The canonical maximal solution in the reference's ordinary-function Sobolev class. All regularity is inherited from its existing shorter evolutions.
The canonical maximal fields in the challenge's position-first, real-time convention. Extension by zero outside the lifespan has no role in the equation.
The extended spatial suprema in the independent challenge agree with the ordinary development's bounded-function norms on every smooth Sobolev slice.
Maximal velocity extension, with branches according to ht : t ∈ Ico (0 : ℝ) L.duration.
Equations
- Euler.ComparatorBridge.maximalVelocityExtension L x t = if ht : t ∈ Set.Ico 0 L.duration then L.maximalVelocity ⟨t, ht⟩ x else 0
Instances For
Maximal pressure extension, with branches according to ht : t ∈ Ico (0 : ℝ) L.duration.
Equations
- Euler.ComparatorBridge.maximalPressureExtension L x t = if ht : t ∈ Set.Ico 0 L.duration then L.maximalPressure ⟨t, ht⟩ x else 0
Instances For
Maximal derivative field, given by eulerRhs (L.maximalField t) (L.maximalPressureField t).
Equations
Instances For
Maximal derivative extension, with branches according to ht : t ∈ Ico (0 : ℝ) L.duration.
Equations
- Euler.ComparatorBridge.maximalDerivativeExtension L x t = if ht : t ∈ Set.Ico 0 L.duration then (Euler.ComparatorBridge.maximalDerivativeField L ⟨t, ht⟩).field x else 0