Coherence of the actual five-row rank correction #
The debt is recomputed from the complete incoming state. Primitive chart data and the shared normalized inverse are transported before applying the actual variable-gauge stream and pressure constructors.
The whole-fiber moment of a compatible field, using only local slow regularity and the actual torus covering.
Reference fields needed for the actual three measured debts.
- radial : ContDiffOn ℝ (↑⊤) (u.gr C n) (PhysicalMeanDomain.slowDomain U)
- angular : ContDiffOn ℝ (↑⊤) ((MeanIncrementBounds.thetaAxial C.base u.mean + u.covariance 2 1) n) (PhysicalMeanDomain.slowDomain U)
- axial : ContDiffOn ℝ (↑⊤) ((MeanIncrementBounds.axialAxial C.base u.mean + u.covariance 2 2) n) (PhysicalMeanDomain.slowDomain U)
- radial_periodic : PhysicalMeanDomain.PeriodicOn U (u.gr C n)
- angular_periodic : PhysicalMeanDomain.PeriodicOn U ((MeanIncrementBounds.thetaAxial C.base u.mean + u.covariance 2 1) n)
- axial_periodic : PhysicalMeanDomain.PeriodicOn U ((MeanIncrementBounds.axialAxial C.base u.mean + u.covariance 2 2) n)
Instances For
All three debts are measured from the full base and state. The powers
are pressure c², angular c²/l³, and axial c²/l².
Primitive rank data use one dimensionless kernel. No rank-output or debt equality is a field of this structure.
- coefficient (s : S) : s ∈ V → r.coefficient n s = rr.coefficient nr (P s)
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Naturality of the literal moving-gauge rank potential. Its source is the already constructed five-row inverse of the measured debt.
All three components are the actual stream reconstruction of the rank correction. No output-increment coherence is assumed.
The actual state before the rank step's pressure is reconstructed.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Coherence survives the complete rank step, including the pressure recomputed from the new actual radial residual.
The actual normalized data used by the recurrence #
All five rows, against the full base #
The five-row conclusion is transported from the actual reference rank solve. Both background slices here are the complete stored base.
The physical axial unit has the required chart differential, with the
actual viscosity/axial coefficient Q^h.
Concrete normalized rank stage at the common cover. Every rank parameter and axial scaling law is derived from the shared data.