The full fully-switched terminal cone #
The release estimate is uniform on the whole remaining logarithmic interval. The closed profile band is treated with the actual smooth heat extension, not with a compact subset of a physical chart. The compensation witness is arbitrary throughout.
The clock at which the heat switch is complete.
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Normalization, given by TerminalPressure.releasedNormalization F.data (OutgoingDilation.switchRadius F XR).
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Shift, given by Real.log (OutgoingDilation.switchRadius F XR) - 1 / 5.
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- NavierStokes.TerminalCone.shift F XR = Real.log (NavierStokes.OutgoingDilation.switchRadius F XR) - 1 / 5
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Profile point, given by (eta, edgeDistance F y).
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The release time and release amplitude depend on the core schedule before the terminal exponent is chosen.
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Release amplitude, given by OutgoingSchedule.radialAmplitude c.P c.dropLength c.lam (releaseTime c) / 2.
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Release budget, given by 16 * annulusRatio * (annulusRatio - 1) * releaseAmplitude c.
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The order is explicit: these bounds use only the already fixed core
schedule, then constrain h; the entrance radius is chosen afterwards.
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Uniform small-argument heat slope, including zero diffusion #
Heat slope, given by -z * deriv (HeatProfileExtension.extension (1 + d.h)) z / HeatProfileExtension.extension (1 + d.h) z.
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- NavierStokes.TerminalCone.heatSlope d z = -z * deriv (NavierStokes.HeatProfileExtension.extension (1 + d.h)) z / NavierStokes.HeatProfileExtension.extension (1 + d.h) z
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Physical-section identities and extension to the closed band #
Profile mass as an element of ℝ.
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- One or more equations did not get rendered due to their size.
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Uniform cone margin through the actual terminal edge #
A numerical direction margin on the entire remaining interval, including both closed parameter endpoints and the stress-free terminal edge.
The root-form true cone for the actual heat/taper backward stress, with
P-a=Tθ/F and J=Tz/F, on the full switched interval.
The identical compensated outgoing field and the ordered radius choice #
Chosen only after the core schedule and h. This bound contains no
compensation coefficient or data-dependent edge-collar width.
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The actual compensated velocity uses precisely the terminal field whose true cone was proved above. The existing witness, its coefficients, and the base outgoing profile are retained.