The actual cylinder endpoint inverse agrees at every spatial/angular point with the finite-dimensional stationary history. The proof first recovers genuine coordinate representatives and their time derivatives, then uses the proved two-endpoint energy uniqueness theorem.
Actual pointwise representatives for coordinate spaces embedded in Space. A fixed bounded embedding and left inverse transfer the proved H³ point evaluation. This will apply to the two-dimensional reference plane, without identifying an L² normal with a pointwise normal vector.
Point field, given by L (EulerCylinderSmoothOrbit.pointField P (pathMap P J p) (pathMap_orbit_contDiff P J p hp) t x).
Equations
- EulerCylinderRetractRepresentative.pointField P J L p hp t x = L (EulerCylinderSmoothOrbit.pointField P ((EulerCylinderConstantMap.pathMap P J) p) ⋯ t x)
Instances For
Point path as an element of C(K,U).
Equations
- EulerCylinderRetractRepresentative.pointPath P J L p hp x = { toFun := fun (t : K) => EulerCylinderRetractRepresentative.pointField P J L p hp t x, continuous_toFun := ⋯ }
Instances For
Initial time integration commutes with the genuine mixed cylinder action.
Endpoint point displacement, given by pointPath P J L (D.endpointDisplacement P Y) (D.endpointDisplacement_orbit_contDiff P hQ hQ₁ hH Y hY) x.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Endpoint point coordinate, given by pointPath P J L (D.endpointCoordinate P Y) (D.endpointCoordinate_orbit_contDiff P hQ hQ₁ hH Y hY) x.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Endpoint point acceleration, given by pointPath P J L (D.endpointAcceleration P Y) (D.endpointAcceleration_orbit_contDiff P hQ hQ₁ hH Y hY) x.
Equations
- One or more equations did not get rendered due to their size.