The actual viscous term vanishes uniformly for a uniformly Sobolev-bounded approximation family.
A concrete strictly positive sequence of viscosities tending to zero.
Equations
- EulerViscosityDefect.viscositySequence n = 1 / (↑n + 1)
Instances For
Each concrete approximation viscosity is strictly positive.
Each concrete approximation viscosity lies in the fixed unit interval.
The actual chosen viscosity sequence converges to zero.
noncomputable def
EulerViscosityDefect.viscousDefect
(period : ℝ)
[Fact (0 < period)]
{q : ℕ}
(hq : 2 ≤ q)
(ν T : ℝ)
(e : C(↑(Set.Icc 0 T), ↥(EulerCylinderSobolevSpace.SobolevSpace period q)))
:
The literal viscosity times the spatial Laplacian, as a continuous L² time path.
Equations
- EulerViscosityDefect.viscousDefect period hq ν T e = ν • (ContinuousLinearMap.compLeftContinuous ℝ (↑(Set.Icc 0 T)) (EulerSobolevHeatGenerator.laplacianEvaluation period q hq)) e
Instances For
theorem
EulerViscosityDefect.viscousDefect_tendsto_zero
(period : ℝ)
[Fact (0 < period)]
{q : ℕ}
(hq : 2 ≤ q)
(T M : ℝ)
(e : ℕ → C(↑(Set.Icc 0 T), ↥(EulerCylinderSobolevSpace.SobolevSpace period q)))
(he : ∀ (n : ℕ), ‖e n‖ ≤ M)
:
Filter.Tendsto (fun (n : ℕ) => viscousDefect period hq (viscositySequence n) T (e n)) Filter.atTop (nhds 0)
Every uniformly bounded genuine Sobolev approximation family has a uniformly vanishing viscous PDE defect.