The complete transverse history/forward field as a genuine cylinder path #
All raw fields are canonical continuous representatives of the constructed L² paths. Restriction recovers the actual history and forward solutions.
Vector, defined pointwise by pointField P (velocityPath τ hτ hτT B G) (velocityPath_orbit τ hτ hτT B G) (D.clamp z.1) (z.2.1,(z.2.2 : AddCircle P)).
Equations
- EulerTransversePacketJoin.vector τ hτ hτT B G z = EulerCylinderSmoothOrbit.pointField P (EulerTransversePacketJoin.velocityPath τ hτ hτT B G) ⋯ (D.clamp z.1) (z.2.1, ↑z.2.2)
Instances For
Vector derivative, defined pointwise by pointField P (derivativePath τ hτ hτT B G) (derivativePath_orbit τ hτ hτT B G) (D.clamp z.1) (z.2.1,(z.2.2 : AddCircle P)).
Equations
- EulerTransversePacketJoin.vectorDerivative τ hτ hτT B G z = EulerCylinderSmoothOrbit.pointField P (EulerTransversePacketJoin.derivativePath τ hτ hτT B G) ⋯ (D.clamp z.1) (z.2.1, ↑z.2.2)
Instances For
Scalar, defined pointwise by scalarPointField P (pressurePath τ hτ hτT B G) (pressurePath_orbit τ hτ hτT B G) (D.clamp z.1) (z.2.1,(z.2.2 : AddCircle P)).
Equations
- EulerTransversePacketJoin.scalar τ hτ hτT B G z = EulerCylinderScalarPrimitive.scalarPointField P (EulerTransversePacketJoin.pressurePath τ hτ hτT B G) ⋯ (D.clamp z.1) (z.2.1, ↑z.2.2)
Instances For
Vector field, bundling path, orbit, raw_eq.
Equations
- EulerTransversePacketJoin.vectorField τ hτ hτT B G = { path := EulerTransversePacketJoin.velocityPath τ hτ hτT B G, orbit := ⋯, raw_eq := ⋯ }
Instances For
Vector derivative field, bundling path, orbit, raw_eq.
Equations
- EulerTransversePacketJoin.vectorDerivativeField τ hτ hτT B G = { path := EulerTransversePacketJoin.derivativePath τ hτ hτT B G, orbit := ⋯, raw_eq := ⋯ }
Instances For
Scalar gradient field, constructed using EulerPacketCylinderField.scalarGradientField.
Equations
- One or more equations did not get rendered due to their size.