Time identities derived from the source deformation data, including the actual inverse and normal paths.
The actual time coefficient of the vector potential, with uniform factorial bounds.
The vector-potential multiplier is a fixed linear contraction of the normal functional.
Normal vector, given by (ContinuousLinearMap.apply ℝ Space (1 : ℝ)).comp (realAdjoint (U := Space) (E := ℝ)).
Equations
Instances For
Normal potential map, given by -(crossOperator.comp normalVector).
Equations
Instances For
No additional inverse or derivative estimate is needed after constructing the normal functional.
The literal vector-potential multiplier inherits the source normal coefficient bounds.
Normal field: an abbreviation for Space →ᵇ (Space →L[ℝ] ℝ).
Equations
Instances For
Potential field: an abbreviation for Space →ᵇ (Space →L[ℝ] Space).
Equations
Instances For
Cache the standard NormedAddCommGroup NormalField instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ NormalField instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup PotentialField instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ PotentialField instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup C(K,NormalField) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ C(K,NormalField) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup C(K,PotentialField) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ C(K,PotentialField) instance to shorten typeclass
synthesis.
Instances For
Potential path map, given by (normalPotentialMap.compLeftContinuousBounded Space).compLeftContinuous ℝ K.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Potential coefficient, given by potentialPathMap (normalFunctional m c hc hm).
Equations
Instances For
The source coefficient passes through a linear contraction, with no radius or shift change.
An inverse-free polynomial formula for the actual normal multiplier's time derivative.
Differentiate the normal functional using only itself and the normal's derivative column.
Equations
- EulerPacketCrossProduct.normalTimeMap N Q₁ = (N ∘SL ContinuousLinearMap.adjoint N) ∘SL ContinuousLinearMap.adjoint Q₁ - 2 • (N ∘SL Q₁) ∘SL N
Instances For
This polynomial coefficient is exactly the derivative of −cross(m)/|m|².
Cache the standard NormedAddCommGroup (Space →L[ℝ] ℝ) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →L[ℝ] ℝ) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup (ℝ →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ (ℝ →L[ℝ] Space) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup NormalField instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ NormalField instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup (Space →ᵇ ℝ →L[ℝ] Space) instance to shorten
typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →ᵇ ℝ →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedAddCommGroup (ℝ →L[ℝ] ℝ) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ (ℝ →L[ℝ] ℝ) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup (Space →ᵇ ℝ →L[ℝ] ℝ) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →ᵇ ℝ →L[ℝ] ℝ) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedAddCommGroup C(K,NormalField) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ C(K,NormalField) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup C(K,Space →ᵇ ℝ →L[ℝ] Space) instance to shorten
typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ C(K,Space →ᵇ ℝ →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedAddCommGroup C(K,Space →ᵇ ℝ →L[ℝ] ℝ) instance to shorten
typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ C(K,Space →ᵇ ℝ →L[ℝ] ℝ) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedAddCommGroup (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedAddCommGroup PotentialField instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ PotentialField instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup C(K,PotentialField) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ C(K,PotentialField) instance to shorten typeclass
synthesis.
Instances For
Time normal path, constructed using pathCompositionMap.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Potential time coefficient, given by potentialPathMap (timeNormalPath (normalFunctional m c hc hm) (normalColumn m₁).field).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The derivative coefficient is polynomial in the already constructed normal functional.
The potential time coefficient from an actual continuous, translation-smooth normal derivative path.
Column path, given by mapCoefficientPath (ContinuousLinearMap.toSpanSingletonLIE ℝ Space).toLinearIsometry.toContinuousLinearMap.
Equations
Instances For
Potential time path, given by potentialPathMap (timeNormalPath (normalFunctional m c hc hm) (columnPath m₁)).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Genuine time derivatives of the inverse deformation and its transported normal.
Cache the standard NormedAddCommGroup (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Inverse unit, bundling val, inv, val_inv, inv_val.
Equations
- EulerDeformationTime.inverseUnit F G hFG hGF = { val := F, inv := G, val_inv := hFG, inv_val := hGF }
Instances For
F_t=MF implies (F⁻¹)_t=−F⁻¹M on the same closed time set.
Adjoint vector as an element of (Space →L[ℝ] Space) →L[ℝ] Space.
Equations
Instances For
The actual transported normal satisfies m_t=−M* m.
Cache the standard NormedAddCommGroup (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →L[ℝ] Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedAddCommGroup (Space →ᵇ Space →L[ℝ] Space) instance to shorten
typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →ᵇ Space →L[ℝ] Space) instance to shorten
typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup C(Icc (0 : ℝ) D.T,Space →ᵇ Space →L[ℝ] Space)
instance to shorten typeclass synthesis.
Equations
Instances For
Cache the standard NormedSpace ℝ C(Icc (0 : ℝ) D.T,Space →ᵇ Space →L[ℝ] Space) instance to
shorten typeclass synthesis.
Equations
Instances For
Cache the standard NormedAddCommGroup (Space →ᵇ Space) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ (Space →ᵇ Space) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup C(Icc (0 : ℝ) D.T,Space →ᵇ Space) instance to
shorten typeclass synthesis.
Equations
Instances For
Cache the standard NormedSpace ℝ C(Icc (0 : ℝ) D.T,Space →ᵇ Space) instance to shorten
typeclass synthesis.
Equations
Instances For
The derivative of the inverse is constructed from the original fields.
Equations
Instances For
The derivative of the transported normal is the fixed adjoint-vector map of that path.
Equations
Instances For
No differentiability of F⁻¹ is assumed: it follows from the actual inverse identities and F_t=MF.
The actual time coefficient for the periodic-potential multiplier.