OAI/MathematicalPhysics/NavierStokes/ForcedComputation/Scalar/PlaneFluid.lean
7 declarations, 0 contain sorry, 0 declared as axioms
The whole-plane scalar produces an actual Navier–Stokes velocity. The force is prescribed from the drift and source, before solving for w.
- theorem
OAI.ForcedComputation.VelocityDetector.GlobalPlaneScalarSolution.hasDerivWithinAtline 15 - theorem
OAI.ForcedComputation.VelocityDetector.GlobalPlaneScalarSolution.initialTimeDerivativeline 27 - theorem
OAI.ForcedComputation.VelocityDetector.triangularVelocity_plane_equationline 43 - theorem
OAI.ForcedComputation.VelocityDetector.triangularVelocity_plane_divergenceline 59 - theorem
OAI.ForcedComputation.VelocityDetector.triangularVelocity_plane_initialline 72 - theorem
OAI.ForcedComputation.VelocityDetector.triangularVelocity_thirdline 79 - theorem
OAI.ForcedComputation.VelocityDetector.triangularVelocity_halfPlane_integralline 85Source documentation
Normalized integration over the period-one coordinate gives exactly the scalar half-plane observation used in the construction.
theorem triangularVelocity_halfPlane_integral (a : ℝ → Plane → Plane) (w : ℝ → Plane → ℝ) (t : ℝ) : (∫ X in ExpandingDetector.upperHalfPlane, ∫ z in Icc (0 : ℝ) 1, triangularVelocity a w (t, atHeight X z) 2) = ∫ X in ExpandingDetector.upperHalfPlane, w t X := by …Mentions: OAI.ForcedComputation.ExpandingDetector.upperHalfPlane, OAI.ForcedComputation.VelocityDetector.triangularVelocity