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LeanPool.NavierStokesAndEuler.Euler.TransversePacketData

Source deformation data for the concrete transverse packet provider #

Only the prescribed deformation, its inverse, and their actual time identity are inputs. The transverse frame, normal, both coercivity constants, and all geometry needed by the forward solve are derived below.

Source geometry for the bounded frame and normal #

The literal fields Q=F R⊥ and m=F⁻ᵀm₀ satisfy the tangency, range, strain, and quantitative normal lower bounds used by the actual transverse solver. Only the original deformation and its genuine pointwise inverse are inputs.

The literal source frame as a uniformly smooth bounded coefficient path #

The reference-plane restriction is a fixed linear contraction. The actual source fields F and F_t therefore construct the full bounded frame fields, with their genuine jets and time derivative. A pointwise bound on F⁻¹ proves the uniform frame coercivity used by the constructed Gram inverse.

The uniform inverse-frame bound gives the precise squared lower frame bound.

theorem EulerTransverseBoundedFrame.normalCoefficient_lower (m₀ : EulerSmoothLimit.Space) {K : Type u_1} [TopologicalSpace K] [CompactSpace K] (F FInv : EulerMeanCoefficients.SmoothCoefficientPath K (EulerSmoothLimit.Space →L[] EulerSmoothLimit.Space)) (hm₀ : m₀ = 1) (hInv : ∀ (t : K) (x v : EulerSmoothLimit.Space), ((FInv.field t) x) (((F.field t) x) v) = v) (B : ) (hB : 0 < B) (hFnorm : ∀ (t : K) (x : EulerSmoothLimit.Space), (F.field t) x B) (t : K) (x : EulerSmoothLimit.Space) :
B⁻¹ ^ 2 ((normalCoefficient m₀ FInv).field t) x ^ 2

The source inverse identity also prevents degeneration of the normal.

Data, collecting T, T_pos, support, support_compact, m₀, m₀_unit and their compatibility conditions.

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    @[reducible, inline]

    Frame: an abbreviation for coefficient D.m₀ D.R D.F.

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      Inverse bound, given by 1+‖D.FInv.field‖.

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        Frame bound, given by 1+‖D.F.field‖.

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          Frame lower, given by D.inverseBound⁻¹^2.

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            Normal lower, given by D.frameBound⁻¹^2.

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              Uniform coercivity follows from the actual inverse deformation.

              The scalar pressure inverse is nondegenerate by the same source identity.

              theorem EulerTransversePacketProvider.Data.frame_range {U : Type u_1} [NormedAddCommGroup U] [InnerProductSpace U] (D : Data U) (t : (Set.Icc 0 D.T)) (x η : EulerSmoothLimit.Space) ( : inner ((D.normal.field t) x) η = 0) :
              ∃ (v : U), ((D.frame.field t) x) v = η