Weak–strong uniqueness at exponents (5,5) #
A finite-energy weak solution with pressure in space-time L⁵ and a
finite-energy weak solution in L^{10/3} satisfying the energy inequality,
with the same datum, agree almost everywhere on the slab. The proof is the
relative energy inequality followed by Gronwall's inequality; this is
lem:pv-serrin-uniqueness.
theorem
ESS.serrin_weak_strong_uniqueness
{T : ℝ}
{a : CKN.Foundation.Parabolic.Vec3 → CKN.Foundation.Parabolic.Vec3}
{u v : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3}
{Du Dv : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3}
{pu pv : CKN.Foundation.Parabolic.ParabolicPoint → ℝ}
(hU : IsSerrinWeakSolution T a u Du pu)
(hV : IsSerrinWeakSolution T a v Dv pv)
(hu5 :
MeasureTheory.MemLp u (ENNReal.ofReal 5) (MeasureTheory.volume.restrict (CKN.spaceTimeSet Set.univ (Set.Ioo 0 T))))
(hv103 :
MeasureTheory.MemLp v (ENNReal.ofReal (10 / 3))
(MeasureTheory.volume.restrict (CKN.spaceTimeSet Set.univ (Set.Ioo 0 T))))
(hvE :
∀ᵐ (t : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 T), ∫ (x : CKN.Foundation.Parabolic.Vec3), ∑ k : Fin 3, v (x, t) k * v (x, t) k ≤ (∫ (x : CKN.Foundation.Parabolic.Vec3), ∑ k : Fin 3, a x k * a x k) - 2 * ∫ (q : CKN.Foundation.Parabolic.ParabolicPoint) in CKN.spaceTimeSet Set.univ (Set.Ioo 0 t), ∑ k : Fin 3, ∑ j : Fin 3, Dv q k j * Dv q k j)
:
v =ᵐ[MeasureTheory.volume.restrict (CKN.spaceTimeSet Set.univ (Set.Ioo 0 T))] u
Weak–strong uniqueness for finite-energy weak solutions with pressures:
the first in space-time L⁵, the second in L^{10/3} with the energy
inequality.