Particular-wave data for the actual correction cycle #
The record below names the particular half of the cycle's analytic data. Its producer uses the literal fixed-parameter solve and incoming invariant.
Exact dynamics of the actual particular correction #
The current harmonic residual is solved on the common cover. Geometry and
carrier identities are proved for the actual selected primary labels;
quantitative controls are supplied by ActualParticularStageControls.
Actual harmonic divergence under a change of product association #
The same complex single-mode field is pulled back along the cylinder isometry. Its genuine cylindrical divergence is preserved, including the transported radial and axial directions. No new divergence premise is needed for the associated particular-solver coordinates.
Primary carrier as an element of HarmonicBlock CyclePoint.
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Preserves carriers: an abbreviation for ∀ l, SameCarrier (x.coefficients.blocks l) (primaryCarrier l).
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Reference point as an element of ActualSignedGeometry.Native.
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Data used in actual particular dynamics.
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The copied normal equality is a true germ, including on the closed transverse core boundary. Only slot time and the slow carrier are open.
The actual modal reconstruction is tangent throughout a neighborhood of a closed-cell point. The normal match is a primitive geometric germ; the tangency of both solved components follows from the modal bridges.
Selected directions as an element of LinearWaveBounds.GraphDirections Native.
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Modal strip, constructed using UniformPrimaryWeights.reindexedStrip.
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The literal common-cover inverse solves the current source at every closed transverse cell point. No open-cell or final equation hypothesis is used.
The support information supplied by the actual incoming source and the common-cover cutoff. The last alternative is proved by zero source on the whole native solve path. It contains no differential equation.
Cells of
SupportData, of typePeriodizedWaveBounds.Cells Native Frequency.- cutoff_support (n : ℕ) (k : TorusInverse.Frequency) : Function.support ((data x l j).cutoff n k) ⊆ self.cells.carrier n k
- cover (n : ℕ) (k : TorusInverse.Frequency) (z : (ActualParticularStageControls.Parameter × ℝ) × TorusInverse.Plane) : z ∈ (CorrectionStep.ParticularParameters.nativeStrip ActualParticularStageControls.associatedStrip).domain → z ∈ self.cells.carrier n k → z ∈ ActualParticularStageControls.controlPatch l n k ∨ ((data x l j).cutoff n k =ᶠ[nhds z] fun (x : (ActualParticularStageControls.Parameter × ℝ) × TorusInverse.Plane) => 0) ∨ ((data x l j).amplitude n k =ᶠ[nhds z] fun (x : (ActualParticularStageControls.Parameter × ℝ) × TorusInverse.Plane) => 0) ∧ ((data x l j).pressure n k =ᶠ[nhds z] fun (x : (ActualParticularStageControls.Parameter × ℝ) × TorusInverse.Plane) => 0) ∧ (data x l j).source n =ᶠ[nhds z] fun (x : (ActualParticularStageControls.Parameter × ℝ) × TorusInverse.Plane) => 0
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Actual wave used in actual particular dynamics.
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Actual update used in actual particular dynamics.
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Actual good used in actual particular dynamics.
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Actual gaussian used in actual particular dynamics.
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Support data, bundling cells, cutoff_support, cover.
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- NavierStokes.ActualParticularDynamics.supportData x hs hN l j = { cells := NavierStokes.ActualParticularStageControls.carrierCells l, cutoff_support := ⋯, cover := ⋯ }
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Source classes type used in actual particular dynamics.
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Actual incoming support and source classes imply solenoidality of the finite particular correction.
The actual current residual is cancelled by the finite common-cover solve, with the computed retained and Gaussian terms on the right.
Cycle update, given by StateReindex.block cycleAssoc (actualUpdate x l N).
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The weighted Gaussian error of the actual particular update #
The native estimates are those of the selected actual Volterra solves, already
transferred back to the original label and band in raw_jets. Gaussian decay
is applied at that original band. The square-root moving-edge weight is kept
through the entire estimate, including the uncovered source term.
Native strip, given by CommonCoverClass.sourceStrip (ActualParticularControl.angleStrip slowStrip).
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Band scales, bundling power, epsilon_eq, boundConstant, constant_one_le and the
required compatibility proofs.
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The clock bounds are imposed only on active pairs.
Clock upper, given by `ActualSignedGeometry.powerBound (CoordinateAlgebra.A ActualPrimary.h
- 1 / 2)`.
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Transported length, given by ActualCarrierTransportBase.referenceLength (supportLabel l) / ActualCarrierTransportBase.clock (supportLabel l) n.
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Length lower, given by ActualInitialExcluded.gaussianLengthLower / clockUpper.
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The auxiliary length agrees with the actual transported slot wherever the analytic patch is used. It only totalizes the Gaussian bookkeeping on inactive label-band pairs.
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Theta, given by ((ActualCarrierTransportBase.geometry (supportLabel l) n).coordinates k z.2).2 / transportedLength l n.
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Gaussian rate, given by ActualGaussianCoverage.gaussianRate (ActualPrimary.choice B N0).prepared.M⁻¹ (ActualPrimary.choice B N0).prepared.u / clockUpper.
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Exact envelope and cutoff readouts on the actual analytic patch.
The uncovered source is zero; it is not estimated without its edge weight.
Every power gain for the literal particular Gaussian error, with constants chosen before the original spatial label and band. The hypotheses concern the incoming source and its actual support, never the solved error.
The literal finite harmonic Gaussian block inherits the same weighted all-power estimate. Its finite modal sum changes the constant, not its uniformity in the original spatial label and band.
Parameters: an abbreviation for ActualCycleParameters.fixedParameters B N0.
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Block: an abbreviation for (parameters B N0).particularBlock x.coefficients (ActualPrimary.commonContext B) x.state.
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Gaussian block: an abbreviation for (parameters B N0).particularGaussianBlock x.coefficients (ActualPrimary.commonContext B) x.state.
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Invariant type used in actual particular cycle data.
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The literal particular increment's analytic outputs. No signed-wave estimate is required to prepare its mean and the subsequent signed request.
- amplitude (i : Fin 3) (j : ℤ) : LabelSumBounds.UniformWaveClass ActualInitialization.strip ActualInitialization.envelope (1 / 2 + σ) fun (l : ActualInitialization.Index B N0) (n : ℕ) (z : ActualInitialization.Point) => ((block x l).velocity n i).coeff j z
- pressure (j : ℤ) : LabelSumBounds.UniformWaveClass ActualInitialization.strip ActualInitialization.envelope (1 + σ) fun (l : ActualInitialization.Index B N0) (n : ℕ) (z : ActualInitialization.Point) => ((block x l).pressure n).coeff j z
- coefficients (l : ActualCycleParameters.Index B N0) (n : ℕ) (i : Fin 3) : HarmonicResidual.SmoothCoefficients ActualInitialization.geometry.domain ((block x l).velocity n i)
- pressureCoefficients (l : ActualCycleParameters.Index B N0) (n : ℕ) : HarmonicResidual.SmoothCoefficients ActualInitialization.geometry.domain ((block x l).pressure n)
- gaussianCoefficients (l : ActualCycleParameters.Index B N0) (n : ℕ) (i : Fin 3) : HarmonicResidual.SmoothCoefficients ActualInitialization.geometry.domain ((gaussianBlock x l).velocity n i)
- solenoidal (l : ActualCycleParameters.Index B N0) : HarmonicWaveInteraction.ModeSolenoidal ActualInitialization.strip (CorrectionInitialization.ActualPrimary.commonContext B) (block x l)
- gaussian (β : ℝ) (i : Fin 3) (j : ℤ) : LabelSumBounds.UniformClass ActualInitialization.strip (fun (x : ActualCycleParameters.Index B N0) (x_1 : ℕ) (z : ActualInitialization.Point) => √(ActualInitialization.strip.zeta z)) β fun (l : ActualCycleParameters.Index B N0) (n : ℕ) (z : ActualInitialization.Point) => ((gaussianBlock x l).velocity n i).coeff j z
- pressureField (n : ℕ) : ContDiffOn ℝ (↑⊤) ((parameters B N0).particularPressure x.coefficients (CorrectionInitialization.ActualPrimary.commonContext B) x.state n) (ActualInitialization.geometry.domain ×ˢ Set.univ)
- linear (i : Fin 3) (j : ℤ) : j ≠ 0 → LabelSumBounds.UniformWaveClass ActualInitialization.strip ActualInitialization.envelope (1 + σ - 3 * ChartScales.kappa) fun (l : ActualInitialization.Index B N0) (n : ℕ) (z : ActualInitialization.Point) => ((HarmonicResidual.residualBlock (CorrectionInitialization.ActualPrimary.commonContext B) x.state (x.coefficients.blocks l) (x.coefficients.gaussian l) (x.coefficients.aliasCoefficients l)).velocity n i).coeff j z + ((HarmonicWaveInteraction.linearGoodBlock (CorrectionInitialization.ActualPrimary.commonContext B) (x.coefficients.blocks l) (block x l) (gaussianBlock x l).velocity).velocity n i).coeff j z
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The actual geometric support supplies the remaining first-wave mean inputs; this does not use any signed increment.
Native data used in actual particular cycle data.
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Native mode, constructed using ActualWaveRegularity.modeOscillation.
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Associated domain, given by ActualCarrierTransport.parameterDomain ×ˢ Set.univ.
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Good block, given by ActualParticularStageControls.outputGood (ActualCycleParameters.particularState x) x.coefficients.residualBand (l.2,l.1).
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Pressure is assembled from the same actual modes as velocity.
Every field is derived for the literal particular construction from the incoming analytic invariant and its separately tracked periods.