OAI/MathematicalPhysics/NavierStokes/ForcedComputation/Scalar/PlaneScalarMildSourceRegularity.lean
9 declarations, 0 contain sorry, 0 declared as axioms
Compatibility and spatial regularity of the effective heat source.
- theorem
OAI.ForcedComputation.PlaneScalarMild.directionalPath_truncateline 13 - theorem
OAI.ForcedComputation.PlaneScalarMild.map_add_add_sumline 22 - theorem
OAI.ForcedComputation.PlaneScalarMild.CompatibleData.product_solution_truncateline 30 - theorem
OAI.ForcedComputation.PlaneScalarMild.CompatibleData.directional_product_truncateline 37 - theorem
OAI.ForcedComputation.PlaneScalarMild.CompatibleData.effectiveSource_truncateline 48Source documentation
The effective source represents the same function at every jet order.
theorem effectiveSource_truncate {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν) (D : CompatibleData T) (k n : ℕ) (hkn : k ≤ n) : truncatePath k n hkn T (D.effectiveSource hT hν n) = D.effectiveSource hT hν k := by …Mentions: OAI.ForcedComputation.PlaneScalarMild.CompatibleData, OAI.ForcedComputation.PlaneScalarMild.truncatePath
- def
OAI.ForcedComputation.PlaneScalarMild.CompatibleData.effectiveSourceValueline 62Source documentation
The common scalar effective source.
def effectiveSourceValue {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν) (D : CompatibleData T) (t : Icc (0 : ℝ) T) (x : Plane) : ℝ := …Mentions: OAI.ForcedComputation.PlaneScalarMild.CompatibleData
- theorem
OAI.ForcedComputation.PlaneScalarMild.CompatibleData.effectiveSourceValue_eqline 66 - theorem
OAI.ForcedComputation.PlaneScalarMild.CompatibleData.effectiveSource_smoothline 80Source documentation
The effective source has smooth spatial slices, obtained from the compatible finite jets.
theorem effectiveSource_smooth {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν) (D : CompatibleData T) (t : Icc (0 : ℝ) T) : ContDiff ℝ ∞ (D.effectiveSourceValue hT hν t) := by …Mentions: OAI.ForcedComputation.PlaneScalarMild.CompatibleData
- theorem
OAI.ForcedComputation.PlaneScalarMild.CompatibleData.effectiveSource_spatial_continuousline 93Source documentation
Every spatial derivative of the effective source varies jointly continuously.
theorem effectiveSource_spatial_continuous {T ν : ℝ} (hT : 0 ≤ T) (hν : 0 < ν) (D : CompatibleData T) (k : ℕ) : Continuous (fun p : Icc (0 : ℝ) T × Plane => iteratedFDeriv ℝ k (D.effectiveSourceValue hT hν p.1) p.2) := by …Mentions: OAI.ForcedComputation.PlaneScalarMild.CompatibleData