Joint regularity of a classical solution up to time zero #
A classical solution is smooth on the closed half-space t ≥ 0. Its space-time derivative
(taken inside the half-space) is continuous up to t = 0, and its spatial gradient and time
derivative are the corresponding components of that joint derivative.
The closed half-space t ≥ 0.
Instances For
noncomputable def
AVenhance.Infra.Section5.RelativeError.classicalJointFDeriv
(θ : ℝ → Homogenization.Vec 2 → ℝ)
:
ℝ × Homogenization.Vec 2 → ℝ × Homogenization.Vec 2 →L[ℝ] ℝ
The joint derivative of a classical solution inside the closed half-space.
Equations
Instances For
theorem
AVenhance.Infra.Section5.RelativeError.classicalJointFDeriv_continuousOn
{θ : ℝ → Homogenization.Vec 2 → ℝ}
(hθ : ContDiffOn ℝ (↑⊤) (Function.uncurry θ) classicalHalfSpace)
:
theorem
AVenhance.Infra.Section5.RelativeError.classicalHasFDerivWithinAt
{θ : ℝ → Homogenization.Vec 2 → ℝ}
(hθ : ContDiffOn ℝ (↑⊤) (Function.uncurry θ) classicalHalfSpace)
{t : ℝ}
(ht : 0 ≤ t)
(x : Homogenization.Vec 2)
:
theorem
AVenhance.Infra.Section5.RelativeError.classical_spaceGrad_eq_joint
{θ : ℝ → Homogenization.Vec 2 → ℝ}
(hθ : ContDiffOn ℝ (↑⊤) (Function.uncurry θ) classicalHalfSpace)
{t : ℝ}
(ht : 0 ≤ t)
(x : Homogenization.Vec 2)
(i : Fin 2)
:
The spatial gradient of a classical solution is a component of the joint derivative.
theorem
AVenhance.Infra.Section5.RelativeError.classical_deriv_eq_joint
{θ : ℝ → Homogenization.Vec 2 → ℝ}
(hθ : ContDiffOn ℝ (↑⊤) (Function.uncurry θ) classicalHalfSpace)
{t : ℝ}
(ht : 0 < t)
(x : Homogenization.Vec 2)
:
HasDerivAt (fun (s : ℝ) => θ s x) ((classicalJointFDeriv θ (t, x)) (1, 0)) t
The time derivative of a classical solution is a component of the joint derivative.