Pressure convergence in the Leray limit #
The regularized transport tensor converges in L^(3/2) when both velocity
factors converge strongly in L³, and the space-time Riesz pressure preserves
that convergence on every finite slab (prop:leray-pressure-limit).
The product-coordinate space-time region corresponding to the interval
(0,T) in the Leray pressure limit (prop:leray-pressure-limit).
Equations
Instances For
noncomputable def
CKN.Leray.lerayProductPressureOnSlab
(T : ℝ)
(v w : Foundation.Parabolic.Vec3 × ℝ → Foundation.Parabolic.Vec3)
(hv : MeasureTheory.MemLp v 3 (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
(hw : MeasureTheory.MemLp w 3 (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
:
The canonical space-time Riesz pressure on a finite slab, formed from the
product of two L³ velocity fields.
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
CKN.Leray.lerayPressureLimit_Lthree
(T : ℝ)
(Jseq useq : ℕ → Foundation.Parabolic.Vec3 × ℝ → Foundation.Parabolic.Vec3)
(u : Foundation.Parabolic.Vec3 × ℝ → Foundation.Parabolic.Vec3)
(hJseq : ∀ (n : ℕ), MeasureTheory.MemLp (Jseq n) 3 (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
(huseq : ∀ (n : ℕ), MeasureTheory.MemLp (useq n) 3 (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
(hu : MeasureTheory.MemLp u 3 (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
(hJconv :
Filter.Tendsto
(fun (n : ℕ) => MeasureTheory.eLpNorm (Jseq n - u) 3 (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
Filter.atTop (nhds 0))
(huconv :
Filter.Tendsto
(fun (n : ℕ) => MeasureTheory.eLpNorm (useq n - u) 3 (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
Filter.atTop (nhds 0))
:
Filter.Tendsto
(fun (n : ℕ) =>
MeasureTheory.eLpNorm (lerayProductPressureOnSlab T (Jseq n) (useq n) ⋯ ⋯ - lerayProductPressureOnSlab T u u hu hu)
(ENNReal.ofReal (3 / 2)) (MeasureTheory.volume.restrict (lerayPressureLimitSlab T)))
Filter.atTop (nhds 0)
The regularized Leray pressures converge strongly in L^(3/2) on each
finite time slab under the exact strong L³ velocity convergences in
prop:leray-limit.