The literal periodic vector potential as an actual continuous cylinder L² path.
Time differentiation of the actual normalized angular integral on the cylinder.
Same-radius mixed-word and continuous-time estimates for the actual angular operator.
Cache the standard NormedAddCommGroup C(K,LiftL2 P) instance to shorten typeclass
synthesis.
Instances For
Cache the standard NormedSpace ℝ C(K,LiftL2 P) instance to shorten typeclass synthesis.
Instances For
Cache the standard NormedAddCommGroup (C(K,LiftL2 P) →L[ℝ] C(K,LiftL2 P)) instance to
shorten typeclass synthesis.
Instances For
Cache the standard NormedSpace ℝ (C(K,LiftL2 P) →L[ℝ] C(K,LiftL2 P)) instance to shorten
typeclass synthesis.
Instances For
Path primitive, given by (primitive P).compLeftContinuous ℝ K.
Equations
Instances For
The angular operation preserves the same fixed base order and radius in the true time supremum.
The representative of the time-dependent L² primitive is the same explicit angular integral.
The literal primitive differentiates within the closed time interval at every angle.
Potential path, given by fullMultiplierMap P B (pathPrimitive P p).
Equations
Instances For
Potential field, given by pointField P (potentialPath P B p) (potentialPath_orbit P B hB p hp) t.
Equations
- EulerCylinderPotential.potentialField P B hB p hp t = EulerCylinderSmoothOrbit.pointField P (EulerCylinderPotential.potentialPath P B p) ⋯ t
Instances For
The canonical representative is the coefficient times the literal angular primitive.
The L² construction is the same actual field used in the compact Piola construction.
Angular integration and multiplication retain the input radius and external shift.