The canonical signed physical family and its current-band realization #
The dependent family, both signed labels, and its positive physical harmonic are retained. Native faces are treated by the literal zero mask before a current-band comparison is used.
Geometry for current signed waves in physical polar charts #
The actual active annulus is covered for every band whose physical scale
ratio lies in (1/2,2). An explicit change of the chart radius identifies
the scaled Cartesian lift with the full native cylindrical graph.
The annulus estimate uses only comparability of the two positive scales, so it holds throughout the full open native scale window.
The exact unscaled chart radius corresponding to a native chart radius.
Equations
- NavierStokes.ActualSignedPhysicalGeometry.chartRadius a n = a / NavierStokes.ChartScales.Q n ^ (-(1 / 2))
Instances For
The scaled and unscaled charts have exactly the same angle.
No angle choice or auxiliary coordinate is discarded by this identity.
The mean graph's slow coordinate does not depend on its auxiliary cover.
This identity is global and needs no radius or time positivity premise.
Zeros of the actual signed physical coefficients #
The native dyadic mask vanishes at both faces and outside the open native band. This file transfers that literal zero to the canonical physical copy family and to every current-band representation of the same label. The current state and the native reference requests are arbitrary.
Label: an abbreviation for ActualSignedPhysicalBinding.Label.
Equations
Instances For
Full point: an abbreviation for ActualSignedCoherence.FullPoint.
Equations
Instances For
The same native slow point in every current band #
Passing literal raw zeros through the current copy sum #
The fixed physical exterior #
Finite-support sums in physical coordinates #
These identities only use finite support and the literal real-coordinate maps.
They let a physical wave assembly retain an unrestricted label finsum while
identifying its value with the finite active-label sum.
An unrestricted scalar-label sum becomes the finite real-part sum once the labels outside the specified finite set vanish.
Reconstructing the Euclidean vector after the componentwise label sums agrees exactly with summing the real vectors of the active labels.
Full point: an abbreviation for ActualSignedCoherence.FullPoint.
Equations
Instances For
Space time: an abbreviation for ProblemStatement.SpaceTime.
Equations
Instances For
Physical index, given by ActualSignedPhysicalData.positiveIndex (ActualSignedExterior.nativeLabel l).
Equations
Instances For
The exact native-to-common physical graph #
Measured states, defined pointwise by ActualSignedPhysicalBinding.nativeStateData l P u H hp.
Equations
Instances For
Singleton vector mode as an element of ComplexVector.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Singleton pressure mode as an element of ℂ.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Canonical potential as an element of ComplexVector.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Canonical pressure as an element of ℂ.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The two literal zero cases, including both native dyadic faces #
The physical copy sum has the current-band value. The last conclusion is complex-valued: it justifies truncating the original complex sum before taking real parts.
The literal correction cycle's physical fields #
Cycle input, given by (ActualCycleParameters.fixedParameters B N0).afterParticular x.coefficients (commonContext B) x.state.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Curl is taken only after equality of the canonical physical potential on an open neighborhood has been proved. The sole analytic bound concerns the actual current common amplitude.
The canonical physical pressure is the same finite signed pressure sum used by the current correction state.