The physical five-row mean update #
The update is the constructed power-moment inverse, transported with the physical length and velocity scales. Each moment carries its own scale.
Angular increment, given by scaleField ell U (FiveRowRank.deltaV lam C a b (normalizeDebt ell U d)).
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Desired axial increment, given by scaleField ell U (FiveRowRank.gamma lam C a b (normalizeDebt ell U d)).
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Background, given by scaleField ell U (FiveRowRank.background lam C).
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- NavierStokes.MeanRankUpdate.background lam C ell U = NavierStokes.MeanRankUpdate.scaleField ell U (NavierStokes.FiveRowRank.background lam C)
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Equation (35) in physical units, with no assumed rank or inverse.
Angular family, given by scaleFamily ell U (fun p => FiveRowRank.deltaV lam (C p.1) a b (normalizeDebt (ell p.1) (U p.1) (d p.1)) p.2).
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Desired axial family, given by scaleFamily ell U (fun p => FiveRowRank.gamma lam (C p.1) a b (normalizeDebt (ell p.1) (U p.1) (d p.1)) p.2).
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A common radial annulus follows from bounds on the physical length.
The slow source is independent of both periodic phase variables.
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- NavierStokes.MeanRankUpdate.slowLift f p = f (p.1, p.2.1)
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With a slow source the transported total is the ordinary radial mass.
There is exactly zero compactification alias for a zero-mass slow source.
The actual stream realizes the desired slow axial field, pointwise, including the axis.
The radial companion is the actual axial derivative of the same stream.
Normalize debt linear map, bundling toFun, map_add, map_smul.
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- NavierStokes.MeanRankUpdate.normalizeDebtLinearMap ell U = { toFun := NavierStokes.MeanRankUpdate.normalizeDebt ell U, map_add' := ⋯, map_smul' := ⋯ }
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Scale field linear map, bundling toFun, map_add, map_smul.
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- NavierStokes.MeanRankUpdate.scaleFieldLinearMap ell U = { toFun := NavierStokes.MeanRankUpdate.scaleField ell U, map_add' := ⋯, map_smul' := ⋯ }
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Angular linear map, given by (scaleFieldLinearMap ell U).comp ((FiveRowRank.deltaVLinearMap lam C a b).comp (normalizeDebtLinearMap ell U)).
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Axial linear map, given by (scaleFieldLinearMap ell U).comp ((FiveRowRank.gammaLinearMap lam C a b).comp (normalizeDebtLinearMap ell U)).
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The update is a fixed finite linear combination of constructed profiles.
Model point: an abbreviation for PhysicalCoordinateBounds.Point.
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The fixed shaped amplitude on the untouched patch.
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- NavierStokes.MeanRankUpdate.shapedAmplitude B η = B / (1 + η ^ 2)
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Model velocity, given by y.1 ^ (-A).
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- NavierStokes.MeanRankUpdate.modelVelocity A y = y.1 ^ (-A)
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Model amplitude, given by shapedAmplitude B (y.2.2 / y.1 ^ PhysicalCoordinateBounds.D coord).
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- NavierStokes.MeanRankUpdate.modelAmplitude coord B y = NavierStokes.MeanRankUpdate.shapedAmplitude B (y.2.2 / y.1 ^ NavierStokes.PhysicalCoordinateBounds.D coord)
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Angular model, given by angularFamily lam a b modelLength (modelVelocity A) (modelAmplitude coord B) (fun _ => d) (y.2.1, y).
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Axial model, given by desiredAxialFamily lam a b modelLength (modelVelocity A) (modelAmplitude coord B) (fun _ => d) (y.2.1, y).
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Model box, given by Icc qlo qhi ×ˢ (Icc rlo rhi ×ˢ Icc (-1 : ℝ) 1).
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Model to inverse, given by (y.1, (y.2.1, y.2.2 * y.1 ^ PhysicalCoordinateBounds.D coord)).
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- NavierStokes.MeanRankUpdate.modelToInverse coord y = (y.1, y.2.1, y.2.2 * y.1 ^ NavierStokes.PhysicalCoordinateBounds.D coord)
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Actual inverse-coordinate jets remain bounded on a normalized closed
q interval, including both limiting values η=±1.
An interior support and genuine finite jet bounds convert! a fixed coefficient to the weighted mean class.
Chart point: an abbreviation for PressureStream.Lift PressureStream.Plane.
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(R,(T,Z),Y) to the actual inverse-coordinate variables (T,R,Z).
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Chart Q, given by PhysicalCoordinateBounds.qCoord coord (chartInput p).
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Chart eta, given by PhysicalCoordinateBounds.etaCoord coord (chartInput p).
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Chart kernel, given by (g ∘ PhysicalCoordinateBounds.inverseCoordinates coord) ∘ chartInput.
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Chart angular, given by angularIncrement lam (shapedAmplitude B (chartEta coord p)) a b (Real.sqrt (chartQ coord p)) (chartQ coord p ^ (-A)) (d p) p.1.
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Chart axial, constructed using desiredAxialIncrement.
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All stripped jets of the actual inverse-coordinate pullback are uniformly bounded, with no band in either the coefficient or the constant.
Support band, given by Prod.fst ⁻¹' Icc (Real.sqrt qlo * a) (Real.sqrt qhi * b).
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The scalar rank coefficients themselves are proved to lie in M₀.
All regularity and all finite jet bounds are derived from the constructed inverse.
Equation (35) maps the slow defect class S_α to M_α in every finite
stripped jet, uniformly over the band index.
Normalized domain, given by {p | chartInput p ∈ PhysicalCoordinateBounds.positiveTime ∧ chartQ coord p ∈ Ioo qlo qhi ∧ p.1 ∈ Ioo rlo rhi}.
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The concrete logarithmic radial weights, restricted to one normalized
physical q/Q strip. The torus variables remain unrestricted.
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No coefficient estimate is an input to this concrete S_α → M_α result.
Normalized physical angular, constructed using angularIncrement.
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Normalized physical axial, constructed using desiredAxialIncrement.
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Uniform class bounds for the physical definition, read in any normalized band; the physical correction itself has no chosen band.
Only the input geometry and defect family occur in this record.
- lam : ℝ
Lam of
SmoothFamily, of typeℝ. - a : ℝ
A of
SmoothFamily, of typeℝ. - b : ℝ
B of
SmoothFamily, of typeℝ. - length : E → ℝ
Length of
SmoothFamily, of typeE → ℝ. - velocity : E → ℝ
Velocity field of
SmoothFamily, of typeE → ℝ. - amplitude : E → ℝ
Amplitude of
SmoothFamily, of typeE → ℝ. - debt : E → Debt
Debt of
SmoothFamily, of typeE → Debt.
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Angular, given by angularFamily F.lam F.a F.b F.length F.velocity F.amplitude F.debt.
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Desired, given by desiredAxialFamily F.lam F.a F.b F.length F.velocity F.amplitude F.debt.
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Potential, given by PressureStream.streamPotential power lo hi M ((0 : E), v) (slowLift F.desired).
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- F.potential power lo hi M v = NavierStokes.PressureStream.streamPotential power lo hi M (0, v) (NavierStokes.MeanRankUpdate.slowLift F.desired)
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Radial, given by PressureStream.streamBeta w (F.potential power lo hi M v).
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- F.radial power lo hi M v w = NavierStokes.PressureStream.streamBeta w (F.potential power lo hi M v)
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Axial, given by PressureStream.streamGamma (PressureStream.physicalSpeed power M) ((0 : E), v) (F.potential power lo hi M v).
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- F.axial power lo hi M v = NavierStokes.PressureStream.streamGamma (NavierStokes.PressureStream.physicalSpeed power M) (0, v) (F.potential power lo hi M v)
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These are the five rows of the actual divergence-free update.
Support set, given by {p | p.1 ∈ Icc (F.length p.2.1 * F.a) (F.length p.2.1 * F.b)}.
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The radial stream correction remains on the same physical mean patch; varying its endpoints introduces no support outside that patch.
Reserved angular base, given by U * HeatedOutgoing.E F XR c ((r / Real.sqrt q) ^ 2 / 2, η).
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Reserved axial base, given by U * HeatedOutgoing.U F XR ((r / Real.sqrt q) ^ 2 / 2, η).
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The five-row repair on the actual untouched heated outgoing mean patch.
Instantiating the actual reserved patch with any smooth physical q>0
and smooth slow defect family supplies all stream input data.
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Primitive model, given by scaledPrimitive (fun r => axialModel coord A B lam a b d (y.1, r, y.2.2)) y.2.1.
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Chart potential, defined pointwise by ∑ i : Fin 3, d p i * chartKernel coord (primitiveModel coord A B lam a b (Pi.single i 1)) p.
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Chart stream radial, given by PressureStream.streamBeta w (chartPotential coord A B lam a b d).
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- NavierStokes.MeanRankUpdate.chartStreamRadial coord A B lam a b w d = NavierStokes.PressureStream.streamBeta w (NavierStokes.MeanRankUpdate.chartPotential coord A B lam a b d)
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The primitive and its actual slow derivative satisfy the same all-jet weighted class. This proves the radial component bound as well.
The stream is the ordinary zero-axis primitive for a slow zero-mass source. Thus neither its cutoff nor its transport parameter changes it.
Only the radial slice is needed for this identity; no extension of the slow data outside its open physical domain is assumed.
Slow chart desired, defined pointwise by chartAxial coord A B lam a b (fun z => d z.2.1) (p.1, p.2, 0).
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Actual chart potential, given by PressureStream.streamPotential power lo hi M ((0 : PressureStream.Plane), v) (slowLift (slowChartDesired coord A B lam a b d)).
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Actual chart radial, given by PressureStream.streamBeta w (actualChartPotential coord A B lam a b power lo hi M v d).
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The full slow stream estimate is for the actual PressureStream
operator. The proof does not extend data outside the positive-time domain.
A local differentiability hypothesis suffices for the true slow axial identity; the source need only be smooth along its radial slice.
Actual chart axial, constructed using PressureStream.streamGamma.
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Exact slow realization and divergence on the actual normalized physical domain, derived from the input defect class rather than assumed regularity.
Arbitrarily large fast parts of the axial graph direction vanish exactly for the slow rank stream. They cannot create a band-dependent loss.