Actual gradient-supremum control of Euler Sobolev norms. The gradient norm is a constructed continuous path, its time integral controls H³, and the checked H³-tame estimate then propagates every higher order on the same time interval.
Sharp H³ products controlled by the actual velocity gradient. The only middle product is D²u D²u, handled by cubic testing.
The sharp middle-derivative interpolation needed by H³ Euler energy. Everything is an actual smooth L² field. Cubic testing and noncompact integration by parts prove the L⁴ inequality without a support or interpolation hypothesis.
Sharp H³ transport energy with the actual L-infinity norm of the velocity gradient. The pressure and undifferentiated transport cancel before the cubic-test interpolation estimate is used.
Gradient energy constant, given by 54*(∑ n ∈ range 4, (6 : ℝ)^n).
Equations
- EulerOrdinarySobolev.gradientEnergyConstant = 54 * ∑ n ∈ Finset.range 4, 6 ^ n
Instances For
Gradient norm path as an element of C(Icc (0 : ℝ) T,ℝ).
Equations
- U.gradientNormPath = { toFun := fun (t : ↑(Set.Icc 0 T)) => ‖EulerMeanSobolevBoundedField.finiteField (U.velocity t).derivative‖, continuous_toFun := ⋯ }
Instances For
Gradient integral, given by realIntegral T hT U.gradientNormPath t.
Equations
Instances For
Gradient H3 bound, given by Real.sqrt (wordEnergy 3 (U.velocity ⟨0,le_rfl,hT⟩)*Real.exp (gradientEnergyConstant*G)).
Equations
- U.gradientH3Bound G = √(EulerOrdinarySobolev.wordEnergy 3 (U.velocity ⟨0, ⋯⟩) * Real.exp (EulerOrdinarySobolev.gradientEnergyConstant * G))