OAI/MathematicalPhysics/NavierStokes/ForcedComputation/Scalar/PlaneScalarMildPointwise.lean

GitHub source file

6 declarations, 0 contain sorry, 0 declared as axioms

Scalar interpretation of the effective source and initial value.

  1. def OAI.ForcedComputation.PlaneScalarMild.scalarPathEvaluation line 13
  2. theorem OAI.ForcedComputation.PlaneScalarMild.scalarPathEvaluation_apply line 20
  3. theorem OAI.ForcedComputation.PlaneScalarMild.CompatibleData.solutionJet_function line 26
  4. theorem OAI.ForcedComputation.PlaneScalarMild.CompatibleData.product_directional_function line 33

    Source documentation

    The represented derivative of a coefficient product is the actual spatial derivative.

    private theorem product_directional_function {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν)
        (D : CompatibleData T) (b : Fin 3 → ℝ × Plane → ℝ)
        (hb : ∀ k i t x, BoundedSpatialJets.function Plane ℝ k (D.coefficient k i t) x = b i (t.val,x))
        (k : ℕ) (i : Fin 3) (v : Plane) (t : Icc (0 : ℝ) T) (x : Plane) :
        scalarPathEvaluation k t x (directionalPath k v T
          (productPath (k+1) (D.coefficient (k+1) i) (D.solutionJet hT hν (k+1)))) =
          fderiv ℝ (fun y => b i (t.val,y) * D.solution hT hν t y) x v := by
    …

    Mentions: OAI.ForcedComputation.PlaneScalarMild.CompatibleData, OAI.ForcedComputation.BoundedSpatialJets.function, OAI.ForcedComputation.PlaneScalarMild.scalarPathEvaluation, OAI.ForcedComputation.PlaneScalarMild.directionalPath, OAI.ForcedComputation.PlaneScalarMild.productPath

  5. theorem OAI.ForcedComputation.PlaneScalarMild.CompatibleData.effectiveSource_function line 52

    Source documentation

    The Banach-space effective source has the expected divergence-form scalar value.

    theorem effectiveSource_function {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν)
        (D : CompatibleData T) (h : ℝ × Plane → ℝ) (b : Fin 3 → ℝ × Plane → ℝ)
        (hh : ∀ k t x, BoundedSpatialJets.function Plane ℝ k (D.source k t) x = h (t.val,x))
        (hb : ∀ k i t x, BoundedSpatialJets.function Plane ℝ k (D.coefficient k i t) x = b i (t.val,x))
        (k : ℕ) (t : Icc (0 : ℝ) T) (x : Plane) :
        BoundedSpatialJets.function Plane ℝ k (D.effectiveSource hT hν k t) x =
          h (t.val,x) + b 0 (t.val,x) * D.solution hT hν t x +
            ∑ j : Fin 2, fderiv ℝ (fun y => b j.succ (t.val,y) * D.solution hT hν t y) x
              (Pi.single j 1) := by
    …

    Mentions: OAI.ForcedComputation.PlaneScalarMild.CompatibleData, OAI.ForcedComputation.BoundedSpatialJets.function

  6. theorem OAI.ForcedComputation.PlaneScalarMild.CompatibleData.solution_initial line 73

    Source documentation

    The mild solution takes exactly its prescribed initial value.

    theorem solution_initial {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν)
        (D : CompatibleData T) (x : Plane) :
        D.solution hT hν ⟨0, le_rfl, hT⟩ x = BoundedSpatialJets.function Plane ℝ 0 (D.initial 0) x := by
    …

    Mentions: OAI.ForcedComputation.PlaneScalarMild.CompatibleData, OAI.ForcedComputation.BoundedSpatialJets.function