import OAI.MathematicalPhysics.NavierStokes.ForcedComputation.Scalar.PlaneCylinderCalculus namespace OAI /-! Spatial derivatives on a closed time slab agree with ordinary derivatives of each full-space slice, including at time zero. -/ noncomputable section namespace ForcedComputation.VelocityDetector open Set open scoped ContDiff variable {E F : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [NormedAddCommGroup F] [NormedSpace ℝ F] theorem cylinder_spatial_fderiv_eq {T : ℝ} {U : ℝ × E → F} (hU : ContDiffOn ℝ ∞ U (Icc 0 T ×ˢ univ)) {t : ℝ} (ht : t ∈ Icc 0 T) (x : E) : fderiv ℝ (fun z => U (t, z)) x = (fderivWithin ℝ U (Icc 0 T ×ˢ univ) (t, x)).comp (ContinuousLinearMap.inr ℝ ℝ E) := by have hd := (hU.differentiableOn (by simp) (t, x) ⟨ht, mem_univ x⟩).hasFDerivWithinAt have hi := (hasFDerivAt_const (𝕜 := ℝ) t x).prodMk (hasFDerivAt_id (𝕜 := ℝ) x) have hc := hd.comp_hasFDerivAt x hi (Filter.Eventually.of_forall (fun z => ⟨ht, mem_univ z⟩)) convert hc.fderiv using 1 · rfl · ext z rfl theorem cylinder_spatial_fderiv_smooth {T : ℝ} (hT : 0 < T) {U : ℝ × E → F} (hU : ContDiffOn ℝ ∞ U (Icc 0 T ×ˢ univ)) : ContDiffOn ℝ ∞ (fun y : ℝ × E => fderiv ℝ (fun z => U (y.1, z)) y.2) (Icc 0 T ×ˢ univ) := by have hS : UniqueDiffOn ℝ (Icc 0 T ×ˢ (univ : Set E)) := (uniqueDiffOn_Icc hT).prod uniqueDiffOn_univ have hf : ContDiffOn ℝ ∞ (fderivWithin ℝ U (Icc 0 T ×ˢ univ)) (Icc 0 T ×ˢ univ) := hU.fderivWithin hS (by simp) have hh := hf.clm_comp (contDiffOn_const (c := ContinuousLinearMap.inr ℝ ℝ E)) apply hh.congr rintro ⟨t, x⟩ hx exact cylinder_spatial_fderiv_eq hU hx.1 x theorem cylinder_second_spatial_fderiv_smooth {T : ℝ} (hT : 0 < T) {U : ℝ × E → F} (hU : ContDiffOn ℝ ∞ U (Icc 0 T ×ˢ univ)) : ContDiffOn ℝ ∞ (fun y : ℝ × E => fderiv ℝ (fderiv ℝ (fun z => U (y.1, z))) y.2) (Icc 0 T ×ˢ univ) := cylinder_spatial_fderiv_smooth hT (cylinder_spatial_fderiv_smooth hT hU) end ForcedComputation.VelocityDetector end end OAI