OAI/MathematicalPhysics/NavierStokes/ForcedComputation/Scalar/PlaneScalarMildDerivatives.lean
9 declarations, 0 contain sorry, 0 declared as axioms
Directional derivatives commute with the actual Gaussian Volterra operators.
- def
OAI.ForcedComputation.PlaneScalarMild.directionalPathline 15Source documentation
Differentiate a continuous jet path pointwise.
def directionalPath (k : ℕ) (v : Plane) (T : ℝ) : WeaklySingular.Path (Jet (k+1)) T →L[ℝ] WeaklySingular.Path (Jet k) T := …Mentions: OAI.ForcedComputation.WeaklySingular.Path, OAI.ForcedComputation.PlaneScalarMild.Jet
- theorem
OAI.ForcedComputation.PlaneScalarMild.directionalPath_applyline 22 - theorem
OAI.ForcedComputation.PlaneScalarMild.extendPath_directionalline 26 - theorem
OAI.ForcedComputation.PlaneScalarMild.rawHeatKernel_directionalline 32 - theorem
OAI.ForcedComputation.PlaneScalarMild.gradientKernel_directionalline 43 - theorem
OAI.ForcedComputation.PlaneScalarMild.rawKernels_directionalline 55 - theorem
OAI.ForcedComputation.PlaneScalarMild.rawKernelIntegral_directionalline 63Source documentation
Spatial differentiation passes through the actual singular time integral.
theorem rawKernelIntegral_directional {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν) (k : ℕ) (v : Plane) (u : WeaklySingular.Path (Jet (k+1)) T) (i : Fin 3) (t : Icc (0 : ℝ) T) : BoundedSpatialJets.directionalDerivativeCLM Plane ℝ k v (∫ s in 0..t.val, rawKernels hν (k+1) i (t.val-s) (WeaklySingular.extendPath (Jet (k+1)) hT u s)) = ∫ s in 0..t.val, rawKernels hν k i (t.val-s) (WeaklySingular.extendPath (Jet k) hT (directionalPath k v T u) s) := by …Mentions: OAI.ForcedComputation.WeaklySingular.Path, OAI.ForcedComputation.PlaneScalarMild.Jet, OAI.ForcedComputation.BoundedSpatialJets.directionalDerivativeCLM, OAI.ForcedComputation.PlaneScalarMild.rawKernels, OAI.ForcedComputation.WeaklySingular.extendPath, OAI.ForcedComputation.PlaneScalarMild.directionalPath
- theorem
OAI.ForcedComputation.PlaneScalarMild.gradient_convolve_C1line 77 - theorem
OAI.ForcedComputation.PlaneScalarMild.gradientKernel_eq_heatDerivativeline 96Source documentation
On finite jets, a Gaussian gradient acting on the input equals heat acting on its derivative.
theorem gradientKernel_eq_heatDerivative {ν : ℝ} (hν : 0 < ν) (k : ℕ) (j : Fin 2) (r : ℝ) (J : Jet (k+1)) : gradientKernel hν k j r (BoundedSpatialJets.truncateCLM Plane ℝ k (k+1) (by omega) J) = rawHeatKernel hν k r (BoundedSpatialJets.directionalDerivativeCLM Plane ℝ k (Pi.single j 1) J) := by …Mentions: OAI.ForcedComputation.PlaneScalarMild.Jet, OAI.ForcedComputation.PlaneScalarMild.gradientKernel, OAI.ForcedComputation.BoundedSpatialJets.truncateCLM, OAI.ForcedComputation.PlaneScalarMild.rawHeatKernel, OAI.ForcedComputation.BoundedSpatialJets.directionalDerivativeCLM