Translation invariance of the ordinary solenoidal projection #
The nonoscillating inverse uses spatial difference quotients. These act on the actual R³ L² space, preserve its weak divergence constraint, and commute with the orthogonal solenoidal projection.
Translation, given by Lp.compMeasurePreservingₗᵢ ℝ (fun x : Space => x + a) (measurePreserving_add_right (volume : Measure Space) a).
Equations
- EulerMeanSolenoidal.translation a = MeasureTheory.Lp.compMeasurePreservingₗᵢ ℝ (fun (x : EulerSmoothLimit.Space) => x + a) ⋯
Instances For
theorem
EulerMeanSolenoidal.translation_ae
(a : EulerSmoothLimit.Space)
(u : ↥L2)
:
↑↑((translation a) u) =ᵐ[MeasureTheory.volume] fun (x : EulerSmoothLimit.Space) => ↑↑u (x + a)
theorem
EulerMeanSolenoidal.gradient_translated
(a : EulerSmoothLimit.Space)
(φ : EulerSmoothLimit.Space → ℝ)
(x : EulerSmoothLimit.Space)
:
theorem
EulerMeanSolenoidal.translated_generator
(a : EulerSmoothLimit.Space)
{g : ↥L2}
(hg : g ∈ gradientGenerators)
:
theorem
EulerMeanSolenoidal.translation_gradient_mem
(a : EulerSmoothLimit.Space)
{g : ↥L2}
(hg : g ∈ gradientSpace)
:
theorem
EulerMeanSolenoidal.translation_solenoidal_mem
(a : EulerSmoothLimit.Space)
{u : ↥L2}
(hu : u ∈ solenoidalSpace)
:
theorem
EulerMeanSolenoidal.solenoidalProjection_translation
(a : EulerSmoothLimit.Space)
(u : ↥L2)
:
Ordinary Helmholtz projection commutes with every spatial translation.