Actual angular history through the release and terminal tail #
The corrected angular field has the exact initial moment required by the release controller. Matching derivatives and initial values identifies its actual integral with each constructed lag solution. The terminal identity then gives the vanishing renormalized angular moment.
Corrected weight, given by Real.exp (3 * y / 2) * correctedAngular d c (y, eta).
Equations
- NavierStokes.ReleaseMoments.correctedWeight d c eta y = Real.exp (3 * y / 2) * NavierStokes.UniformAngularReset.correctedAngular d c (y, eta)
Instances For
History, given by (5 / 8) * d.core.P * shape eta + primitive (correctedWeight d c eta) y.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Moment candidate, given by (1 + q y) * releaseWeight d y / (1 - d.h).
Equations
- NavierStokes.ReleaseMoments.momentCandidate d q y = (1 + q y) * NavierStokes.ReleaseMoments.releaseWeight d y / (1 - d.h)
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The lag equation turns the candidate into a primitive of the actual release weight. This is the uniqueness mechanism used below.
Normalized lag, given by (1 - d.h) * history d c eta y / releaseWeight d y - 1.
Equations
- NavierStokes.ReleaseMoments.normalizedLag d c eta y = (1 - d.h) * NavierStokes.ReleaseMoments.history d c eta y / NavierStokes.ReleaseMoments.releaseWeight d y - 1
Instances For
Power weight, given by powerConstant d * Real.exp ((1 - d.h) * y).
Equations
- NavierStokes.ReleaseMoments.powerWeight d y = NavierStokes.OutgoingTail.powerConstant d * Real.exp ((1 - d.h) * y)
Instances For
Radial H, given by Real.sqrt (2 * X) * correctedAngular d c (Real.log X, eta).
Equations
- NavierStokes.ReleaseMoments.radialH d c eta X = √(2 * X) * NavierStokes.UniformAngularReset.correctedAngular d c (Real.log X, eta)
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The eventual physical history, in the manuscript's X coordinate.
The exact renormalized angular moment (12), for the actual corrected field and the actual eventual power coefficient.
The actual scheduled correction has the exact renormalized angular
moment and eventual physical history for a common small-lam threshold.