The exact temporal mean update #
The native-to-absolute inverse identity is derived from the actual covering map, Fourier coefficients, and uniqueness for the zero-mean periodic directional equation. Band factors remain explicit.
Partial Y, given by fderiv ℝ f z (0, 1).
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Time derivative, given by fderiv ℝ f z (vector .temporal).
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Fourier differentiation, including the zero first frequency.
The temporal Fourier symbol is the actual multiplier of the derivative.
Uniqueness for the smooth periodic temporal equation with a prescribed mean. The proof uses actual Fourier differentiation and reconstruction.
The actual integer covering as a continuous linear map.
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Cover map as an element of `ℕ → Plane →L[ℝ] Plane | 0 => ContinuousLinearMap.id ℝ Plane | n
- 1 => coverLinear.comp (coverMap n)`.
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Absolute inverse, given by directionalInverse .temporal (SmoothFourierData.coefficient f).
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The native factor is forced by the covering derivative and zero-mean uniqueness. Both sides are the actual Fourier-defined inverse.
The native chart prefactor, including the physical velocity rescaling.
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The exponential-looking native factors together cost just one power of the slow band scale.
Multiplication by the actual chart prefactor preserves the class
exponent, for bands numbered n+4 where the native-index bounds hold.
Finite initial bands are absorbed into an explicit constant. The native
indices are unchanged; the slow scale may be max 1 (S n).
Remove exactly the auxiliary torus average, retaining every slow parameter.
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- NavierStokes.TemporalMeanUpdate.centered f z = f z - NavierStokes.PressureStream.torusAverage f (z.1, z.2.1)
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Taking a real part commutes with the actual double integral.
The source in joint slow-parameter/torus coordinates, with the real source embedded isometrically in the complex Fourier construction.
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The actual normalized temporal Fourier inverse on a real joint family.
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The real joint inverse solves the genuine Fréchet directional equation.
Fiberwise native-to-absolute covariance for the actual real family inverse.
The desired angular or axial mean increment in its native chart.
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The actual fast-time derivative, including its chart coefficient.
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In particular this gives both the angular r² bar mass and axial r
bar mass without an extra normalization term.
Exact cancellation of the source's zero-bar part.
Pullback cover, given by f (z.1, (z.2.1, coverMap i z.2.2)).
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- NavierStokes.TemporalMeanUpdate.pullbackCover i f z = f (z.1, z.2.1, (NavierStokes.TemporalMeanUpdate.coverMap i) z.2.2)
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Pulling the native update through its actual covering gives the same
absolute temporal inverse. There is exactly one native Tg⁻ⁱ factor.
Axial potential, given by PressureStream.streamPotential d a b M ((0 : S), v) (desiredIncrement h n f).
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- NavierStokes.TemporalMeanUpdate.axialPotential d a b M v h n f = NavierStokes.PressureStream.streamPotential d a b M (0, v) (NavierStokes.TemporalMeanUpdate.desiredIncrement h n f)
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Axial update, given by PressureStream.streamGamma (PressureStream.physicalSpeed d M) ((0 : S), v) (axialPotential d a b M v h n f).
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Radial update, given by PressureStream.streamBeta w (axialPotential d a b M v h n f).
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- NavierStokes.TemporalMeanUpdate.radialUpdate d a b M v w h n f = NavierStokes.PressureStream.streamBeta w (NavierStokes.TemporalMeanUpdate.axialPotential d a b M v h n f)
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The retained compactification alias, with its physical 1/r factor.
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No compactification error is removed from the reconstructed axial field.
Fast time cancels the axial zero-bar source, retaining exactly the fast-time derivative of the compactification alias.
The actual two-component fast-time update and incompressible stream, with the exact axial alias in the resulting residual.
A fixed smooth radial multiplier preserves the actual all-jet class. The constant is obtained from the derivative product rule on the compact annulus.
Division by the positive radius preserves the class for supported fields. A globally smooth positive regularization proves all derivative bounds.
The actual stream potential preserves the original exponential weight and its exponent, uniformly for all bandwise transport coefficients.
A fixed full axial direction may include every slow variable. Its actual derivative of the stream has the same class exponent.
Alias factor, given by RadialPullback.radialJacobian d (RadialPullback.positiveRadius (a / 4) r) / RadialPullback.positiveRadius (a / 4) r.
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The physical divided alias is exactly a fixed radial multiplier times the normalized transport alias pulled through the power chart.
A uniform full-jet estimate for the actual physical alias follows from the corresponding normalized alias estimate. The transfer constant is fixed before the source, transport coefficient, and transport direction are given.
The complete desired temporal update preserves the original exponent in every band, including the initial bands. No inverse estimate is assumed.
The actual chart axial direction carries ε; its radial stream
component therefore gains one full mean-class exponent.
The actual physical divided alias is uniformly superflat for the manuscript's radial frequencies and any jointly smooth zero-bar source family.
Superflatness of the exact alias in the constructed temporal axial update.
The actual fast-time residual alias is superflat in every full joint jet.
The physical alias has support in one fixed compact subannulus, uniformly in the source, band, and direction.
A fixed interior support converts uniform band bounds into the full weighted class by an actual positive minimum of the exponential weight.
The actual divided compactification alias lies in the same weighted class; its fixed interior support supplies the full edge weight.
The reconstructed axial field, including its exact nonzero alias, has the original mean-class exponent.