Total raw-field provider for a positive history time #
Every admissible input is sent to the constructed history/forward solution. Its raw PDE, tangent constraint, parity, actual Field witnesses, true time derivative, pressure gradient and literal curl corrector are all exported.
The genuine cylinder forcing path is determined by its prescribed raw field.
The total high operator, backed by the unique genuine solution on admissible inputs.
Equations
- One or more equations did not get rendered due to their size.
Instances For
High vector field, given by (vectorField τ hτ hτT B (Classical.choice h)).congr (fun t x θ => by rw [highSolve_of_admissible τ hτ hτT B h]).
Equations
- EulerTransversePacketJoin.highVectorField τ hτ hτT B h = (EulerTransversePacketJoin.vectorField τ hτ hτT B (Classical.choice h)).congr ⋯
Instances For
High derivative field, given by vectorDerivativeField τ hτ hτT B (Classical.choice h).
Equations
- EulerTransversePacketJoin.highDerivativeField τ hτ hτT B h = EulerTransversePacketJoin.vectorDerivativeField τ hτ hτT B (Classical.choice h)
Instances For
High pressure gradient field, given by (scalarGradientField τ hτ hτT B (Classical.choice h)).congr (fun t x θ => by rw [highSolve_of_admissible τ hτ hτT B h]).
Equations
- EulerTransversePacketJoin.highPressureGradientField τ hτ hτT B h = (EulerTransversePacketJoin.scalarGradientField τ hτ hτT B (Classical.choice h)).congr ⋯
Instances For
High corrector field, bundling path, orbit, raw_eq.
Equations
- EulerTransversePacketJoin.highCorrectorField τ hτ hτT B h = { path := EulerTransversePacketJoin.correctorPath τ hτ hτT B (Classical.choice h), orbit := ⋯, raw_eq := ⋯ }
Instances For
High corrector derivative field, bundling path, orbit, raw_eq.
Equations
- EulerTransversePacketJoin.highCorrectorDerivativeField τ hτ hτT B h = { path := EulerTransversePacketJoin.correctorTimePath τ hτ hτT B (Classical.choice h), orbit := ⋯, raw_eq := ⋯ }