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

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Integrating time-dependent sources in the finite spatial jet Banach space.

  1. theorem OAI.ForcedComputation.BoundedSpatialJets.function_intervalIntegral line 18

    Source documentation

    Time integration commutes with pointwise evaluation of the represented function.

    theorem function_intervalIntegral (k : ℕ) (J : ℝ → Space E F k) (a b : ℝ)
        (hJ : IntervalIntegrable J volume a b) (x : E) :
        function E F k (∫ t in a..b, J t) x =
          ∫ t in a..b, function E F k (J t) x := by
    …

    Mentions: OAI.ForcedComputation.BoundedSpatialJets.Space, OAI.ForcedComputation.BoundedSpatialJets.function

  2. theorem OAI.ForcedComputation.BoundedSpatialJets.jet_intervalIntegral line 27

    Source documentation

    Every recorded spatial jet commutes with time integration.

    theorem jet_intervalIntegral (k : ℕ) (J : ℝ → Space E F k) (a b : ℝ)
        (hJ : IntervalIntegrable J volume a b) (i : Fin (k + 1)) (x : E) :
        (∫ t in a..b, J t).val i x = ∫ t in a..b, (J t).val i x := by
    …

    Mentions: OAI.ForcedComputation.BoundedSpatialJets.Space

  3. theorem OAI.ForcedComputation.BoundedSpatialJets.iteratedFDeriv_intervalIntegral line 35

    Source documentation

    Time integration preserves all spatial derivatives through the selected finite order.

    theorem iteratedFDeriv_intervalIntegral (k : ℕ) (J : ℝ → Space E F k) (a b : ℝ)
        (hJ : IntervalIntegrable J volume a b) (n : ℕ) (hn : n ≤ k) (x : E) :
        iteratedFDeriv ℝ n (function E F k (∫ t in a..b, J t)) x =
          ∫ t in a..b, iteratedFDeriv ℝ n (function E F k (J t)) x := by
    …

    Mentions: OAI.ForcedComputation.BoundedSpatialJets.Space, OAI.ForcedComputation.BoundedSpatialJets.function

  4. theorem OAI.ForcedComputation.BoundedSpatialJets.norm_intervalIntegral_le line 44

    Source documentation

    A uniform source bound gives the exact interval-length bound in the jet norm.

    theorem norm_intervalIntegral_le (k : ℕ) (J : ℝ → Space E F k) (a b C : ℝ)
        (hJ : ∀ t ∈ Set.uIoc a b, ‖J t‖ ≤ C) :
        ‖∫ t in a..b, J t‖ ≤ C * |b - a| :=
    …

    Mentions: OAI.ForcedComputation.BoundedSpatialJets.Space

  5. theorem OAI.ForcedComputation.BoundedSpatialJets.intervalIntegrable_bilinear line 54

    Source documentation

    A time-dependent coefficient and unknown yield an integrable jet-valued source.

    theorem intervalIntegrable_bilinear (k : ℕ) (B : F →L[ℝ] G →L[ℝ] H)
        (J : ℝ → Space E F k) (K : ℝ → Space E G k) (a b : ℝ)
        (hJ : ContinuousOn J (Set.uIcc a b)) (hK : ContinuousOn K (Set.uIcc a b)) :
        IntervalIntegrable (fun t => bilinear E F G H k B (J t) (K t)) volume a b :=
    …

    Mentions: OAI.ForcedComputation.BoundedSpatialJets.Space, OAI.ForcedComputation.BoundedSpatialJets.bilinear

  6. theorem OAI.ForcedComputation.BoundedSpatialJets.norm_intervalIntegral_bilinear_le line 62

    Source documentation

    Explicit finite-time source bound, with the finite-order Leibniz constant.

    theorem norm_intervalIntegral_bilinear_le (k : ℕ) (B : F →L[ℝ] G →L[ℝ] H)
        (J : ℝ → Space E F k) (K : ℝ → Space E G k) (a b A C : ℝ)
        (hC : 0 ≤ C) (hJ : ∀ t ∈ Set.uIoc a b, ‖J t‖ ≤ A)
        (hK : ∀ t ∈ Set.uIoc a b, ‖K t‖ ≤ C) :
        ‖∫ t in a..b, bilinear E F G H k B (J t) (K t)‖ ≤
          (‖B‖ * (2 : ℝ) ^ k * A * C) * |b - a| := by
    …

    Mentions: OAI.ForcedComputation.BoundedSpatialJets.Space, OAI.ForcedComputation.BoundedSpatialJets.bilinear