Source budgets and the actual initialized residual construct exact corrected lifted packets at every sufficiently large frequency.
The output fields and all their properties are conclusions of the constructed correction and the verified approximate residual.
- velocity : EulerAllOrderCorrectionData.FieldTower P T
Velocity field of
ExactLiftedPacket, of typeFieldTower P T. - pressure : EulerAllOrderCorrectionData.FieldTower P T
Pressure field of
ExactLiftedPacket, of typeFieldTower P T. - zero_initial_correction (q : ℕ) : (self.velocity.realization q) ⟨0, ⋯⟩ - (A.approximation.realization q) ⟨0, ⋯⟩ = 0
- energy (n : ℕ) (t : ↑(Set.Icc 0 T)) : EulerGevreyMetricEstimate.energyNorm P n ⋯ (B.radius t) ((EulerCorrectionEnergyData.MetricBudget.operatorPath P B.metric) t) ((self.velocity.realization (n + 6 + 1)) t - (A.approximation.realization (n + 6 + 1)) t) ≤ 2 * (B.spatial (n + 6) ⋯).full.residual * Real.exp (3 * B.growthCoefficient * ↑t) ∧ EulerGevreyMetricEstimate.energyNorm P n ⋯ (B.radius t) ((EulerCorrectionEnergyData.MetricBudget.operatorPath P B.metric) t) ((self.velocity.realization (n + 6 + 1)) t - (A.approximation.realization (n + 6 + 1)) t) ≤ B.delta / 2
- equation (q : ℕ) (hq : 6 ≤ q) (t : ℝ) (ht : t ∈ Set.Ioo 0 T) : HasDerivAt (EulerVolterraConvolution.extendPath T ⋯ (self.velocity.realization q)) (-EulerCorrectionResidualCancellation.nonlinearity P (EulerAllOrderCorrectionData.Data.atOrder P A q) hq ⟨t, ⋯⟩ ((self.velocity.realization (q + 1)) ⟨t, ⋯⟩) - (EulerSobolevCoefficientPressure.coefficientSobolevOperator P (A.metric.jet q ⟨t, ⋯⟩)) ((self.pressure.realization q) ⟨t, ⋯⟩)) t
Instances For
Exact packet of residual, bundling velocity, pressure, zero_initial_correction,
divergence and the required compatibility proofs.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Initialized exact packet, given by exactPacketOfResidual period Q (initializedApproximationResidual M D hTime τ hτ hτT B δ hδ ξ hs α Cagree N hN k hk).
Equations
- One or more equations did not get rendered due to their size.
Instances For
No inverse budget, residual equation or pressure is postulated here. The original source data construct the budget and the exact corrected pair for every sufficiently large frequency, with fixed positive radius and cost.