Heat operator of the short-time cutoff field #
The specified weak heat vector separates into the scaled equation and the
first and second derivatives of the smooth cutoff in lem:bu-small-time.
noncomputable def
ESS.buCutHeatError
(κ : CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ)
(v : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dv : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(z : CKN.Foundation.Parabolic.ParabolicPoint)
:
The cutoff derivative terms in the weak heat equation.
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
ESS.buCutHeat_eq
(κ : CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ)
(v : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dv : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(D2v : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(Dtv : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(z : CKN.Foundation.Parabolic.ParabolicPoint)
:
ucWeakHeatVector (buCutD2 κ v Dv D2v) (buCutDt κ v Dtv) z = buCutScalar κ z • ucWeakHeatVector D2v Dtv z + buCutHeatError κ v Dv z
The weak heat vector of the cutoff field is the scalar cutoff times the original weak heat vector plus the cutoff derivative error.