The potential and slow curl of the actual transverse solution, with their genuine time derivatives.
Cache the standard NormedAddCommGroup (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
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Cache the standard NormedSpace ℝ (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
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Cache the standard NormedAddCommGroup PotentialField instance to shorten typeclass
synthesis.
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Cache the standard NormedSpace ℝ PotentialField instance to shorten typeclass synthesis.
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Cache the standard NormedAddCommGroup C(Icc (0 : ℝ) D.T,PotentialField) instance to
shorten typeclass synthesis.
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Cache the standard NormedSpace ℝ C(Icc (0 : ℝ) D.T,PotentialField) instance to shorten
typeclass synthesis.
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Potential coefficient path: an abbreviation for potentialCoefficient D.normal D.normalLower D.normalLower_pos D.normal_lower.
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Cache the standard NormedAddCommGroup (LiftL2 P) instance to shorten typeclass synthesis.
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Cache the standard NormedSpace ℝ (LiftL2 P) instance to shorten typeclass synthesis.
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Cache the standard NormedAddCommGroup (Supported P Space D.support D.support_measurable)
instance to shorten typeclass synthesis.
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Cache the standard NormedSpace ℝ (Supported P Space D.support D.support_measurable)
instance to shorten typeclass synthesis.
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Cache the standard NormedAddCommGroup C(Icc (0 : ℝ) D.T,LiftL2 P) instance to shorten
typeclass synthesis.
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Cache the standard NormedSpace ℝ C(Icc (0 : ℝ) D.T,LiftL2 P) instance to shorten typeclass
synthesis.
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Full velocity path: an abbreviation for includePath P D.support D.support_measurable (G.velocityPath I).
Equations
- G.fullVelocityPath I = (EulerLpCylinderPaths.includePath P D.support ⋯) (G.velocityPath I)
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Full derivative path: an abbreviation for includePath P D.support D.support_measurable (G.derivativePath I).
Equations
- G.fullDerivativePath I = (EulerLpCylinderPaths.includePath P D.support ⋯) (G.derivativePath I)
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Potential path, given by EulerCylinderPotential.potentialPath P D.potentialCoefficientPath (G.fullVelocityPath I).
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Potential time path, constructed using EulerCylinderPotential.potentialDerivative.
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Corrector path, given by EulerCylinderSlowCurl.path P D.FInv.field (G.potentialPath I).
Equations
- G.correctorPath I = EulerCylinderSlowCurl.path P D.FInv.field (G.potentialPath I)
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Corrector time path, given by EulerCylinderSlowCurl.derivative P D.T D.FInv.field D.inverseDerivative (G.potentialPath I) (G.potentialTimePath I).
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- G.correctorTimePath I = EulerCylinderSlowCurl.derivative P D.T D.FInv.field D.inverseDerivative (G.potentialPath I) (G.potentialTimePath I)
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Corrector, defined pointwise by pointField P (G.correctorPath I) (G.correctorPath_orbit I) (D.clamp z.1) (z.2.1,(z.2.2 : AddCircle P)).
Equations
- G.corrector I z = EulerCylinderSmoothOrbit.pointField P (G.correctorPath I) ⋯ (D.clamp z.1) (z.2.1, ↑z.2.2)
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Corrector derivative, defined pointwise by pointField P (G.correctorTimePath I) (G.correctorTimePath_orbit I) (D.clamp z.1) (z.2.1,(z.2.2 : AddCircle P)).
Equations
- G.correctorDerivative I z = EulerCylinderSmoothOrbit.pointField P (G.correctorTimePath I) ⋯ (D.clamp z.1) (z.2.1, ↑z.2.2)
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This potential is exactly the manuscript's normalized angular integral of −m×A/|m|².
The stored corrector is the literal slow curl with the actual inverse deformation.