Potentially Singular Behavior of the 3D Navier–Stokes Equations
Potentially Singular Behavior of the 3D Navier–Stokes Equations
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DOI:
10.1007/s10208-022-09578-4
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发表时间:
2021-07
影响因子:
3
通讯作者:
T. Hou
中科院分区:
文献类型:
--
作者:
T. Hou
Whether the 3D incompressible Navier–Stokes equations can develop a finite time singularity from smooth initial data is one of the most challenging problems in nonlinear PDEs. In this paper, we present some new numerical evidence that the incompressible axisymmetric Navier–Stokes equations with smooth initial data of finite energy seem to develop potentially singular behavior at the origin. This potentially singular behavior is induced by a potential finite time singularity of the 3D Euler equations that we reported in a companion paper published in the same issue, see also Hou (Potential singularity of the 3D Euler equations in the interior domain. arXiv:2107.05870 [math.AP], 2021). We present numerical evidence that the 3D Navier–Stokes equations develop nearly self-similar singular scaling properties with maximum vorticity increased by a factor of. We have applied several blow-up criteria to study the potentially singular behavior of the Navier–Stokes equations. The Beale–Kato–Majda blow-up criterion and the blow-up criteria based on the growth of enstrophy and negative pressure seem to imply that the Navier–Stokes equations using our initial data develop a potential finite time singularity. We have also examined the Ladyzhenskaya–Prodi–Serrin regularity criteria (Kiselev and Ladyzhenskaya in Izv Akad Nauk SSSR Ser Mat 21(5):655–690, 1957; Prodi in Ann Math Pura Appl 4(48):173–182, 1959; Serrin in Arch Ration Mech Anal 9:187–191, 1962) that are based on the growth rate ofnorm of the velocity with. Our numerical results for the cases ofandprovide strong evidence for the potentially singular behavior of the Navier–Stokes equations. The critical case ofis more difficult to verify numerically due to the extremely slow growth rate in thenorm of the velocity field and the significant contribution from the far field where we have a relatively coarse grid. Our numerical study shows that while the globalnorm of the velocity grows very slowly, the localized version of thenorm of the velocity experiences rapid dynamic growth relative to the localizednorm of the initial velocity. This provides further evidence for the potentially singular behavior of the Navier–Stokes equations.