Forced Fourier mode calculus on the space-time cell #
Support lemmas for the forced weak energy identity: the forcing seen by a smooth periodic spatial mode, its integrability, and the finite Fourier sums attached to a weak path.
noncomputable def
AVenhance.Infra.Section5.RelativeError.forcedModeIntegrand
(κ : ℝ)
(Du : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2)
(G : ℝ × Homogenization.Vec 2 → ℝ)
(F : ℝ × Homogenization.Vec 2 → Homogenization.Vec 2)
(ψ : Homogenization.Vec 2 → ℝ)
(p : ℝ × Homogenization.Vec 2)
:
The forcing density seen by a smooth spatial mode ψ: transport/forcing scalar G,
diffusion κ Du·∇ψ and flux F·∇ψ.
Equations
- One or more equations did not get rendered due to their size.
Instances For
noncomputable def
AVenhance.Infra.Section5.RelativeError.forcedModeForcing
(κ : ℝ)
(Du : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2)
(G : ℝ × Homogenization.Vec 2 → ℝ)
(F : ℝ × Homogenization.Vec 2 → Homogenization.Vec 2)
(ψ : Homogenization.Vec 2 → ℝ)
(s : ℝ)
:
The time-slice integral of forcedModeIntegrand.
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
AVenhance.Infra.Section5.RelativeError.forced_continuous_bound
{Z : Homogenization.Vec 2 → ℝ}
(hZ : Continuous Z)
:
A continuous bounded function of the spatial variable alone is bounded on the time cell.
theorem
AVenhance.Infra.Section5.RelativeError.forced_vecDot_integrable
{Y : ℝ × Homogenization.Vec 2 → Homogenization.Vec 2}
(hY :
∀ (i : Fin 2),
MeasureTheory.MemLp (fun (p : ℝ × Homogenization.Vec 2) => Y p i) 2 (MeasureTheory.volume.restrict timeCube))
{Z : Homogenization.Vec 2 → Homogenization.Vec 2}
(hZ : Continuous Z)
:
MeasureTheory.Integrable (fun (p : ℝ × Homogenization.Vec 2) => Homogenization.vecDot (Y p) (Z p.2))
(MeasureTheory.volume.restrict timeCube)
A coordinatewise L² field paired with a continuous spatial field is integrable.
theorem
AVenhance.Infra.Section5.RelativeError.forcedModeIntegrand_integrable
{κ : ℝ}
{Du : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2}
{G : ℝ × Homogenization.Vec 2 → ℝ}
{F : ℝ × Homogenization.Vec 2 → Homogenization.Vec 2}
(hDu :
∀ (i : Fin 2),
MeasureTheory.MemLp (fun (p : ℝ × Homogenization.Vec 2) => Du p.1 p.2 i) 2 (MeasureTheory.volume.restrict timeCube))
(hG : MeasureTheory.MemLp G 2 (MeasureTheory.volume.restrict timeCube))
(hF :
∀ (i : Fin 2),
MeasureTheory.MemLp (fun (p : ℝ × Homogenization.Vec 2) => F p i) 2 (MeasureTheory.volume.restrict timeCube))
{ψ : Homogenization.Vec 2 → ℝ}
(hψ : ContDiff ℝ (↑⊤) ψ)
:
The mode forcing density is integrable on the time cell.
theorem
AVenhance.Infra.Section5.RelativeError.forcedModeForcing_intervalIntegrable
{κ : ℝ}
{Du : ℝ → Homogenization.Vec 2 → Homogenization.Vec 2}
{G : ℝ × Homogenization.Vec 2 → ℝ}
{F : ℝ × Homogenization.Vec 2 → Homogenization.Vec 2}
(hDu :
∀ (i : Fin 2),
MeasureTheory.MemLp (fun (p : ℝ × Homogenization.Vec 2) => Du p.1 p.2 i) 2 (MeasureTheory.volume.restrict timeCube))
(hG : MeasureTheory.MemLp G 2 (MeasureTheory.volume.restrict timeCube))
(hF :
∀ (i : Fin 2),
MeasureTheory.MemLp (fun (p : ℝ × Homogenization.Vec 2) => F p i) 2 (MeasureTheory.volume.restrict timeCube))
{ψ : Homogenization.Vec 2 → ℝ}
(hψ : ContDiff ℝ (↑⊤) ψ)
:
IntervalIntegrable (forcedModeForcing κ Du G F ψ) MeasureTheory.volume 0 1
Mode forcing is interval integrable on [0,1].