The force curve of the forced regularized construction #
A locally square-integrable force has a strongly measurable modification on
positive times; its time slices form a strongly measurable curve of L²
fields whose squared norms are integrable on bounded time intervals. This is
the force entering the Duhamel term of eq:reg-mild-forced.
theorem
CKN.Leray.exists_forcedForceModification
{f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3}
(hf : IsLocallySquareIntegrableForce f)
:
∃ (F : Foundation.Parabolic.Vec3 × ℝ → Foundation.Parabolic.Vec3),
MeasureTheory.StronglyMeasurable F ∧ ∀ (T : ℝ),
0 < T →
∀ᵐ (z : Foundation.Parabolic.Vec3 × ℝ) ∂MeasureTheory.volume.restrict (spaceTimeSet Set.univ (Set.Ioo 0 T)), F z = f z
noncomputable def
CKN.Leray.forcedForceMod
(f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3)
(hf : IsLocallySquareIntegrableForce f)
:
A strongly measurable modification of a locally square-integrable force.
Equations
Instances For
theorem
CKN.Leray.forcedForceMod_ae_eq
(f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3)
(hf : IsLocallySquareIntegrableForce f)
{T : ℝ}
(hT : 0 < T)
:
∀ᵐ (z : Foundation.Parabolic.Vec3 × ℝ) ∂MeasureTheory.volume.restrict (spaceTimeSet Set.univ (Set.Ioo 0 T)), forcedForceMod f hf z = f z
theorem
CKN.Leray.realVectorL2OfCoordinateFunction_ae_eq_toLp
(a : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3)
(ha : MeasureTheory.MemLp a 2 MeasureTheory.volume)
:
↑↑(realVectorL2OfCoordinateFunction a ha) =ᵐ[MeasureTheory.volume] fun (y : Foundation.Parabolic.L2Vec3) =>
WithLp.toLp 2 (a y.ofLp)
The class of a square-integrable coordinate field agrees on the Euclidean carrier with the transferred field.
theorem
CKN.Leray.forcedForceSlice_stronglyMeasurable
{F : Foundation.Parabolic.Vec3 × ℝ → Foundation.Parabolic.Vec3}
(hF : MeasureTheory.StronglyMeasurable F)
:
The force slice curve of a strongly measurable field is strongly measurable.
theorem
CKN.Leray.norm_forcedForceSlice_le
(F : Foundation.Parabolic.Vec3 × ℝ → Foundation.Parabolic.Vec3)
(s : ℝ)
:
‖forcedForceSlice F s‖ ≤ 2 * (MeasureTheory.eLpNorm (fun (x : Foundation.Parabolic.Vec3) => F (x, s)) 2 MeasureTheory.volume).toReal
theorem
CKN.Leray.memLp_forcedForceMod_prod
(f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3)
(hf : IsLocallySquareIntegrableForce f)
{T : ℝ}
(hT : 0 < T)
:
MeasureTheory.MemLp (forcedForceMod f hf) 2 (MeasureTheory.volume.prod (MeasureTheory.volume.restrict (Set.Ioo 0 T)))
The strongly measurable modification is square integrable on every positive-time slab.
theorem
CKN.Leray.integrableOn_forcedForceSlice_sq
(f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3)
(hf : IsLocallySquareIntegrableForce f)
(T : ℝ)
:
MeasureTheory.IntegrableOn (fun (s : ℝ) => ‖forcedForceSlice (forcedForceMod f hf) s‖ ^ 2) (Set.Ioc 0 T)
MeasureTheory.volume
The squared norms of the force curve are integrable on bounded time intervals.