Passing to the limit in the weak form #
If weak solutions with diffusivities κ j → 0 converge uniformly in L²(cell) to Θ, then Θ
satisfies the divergence-form transport identity, has weakly continuous pairings, and bounded
energy.
theorem
AVenhance.Infra.FullTheorem.TransportLimit.l2NormSq_sub_le
{f g : Homogenization.Vec 2 → ℝ}
(hf : Homogenization.MemL2On unitCube f)
(hg : Homogenization.MemL2On unitCube g)
:
theorem
AVenhance.Infra.FullTheorem.TransportLimit.limit_l2_bound
{θ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
{Θ : ℝ → Homogenization.Vec 2 → ℝ}
(hmem : ∀ (j : ℕ), ∀ t ∈ Set.Icc 0 1, Homogenization.MemL2On unitCube (θ j t))
(hbd : ∀ (j : ℕ), ∃ (C : ℝ), ∀ t ∈ Set.Icc 0 1, l2NormSq (θ j t) ≤ C)
(hΘ : ∀ t ∈ Set.Icc 0 1, Homogenization.MemL2On unitCube (Θ t))
(hunif :
∀ (η : ℝ),
0 < η → ∃ (N : ℕ), ∀ j ≥ N, ∀ t ∈ Set.Icc 0 1, √(l2NormSq fun (x : Homogenization.Vec 2) => θ j t x - Θ t x) ≤ η)
:
Bounded energy of the limit.
theorem
AVenhance.Infra.FullTheorem.TransportLimit.limit_weak_continuity
{θ : ℕ → ℝ → Homogenization.Vec 2 → ℝ}
{Θ : ℝ → Homogenization.Vec 2 → ℝ}
(hmem : ∀ (j : ℕ), ∀ t ∈ Set.Icc 0 1, Homogenization.MemL2On unitCube (θ j t))
(hΘ : ∀ t ∈ Set.Icc 0 1, Homogenization.MemL2On unitCube (Θ t))
(hcont :
∀ (j : ℕ) (ψ : Homogenization.Vec 2 → ℝ),
ContDiff ℝ (↑⊤) ψ →
IsZ2Periodic ψ →
ContinuousOn (fun (t : ℝ) => ∫ (x : Homogenization.Vec 2) in unitCube, θ j t x * ψ x) (Set.Icc 0 1))
(hunif :
∀ (η : ℝ),
0 < η → ∃ (N : ℕ), ∀ j ≥ N, ∀ t ∈ Set.Icc 0 1, √(l2NormSq fun (x : Homogenization.Vec 2) => θ j t x - Θ t x) ≤ η)
{ψ : Homogenization.Vec 2 → ℝ}
(hψ : ContDiff ℝ (↑⊤) ψ)
(hψp : IsZ2Periodic ψ)
:
ContinuousOn (fun (t : ℝ) => ∫ (x : Homogenization.Vec 2) in unitCube, Θ t x * ψ x) (Set.Icc 0 1)
Weak continuity of the limit's pairings with smooth periodic functions.