Actual spatial jets outside a closed support and for angle-independent fields.
Precisely the spatial parts of the jet that occur in the packet nonlinearities.
- spatial (θ : ℝ) (v : EulerSmoothLimit.Space) : (J θ).2 (EulerPacketPointJets.spatialInjection v) = (J 0).2 (EulerPacketPointJets.spatialInjection v)
Instances For
theorem
EulerPacketCylinderField.AngleIndependentJet.add
{J K : ℝ → EulerPacketPointJets.VectorJet}
(hJ : AngleIndependentJet J)
(hK : AngleIndependentJet K)
:
AngleIndependentJet fun (θ : ℝ) => J θ + K θ
theorem
EulerPacketCylinderField.raw_fderiv_zero_outside
{T : ℝ}
{raw : EulerPacketProfileRecursion.VectorField}
(S : Set EulerSmoothLimit.Space)
(hS : IsClosed S)
(h : ∀ (t : ↑(Set.Icc 0 T)), ∀ x ∉ S, ∀ (θ : ℝ), raw (↑t, x, θ) = 0)
(t : ↑(Set.Icc 0 T))
(x : EulerSmoothLimit.Space)
(hx : x ∉ S)
(θ : ℝ)
:
theorem
EulerPacketCylinderField.slicedJet_angleIndependent_of_support
{T : ℝ}
{raw : EulerPacketProfileRecursion.VectorField}
(s : Set ℝ)
(S : Set EulerSmoothLimit.Space)
(hS : IsClosed S)
(h : ∀ (t : ↑(Set.Icc 0 T)), ∀ x ∉ S, ∀ (θ : ℝ), raw (↑t, x, θ) = 0)
(t : ↑(Set.Icc 0 T))
(x : EulerSmoothLimit.Space)
(hx : x ∉ S)
:
AngleIndependentJet fun (θ : ℝ) => EulerPacketPointJets.slicedJet s raw (↑t, x, θ)
theorem
EulerPacketCylinderField.Field.raw_fderiv_of_angleIndependent
{P T : ℝ}
[Fact (0 < P)]
{raw : EulerPacketProfileRecursion.VectorField}
(G : Field P T raw)
(h : ∀ (t : ↑(Set.Icc 0 T)) (x : EulerSmoothLimit.Space) (θ : ℝ), raw (↑t, x, θ) = raw (↑t, x, 0))
(t : ↑(Set.Icc 0 T))
(x : EulerSmoothLimit.Space)
(θ : ℝ)
:
theorem
EulerPacketCylinderField.Field.slicedJet_angleIndependent
{P T : ℝ}
[Fact (0 < P)]
{raw : EulerPacketProfileRecursion.VectorField}
(G : Field P T raw)
(s : Set ℝ)
(h : ∀ (t : ↑(Set.Icc 0 T)) (x : EulerSmoothLimit.Space) (θ : ℝ), raw (↑t, x, θ) = raw (↑t, x, 0))
(t : ↑(Set.Icc 0 T))
(x : EulerSmoothLimit.Space)
:
AngleIndependentJet fun (θ : ℝ) => EulerPacketPointJets.slicedJet s raw (↑t, x, θ)