (hu : ContDiff ℝ (↑(⊤ : ℕ∞)) u) (j : Fin 2) : ContDiff ℝ (↑(⊤ : ℕ∞)) (fun x => (H x*gradientColumns (fderiv ℝ u x)).col j) := by have hm : ContDiff ℝ (↑(⊤ : ℕ∞)) (fun x => H x*gradientColumns (fderiv ℝ u x)) := by rw [contDiff_iff_contDiffAt] intro x exact contDiffAt_matrix_mul hH.contDiffAt (contDiff_gradientColumns u hu).contDiffAt apply contDiff_pi.mpr intro i exact contDiff_pi.mp (contDiff_pi.mp hm i) j lemma symmetricFlux_compact {H : Coord3 → Mat3} (hH : HasCompactSupport H) (u : Coord3 → Fin 2 → ℝ) (j : Fin 2) : HasCompactSupport (fun x => (H x*gradientColumns (fderiv ℝ u x)).col j) := hH.of_isClosed_subset isClosed_closure (tensorColumn_tsupport H _ j) theorem symmetric_cutoff_sources (H : Coord3 → Mat3) (hH : ContDiff ℝ (↑(⊤ : ℕ∞)) H) (hs : HasCompactSupport H) (hsy : ∀ x,(H x).IsSymm) (u : Coord3 → Fin 2 → ℝ) (hu : ContDiff ℝ (↑(⊤ : ℕ∞)) u) : (∀ j,ContDiff ℝ (↑(⊤ : ℕ∞)) (symmetricSource H u j)) ∧ (∀ j,HasCompactSupport (symmetricSource H u j)) ∧ (∀ j (ψ : Coord3 → ℝ),ContDiff ℝ (↑(⊤ : ℕ∞)) ψ → (∫ x,fderiv ℝ ψ x ((H x*gradientColumns (fderiv ℝ u x)).col j))= -(∫ x,ψ x*symmetricSource H u j x)) ∧ (∫ x,symmetricSource H u 0 x)=0 ∧ (∫ x,symmetricSource H u 1 x)=0 ∧ (∫ x,u x 1*symmetricSource H u 0 x-u x 0*symmetricSource H u 1 x)=0 := by have hr (j : Fin 2) : ContDiff ℝ (↑(⊤ : ℕ∞)) (symmetricSource H u j) := coordinateDivergence_smooth (symmetricFlux_smooth hH hu j) have hsr (j : Fin 2) : HasCompactSupport (symmetricSource H u j) := coordinateDivergence_compact (symmetricFlux_compact hs u j) have hw (j : Fin 2) (ψ : Coord3 → ℝ) (hψ : ContDiff ℝ (↑(⊤ : ℕ∞)) ψ) : (∫ x,fderiv ℝ ψ x ((H x*gradientColumns (fderiv ℝ u x)).col j))= -(∫ x,ψ x*symmetricSource H u j x) := coordinateDivergence_weak (symmetricFlux_smooth hH hu j) (symmetricFlux_compact hs u j) ψ hψ exact ⟨hr,hsr,hw,compact_symmetric_source_moments u hu H hsy _ hr hsr hw⟩ end ScalarConductivity end end OAI