Three exact terminal compensation moments #
Three constructed, separated additive bumps in a positive interval repair the pressure, energy, and angular moments. Factoring out the positive shaped-wait amplitude leaves one fixed quadratic map, so its smooth inverse and estimates are uniform in the transverse parameter.
Correction, given by ∑ j, c j * bump P j x.
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- NavierStokes.TerminalCompensation.correction P c x = ∑ j : Fin 3, c j * NavierStokes.TerminalCompensation.bump P j x
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Square moment, given by ∫ x, x ^ s * (bump P j x) ^ 2.
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- NavierStokes.TerminalCompensation.squareMoment P s j = ∫ (x : ℝ), x ^ s * NavierStokes.TerminalCompensation.bump P j x ^ 2
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Slope, given by -1 / 2 - lam.
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- NavierStokes.TerminalCompensation.slope lam = -1 / 2 - lam
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The three powers are those of pressure, energy, and angular momentum.
Quadratic continuous linear map, constructed using LinearMap.toContinuousLinearMap.
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A single smooth inverse repairs all three actual moments and has uniform value, derivative, and spatial first-jet bounds. Smallness also preserves positivity.
Composition with the debt gives the true parameter derivative, with no regularity hypothesis on a previously chosen solution branch.
Clean profile, given by a * baseProfile lam (X / R).
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- NavierStokes.TerminalCompensation.cleanProfile lam R a X = a * NavierStokes.TerminalCompensation.baseProfile lam (X / R)
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The normalization constants follow from the actual change of variable X=R*x.
Normalization factors, given by `![(2 * a ^ 2)⁻¹, (2 * R * a ^ 2)⁻¹, (R * Real.sqrt (2 * R)
- a)⁻¹]`.
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Signed debts are negated so that their sum with the patch changes is zero.
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Amplitude debt, given by -(amplitudeFactors a * v).
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The value, normalized radial derivative, and parameter derivative of the actual additive profile perturbation are all small.
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- One or more equations did not get rendered due to their size.
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One debt threshold and one first-jet constant work on the entire compact parameter range. Both are independent of the physical radial scale.
Heat debt as an element of Coeff.
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- One or more equations did not get rendered due to their size.
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The actual heat-tail debts become uniformly O(1/K) in the fixed patch
coordinate when the patch radius is q*K. No debt estimate is assumed.
The actual outgoing heat edit is compensated for every sufficiently large
radius, uniformly on the compact parameter range, with O(1/K) first-jet cost.
All three physical moment changes are genuine integrable functions.
The whole-line definitions equal the usual positive-radius moment integrals.
A reserved patch ending before the heat switch has no overlap with the actual heat perturbation on positive radii.
The constructed physical profile is jointly smooth in the parameter and positive radius, whenever the amplitude and solved coefficients are smooth.