The actual flow displacement and material velocity, with every spatial jet in the uniform continuous-time bounded-field space.
Genuine joint time-space regularity of the constructed flow and its inverse. Interior C² uses only the actual first time derivative of the velocity coefficient, together with its existing smooth spatial jets.
Joint time-space differentiability of a genuine smooth family of continuous paths, and the actual mixed derivative of its spatial Jacobian.
Time slice, given by extendPath T hT (f x) t.
Equations
- EulerSmoothPathJoint.timeSlice T hT f t x = EulerVolterraConvolution.extendPath T hT (f x) t
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Spatial derivative as an element of C(Icc (0 : ℝ) T,E →L[ℝ] V).
Equations
- EulerSmoothPathJoint.spatialDerivative T f x = (ContinuousLinearMap.compLeftContinuous ℝ ↑(Set.Icc 0 T) ↑↑(continuousMultilinearCurryFin1 ℝ E V)) (EulerSmoothPathTimeJets.jetFamily T f 1 x)
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Joint derivative, given by (ContinuousLinearMap.toSpanSingleton ℝ (timeSlice T hT q t x)).coprod (timeSlice T hT (spatialDerivative T f) t x).
Equations
- One or more equations did not get rendered due to their size.
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The actual acceleration of the constructed nonlinear flow is the material derivative of its velocity, including the one-sided endpoint identities. All coefficient time derivatives are literal hypotheses.
Acceleration family, given by A₁.superposition (pathFamily T hT A x) + multiplier (A.derivative.superposition (pathFamily T hT A x)) (velocityFamily T hT A x).
Equations
- One or more equations did not get rendered due to their size.
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Time lift equiv, constructed using ContinuousLinearEquiv.equivOfInverse.
Equations
- One or more equations did not get rendered due to their size.
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Lift forward, given by (p.1, (flowData T hT A).forward p.1 p.2).
Equations
- EulerSmoothBanachFlow.liftForward T hT A p = (p.1, (EulerSmoothBanachFlow.flowData T hT A).forward p.1 p.2)
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Lift backward, given by (p.1, (flowData T hT A).backward p.1 p.2).
Equations
- EulerSmoothBanachFlow.liftBackward T hT A p = (p.1, (EulerSmoothBanachFlow.flowData T hT A).backward p.1 p.2)
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Constructing literal bounded smooth coefficient paths from an actual smooth path family and uniform bounds on its differentiated evolution.
Uniform bounds on a genuine time derivative turn a continuous family of paths into a continuous path of bounded fields.
Bounded slice, given by BoundedContinuousFunction.ofNormedAddCommGroup (fun x => f x t) ((ContinuousMap.evalCLM ℝ t).continuous.comp hf) C (hC t).
Equations
- EulerBoundedPathFamily.boundedSlice T f hf C hC t = BoundedContinuousFunction.ofNormedAddCommGroup (fun (x : X) => (f x) t) ⋯ C ⋯
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Bounded path, bundling toFun, continuous_toFun.
Equations
- EulerBoundedPathFamily.boundedPath T hT f q hf C D hC hD hq hd = { toFun := EulerBoundedPathFamily.boundedSlice T f hf C hC, continuous_toFun := ⋯ }
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Cache the standard NormedAddCommGroup (E [×n]→L[ℝ] V) instance to shorten typeclass
synthesis.
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Cache the standard NormedSpace ℝ (E [×n]→L[ℝ] V) instance to shorten typeclass synthesis.
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Cache the standard NormedAddCommGroup (E →ᵇ (E [×n]→L[ℝ] V)) instance to shorten typeclass
synthesis.
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Cache the standard NormedSpace ℝ (E →ᵇ (E [×n]→L[ℝ] V)) instance to shorten typeclass
synthesis.
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Of path family, bundling field, smooth, change, jet and the required compatibility
proofs.
Equations
- One or more equations did not get rendered due to their size.
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Cache the standard NormedAddCommGroup (E [×n]→L[ℝ] E) instance to shorten typeclass
synthesis.
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Cache the standard NormedSpace ℝ (E [×n]→L[ℝ] E) instance to shorten typeclass synthesis.
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Cache the standard NormedAddCommGroup (E →ᵇ (E [×n]→L[ℝ] E)) instance to shorten typeclass
synthesis.
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Cache the standard NormedSpace ℝ (E →ᵇ (E [×n]→L[ℝ] E)) instance to shorten typeclass
synthesis.
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Displacement coefficient, constructed using SmoothTimeField.ofPathFamily.
Equations
- One or more equations did not get rendered due to their size.
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Velocity coefficient, constructed using SmoothTimeField.ofPathFamily.
Equations
- One or more equations did not get rendered due to their size.