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LeanPool.NavierStokesAndEuler.Euler.CorrectionBudgetRestriction

Genuine coefficient and metric budgets persist under restriction to a partial time interval.

Actual correction coefficient data restricted along continuous time maps.

def EulerCorrectionOperators.CoefficientPath.comp (period : ) [Fact (0 < period)] {q : } {T : Type u_1} {U : Type u_2} [TopologicalSpace T] [TopologicalSpace U] (A : CoefficientPath period q T) (f : C(U, T)) :
CoefficientPath period q U

Restrict the actual spatial coefficient and its jet along a continuous parameter map.

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    noncomputable def EulerCorrectionOperators.CorrectionData.comp (period : ) [Fact (0 < period)] {q : } {T : Type u_1} {U : Type u_2} [TopologicalSpace T] [TopologicalSpace U] (D : CorrectionData period q T) (f : C(U, T)) :
    CorrectionData period q U

    Restrict every actual coefficient, background field, and residual along the same time map.

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      theorem EulerCorrectionOperators.CorrectionData.comp_source (period : ) [Fact (0 < period)] {q : } {T : Type u_1} {U : Type u_2} [TopologicalSpace T] [TopologicalSpace U] (D : CorrectionData period q T) (f : C(U, T)) (hq : 6 q) (t : U) (u : (EulerCylinderSobolevSpace.SobolevSpace period (q + 1))) :
      (coefficients period (comp period D f) hq).apply t u = (coefficients period D hq).apply (f t) u

      The restricted correction source is the original actual source at the restricted time.

      theorem EulerCorrectionOperators.CorrectionData.comp_quadraticDuhamel (period : ) [Fact (0 < period)] {q : } (hq : 6 q) (ν : ) ( : 0 < ν) {T S : } (hT : 0 T) (hTS : T S) (D : CorrectionData period q (Set.Icc 0 S)) (u₀ : (EulerCylinderSobolevSpace.SobolevSpace period (q + 1))) (u : C((Set.Icc 0 T), (EulerCylinderSobolevSpace.SobolevSpace period (q + 1)))) (t : (Set.Icc 0 T)) :
      EulerQuadraticSource.quadraticDuhamel period ν hT (coefficients period (comp period D (EulerQuadraticSource.timeInclusion hTS)) hq) u₀ u t = EulerQuadraticSource.quadraticDuhamel period ν hT hTS (coefficients period D hq) u₀ u t

      Restricting the concrete data gives precisely the same nonlinear mild equation on a shorter interval.

      Clamped restriction agrees with the original continuous path at every time in the shorter interval.

      Restriction of a genuine time derivative gives the same genuine derivative in the shorter interval.

      Every concrete spatial budget restricts with exactly the same numerical constants.

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        The actual inverse metric and its genuine derivative restrict with unchanged numerical budgets.

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