The true cone after radial modulation #
The error estimates below concern the genuine derivatives of the realized profiles. Their constants are obtained from the constructed periodic primitives on compact sets, independently of the modulation frequency.
Quantitative stock bounds from actual field and history data #
The two stock maps below are the exact integrated lag formulas. Their Lipschitz constants are derived from smoothness and compactness on sets with positive angular field and radius. No stock error estimate is assumed.
The field values followed by the actual five histories and their first parameter derivatives. Pressure includes its prescribed value on the axis.
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Stock map as an element of ℝ × ℝ.
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Stock domain, given by {q | 0 < q.1.1 ∧ NaturalAxisData.L h q.1.2 ≠ 0 ∧ 0 < q.2 0}.
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- NavierStokes.ModulatedStockBounds.stockDomain h = {q : NavierStokes.ModulatedStockBounds.StockArgument | 0 < q.1.1 ∧ NavierStokes.NaturalAxisData.L h q.1.2 ≠ 0 ∧ 0 < q.2 0}
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Uniform Lipschitz continuity in all field/history data on a compact positive-radius set. Only the reference coefficients depend on position.
A small data perturbation automatically retains a positive angular field, and its exact stock error is bounded linearly by the data error.
Coordinatewise bounds on genuine field/history data give the required norm bound; all first history derivatives are actual parameter derivatives.
Uniform quantitative stability of both actual profile stocks, around a fixed smooth positive nominal profile on a compact set.
The actual stock difference is bounded linearly by a common bound for the two field values and the five history values/first parameter derivatives.
A first parameter-jet bound on an actual history difference supplies exactly the value/derivative estimates used by the stock adapter.
Actual field and five-row history estimates of order 1/n imply an
eventual uniform 1/n estimate for both actual lag stocks. The integer
threshold and the stock constant are conclusions.
The actual angular shear of an angular profile E.
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The signed axial shear, in the C = -b convention of TrueConeLoop.
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Compactness bounds a continuous periodic family at all real phases.
The slow radial derivative of a periodic primitive, with the phase held fixed.
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Differentiation in the slow radius preserves phase periodicity.
Angular error factor, given by -2 * z.1.1 * slowRadial r.angularPrimitive z.
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A smooth error factor at inverse frequency zero.
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Exact factorization of both errors in genuine realized shears.
The axial error factor is continuous even at inverse frequency zero.
Both actual shears differ from their prescribed loop values by C/n.
No derivative estimate for the modulated profiles is assumed.
Cone coordinates, given by (z.1.1 + z.1.2 * (z.2.2 / z.2.1), z.1.2 - z.1.1 * (z.2.2 / z.2.1), z.2.1 * (1 + (z.2.2 / z.2.1) ^ 2)).
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Stock shear cone, given by {z | TrueConeLoop.InTrueCone z.1.1 z.1.2 z.2.1 z.2.2}.
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- NavierStokes.ModulatedCone.stockShearCone = {z : NavierStokes.ModulatedCone.StockShearDatum | NavierStokes.TrueConeLoop.InTrueCone z.1.1 z.1.2 z.2.1 z.2.2}
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Openness is inherited from the already verified exact root cone.
A compact periodic loop has a single tolerance in the original four coordinates, including stock errors and both shear errors.
The tolerance is available for the actual loop selected from nominal relaxed-cone data, without a true-cone assumption on those nominal shears.
Interface for combining the derived shear bound with derived stock
estimates. The actual history construction supplies hstock below.
A small edit in field value and first radial derivatives produces a small edit in both genuine shear quotients.
Equality on an open collar includes equality of the actual shears.
The genuine derivative with the parameter held fixed.
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Compact smooth positive nominal fields have a uniform C¹-to-shear
estimate. The positive denominator after the edit is a conclusion.
The primitive construction preserves a single open collar for the values and the genuine radial shears, at every frequency.
Local agreement along the radial variable suffices for exact shear agreement.
The same four-coordinate tolerance applies to an ordinary compact nominal true-cone patch (the constant periodic-loop case).
Composition interface for the actual following repair. The modulation
region uses its derived shear estimate, while a nominal true-cone patch uses
the derived C¹ perturbation estimate. Later the actual history and moment
construction supplies the stock/edit bounds and the local equality premise.
History index as an element of HistoryRow → Fin 5 | .mass => 0 | .angular => 1 | .transport => 2 | .energy => 3 | .pressure => 4.
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- NavierStokes.ModulatedCone.Localized.historyIndex NavierStokes.StressActivation.HistoryRow.mass = 0
- NavierStokes.ModulatedCone.Localized.historyIndex NavierStokes.StressActivation.HistoryRow.angular = 1
- NavierStokes.ModulatedCone.Localized.historyIndex NavierStokes.StressActivation.HistoryRow.transport = 2
- NavierStokes.ModulatedCone.Localized.historyIndex NavierStokes.StressActivation.HistoryRow.energy = 3
- NavierStokes.ModulatedCone.Localized.historyIndex NavierStokes.StressActivation.HistoryRow.pressure = 4
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Localization preserves the uniform field-value estimate, including at all points outside the modulation window.
Each actual localized profile history has the constructed integral difference; the pressure constant is retained exactly.
Actual localized history values and their first parameter derivatives
have one frequency-independent C/n bound.
The actual stocks of the localized modulation have a uniform C/n
bound, derived from its actual axis-integrated histories.
The endpoint collars make the localized functions locally equal to the raw modulated functions even at both endpoints of the closed window.
The actual localized physical fields agree locally with the raw realized fields, including at the boundary collars.
Both shears of the actual localized physical profiles equal the already estimated realized shears, including at the boundary collars.
A finite integer frequency puts the actual localized profiles, with their actual axis-integrated stresses, in the true cone throughout the closed modulation window. All error bounds are derived in this theorem.
The localized Profiles family used by the cone theorems is actually
constructed from the modulation and one common axis-pressure function.
The actual physical correction, retaining the existing axis pressure.
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Rows eta, given by ![parameterPartial P.M p, parameterPartial P.I p, parameterPartial P.J p, parameterPartial P.S p, parameterPartial P.pressure p].
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Vector bounds for the five actual history jets imply each actual history/parameter-derivative bound needed by the stock estimate.
The actual correction leaves the physical fields and both radial shears unchanged outside the open repair patch.
On a patch where the base profile is nominal, the actual physical repair has exactly its prescribed additive value and derivative errors.
The actual moment edit supplies a uniform first-radial-derivative bound from its coefficient jet bound. No shear estimate is a premise.
A later repair preserves the already realized shears on the entire closed modulation window, including both endpoint collars.
The actual repaired profile data satisfy a uniform estimate before, inside, and after the repair. The two contributions are the modulation error and the coefficient size of this same physical repair.
Uniform stock estimates for a family of actual repaired profiles, using only the proved coefficient size of the moment solver.
Both portions of the actual repaired construction lie in the true cone for one finite frequency threshold. The coefficient input is the quantitative output of the actual moment solver.
The actual nonlinear five-row solve and the actual modulation allow one finite integer frequency with the true cone throughout the loop and following nominal patch. All five histories are restored exactly after the repair, and every radial germ outside its support is unchanged.