Weighted bounds for the actual leading stress #
The stress consists of the two genuine coefficients in LeadingStress.
Its edge factors are transported through the literal finite modulation and
the five restored profile histories.
Stress, given by (LeadingStress.theta P h p, LeadingStress.axial P h p).
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Stress domain, given by {p | p ∈ D.carrier ∧ 0 < p.1 ∧ P.f p ≠ 0 ∧ NaturalAxisData.L h p.2 ≠ 0}.
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Log point, given by (Real.exp p.2, p.1).
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Log stress, given by stress P h ∘ logPoint.
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Log stress domain, given by logPoint ⁻¹' stressDomain P h.
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Activation profiles, constructed using FromReference.histories.
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Activation stress, constructed using ActivationCone.activatedStress.
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Inner width, given by min W.controls.referenceWidth (Real.log (d.modulation.left / NominalConeAssembly.activeLeft W)).
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Left edge, given by Real.log (NominalConeAssembly.activeLeft W).
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Right edge, given by Real.log (NominalConeAssembly.activeRight W).
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Outer width, given by min 1 (Real.log (NominalConeAssembly.activeRight W / (ModulatedProfileAssembly.repairPatch W).right)).
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The actual two leading stresses vanish on the whole terminal exterior, including the edge. All five histories, not just the velocity, are retained.
The actual full-annulus cone delivered by the finite modulation theorem.
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A full true cone rules out the inactive value kappa = 1. This is
derived for the supplied final witness, without choosing new controls.
Equation (20) for the same final finite-modulation witness. The tensor bounds contain every mixed profile derivative, in both logarithmic and physical radial charts.
Log shear A, given by ActivationContinuation.shearA P (logPoint p).
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Log shear B, given by ActivationContinuation.shearB P (logPoint p).
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Log speed, given by ActivationContinuation.shearSize (logShearA P p) (logShearB P p).
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Log slope, given by logShearB P p / logShearA P p.
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Transfer a genuine smooth directional extension through exact local stress and shear identities. Shrinking keeps all closed collar endpoints.
The actual stress has the inner flat factor and a smooth unit direction with strict margins for the actual modulated shear.
The inverse-cubic terminal factor has a smooth nonzero direction, with strict cone margin through the true terminal edge.
The reference shear remains strictly admissible also at the two closed annulus endpoints; the strict interior is the actual modulation theorem.
Activation speed, constructed using shearSize.
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Activation slope, constructed using shearSlope.
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A single actual inner factor carries both the positive angular orientation and the strict directional certificate.
The actual terminal inverse-cubic factor, with its positive angular orientation and strict directional certificate on the same factor.
Both actual leading stress components are zero on the entire inner physical region, with the axis included by their literal formulas.
The actual product weight, with the two fixed physical attachment points and the same activation time used to construct the profile.
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Distance, given by edgeDistance (leftEdge W) (rightEdge W) (Real.log X).
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A positive multiple of the actual radial product weight is below the norm of the literal two leading stress components.
Every actual mixed physical profile tensor has the same flat product weight, with a finite derivative-dependent inverse-distance loss.
One no-input instance of the complete actual weighted profile and its two oriented strict edge-direction certificates.