Scalar Grönwall estimate for vorticity energy #
This scalar estimate is the time integration step in the smooth energy argument
for lem:localized-vorticity-energy.
theorem
ESS.vorticityEnergyGronwallCore
{a b K e₀ : ℝ}
{e de f : ℝ → ℝ}
(hab : a ≤ b)
(hK : 0 ≤ K)
(hecont : ContinuousOn e (Set.Icc a b))
(hfcont : Continuous f)
(hepos : ∀ t ∈ Set.Icc a b, 0 ≤ e t)
(hfpos : ∀ t ∈ Set.Icc a b, 0 ≤ f t)
(hederiv : ∀ t ∈ Set.Ico a b, HasDerivAt e (de t) t)
(hineq : ∀ t ∈ Set.Ico a b, de t ≤ K * e t + f t)
(hinit : e a ≤ e₀)
(t : ℝ)
:
A nonnegative energy with a differential upper bound has the expected exponential control by its initial value and the total forcing.
theorem
ESS.vorticityEnergyGronwallDissipation
{a b K e₀ : ℝ}
{e de d f : ℝ → ℝ}
(hab : a ≤ b)
(hK : 0 ≤ K)
(hecont : ContinuousOn e (Set.Icc a b))
(hdecont : Continuous de)
(hdcont : Continuous d)
(hfcont : Continuous f)
(hepos : ∀ t ∈ Set.Icc a b, 0 ≤ e t)
(hdpos : ∀ t ∈ Set.Icc a b, 0 ≤ d t)
(hfpos : ∀ t ∈ Set.Icc a b, 0 ≤ f t)
(hederiv : ∀ t ∈ Set.Ico a b, HasDerivAt e (de t) t)
(hineq : ∀ t ∈ Set.Icc a b, de t + d t ≤ K * e t + f t)
(hinit : e a ≤ e₀)
:
The scalar differential energy inequality controls both the supremum of the energy and the time integral of a nonnegative dissipation term.