Abstract:We prove global existence of smooth solutions for a slightly supercritical hyperdissipative Navier-Stokes under the optimal condition on the correction to the dissipation. This proves a conjecture formulated by Tao [Tao09].
From the generalized Fourier Navier-Stokes to the dyadic equationThis section contains one of the crucial steps in our approach. We show that the proof of Theorem 1.2 can be reduced to a proof of decay of solutions of a suitable
“…Let > 0. Assume that (1) and (2) are two solutions of (1.2) satisfying, ( ) ∈ ∞ ( 0, ; 1 ( ℝ 3 )) for = 1, 2, ( Λ ) ∇ (2) 3 ∈ 2 ( ℝ 3 × (0, ) ) .…”
Section: Uniquenessmentioning
confidence: 99%
“…Proof. Let (1) and (2) be the pressures associated with (1) and (2) , respectively. Then the differences̃= (1) − (2) and = (1) − (2) satisfy (3.1) Dotting (3.1) with̃and invoking the divergence-free conditions ∇ ⋅ (1) = 0 and ∇ ⋅̃= 0, we obtain We estimate 1 and write its terms explicitly,…”
Section: Uniquenessmentioning
confidence: 99%
“…More precisely, he shows that replacing by still leads to a unique global solution. Tao's result was later improved by to allow additional power in the logarithm, namely with . Efforts have also been devoted to the incompressible magnetohydrodynamic equations with hyperdissipation and the results are not completely parallel (see, e.g., ).…”
Section: Introductionmentioning
confidence: 99%
“…We remove some components of the hyperdissipation in (1.1). More precisely, we study the following 3D Navier-Stokes equations with fractional partial dissipation, 1 where the fractional partial dissipation operators Λ with > 0 and = 1, 2, 3 are defined via the Fourier transform Λ ( ) = | |̂( ).…”
The three‐dimensional incompressible Navier–Stokes equations with the hyperdissipation false(−normalΔfalse)γ always possess global smooth solutions when γ≥54. Tao [6] and Barbato, Morandin and Romito [1] made logarithmic reductions in the dissipation and still obtained the global regularity. This paper makes a different type of reduction in the dissipation and proves the global existence and uniqueness in the H1‐functional setting.
“…Let > 0. Assume that (1) and (2) are two solutions of (1.2) satisfying, ( ) ∈ ∞ ( 0, ; 1 ( ℝ 3 )) for = 1, 2, ( Λ ) ∇ (2) 3 ∈ 2 ( ℝ 3 × (0, ) ) .…”
Section: Uniquenessmentioning
confidence: 99%
“…Proof. Let (1) and (2) be the pressures associated with (1) and (2) , respectively. Then the differences̃= (1) − (2) and = (1) − (2) satisfy (3.1) Dotting (3.1) with̃and invoking the divergence-free conditions ∇ ⋅ (1) = 0 and ∇ ⋅̃= 0, we obtain We estimate 1 and write its terms explicitly,…”
Section: Uniquenessmentioning
confidence: 99%
“…More precisely, he shows that replacing by still leads to a unique global solution. Tao's result was later improved by to allow additional power in the logarithm, namely with . Efforts have also been devoted to the incompressible magnetohydrodynamic equations with hyperdissipation and the results are not completely parallel (see, e.g., ).…”
Section: Introductionmentioning
confidence: 99%
“…We remove some components of the hyperdissipation in (1.1). More precisely, we study the following 3D Navier-Stokes equations with fractional partial dissipation, 1 where the fractional partial dissipation operators Λ with > 0 and = 1, 2, 3 are defined via the Fourier transform Λ ( ) = | |̂( ).…”
The three‐dimensional incompressible Navier–Stokes equations with the hyperdissipation false(−normalΔfalse)γ always possess global smooth solutions when γ≥54. Tao [6] and Barbato, Morandin and Romito [1] made logarithmic reductions in the dissipation and still obtained the global regularity. This paper makes a different type of reduction in the dissipation and proves the global existence and uniqueness in the H1‐functional setting.
“…and which is conserved in time for solutions of (NLW). When F is given by (1), one has G(u) ≈ u 4 log(3 + u 2 ), while when F is of power-type |u| p u, G(u) = 1 p+2 |u| p+2 . In recent years, beginning with work of Tao [29], several authors have studied the global well-posedness and scattering problem for various cases of the threedimensional nonlinear wave equation with slightly energy-supercritical nonlinearity, obtaining striking results which show that the global well-posedness theory can be extended from the energy-subcritical and energy-critical settings into the slightly energy-supercritical regime (that is, admitting the inclusion of logarithmic factors).…”
We establish global well-posedness and scattering results for the logarithmically energy-supercritical nonlinear wave equation, under the assumption that the initial data satisfies a partial symmetry condition. These results generalize and extend work of Tao in the radially symmetric setting. The techniques involved include weighted versions of Morawetz and Strichartz estimates, with weights adapted to the partial symmetry assumptions.In an appendix, we establish a corresponding quantitative result for the energy-critical problem.
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