具有退化黏度系数的不可压缩轴对称欧拉方程的势奇异形成

T. Hou, D. Huang
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引用次数: 1

摘要

本文给出了具有退化黏度系数和有限能量光滑初始数据的不可压缩轴对称欧拉方程在原点处具有潜在的有限时间局部自相似奇点的强有力的数值证据。这个潜在奇点的一个重要特征是,解产生了一个向原点传播的双尺度行波。双尺度特征的标度特性是行波的中心位于围绕对称轴的半径为$O((T-t)^{1/2})$的环上,而环的厚度以$O(T-t)$的速率崩塌。这种潜在奇点的驱动机制是由于一个反对称涡旋偶极子在径向和轴向速度场中都产生了一个强剪切层。在没有进行粘性正则化的情况下,3 D欧拉方程在远场呈现出尖锐的锋面和一定程度的剪切不稳定性。另一方面,具有恒定黏度系数的Navier-Stokes方程使双尺度解结构正则化,并且对相同的初始数据不产生有限时间奇点。
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Potential Singularity Formation of Incompressible Axisymmetric Euler Equations with Degenerate Viscosity Coefficients
In this paper, we present strong numerical evidences that the incompressible axisymmetric Euler equations with degenerate viscosity coefficients and smooth initial data of finite energy develop a potential finite-time locally self-similar singularity at the origin. An important feature of this potential singularity is that the solution develops a two-scale traveling wave that travels towards the origin. The two-scale feature is characterized by the scaling property that the center of the traveling wave is located at a ring of radius $O((T-t)^{1/2})$ surrounding the symmetry axis while the thickness of the ring collapses at a rate $O(T-t)$. The driving mechanism for this potential singularity is due to an antisymmetric vortex dipole that generates a strong shearing layer in both the radial and axial velocity fields. Without the viscous regularization, the $3$D Euler equations develop a sharp front and some shearing instability in the far field. On the other hand, the Navier-Stokes equations with a constant viscosity coefficient regularize the two-scale solution structure and do not develop a finite-time singularity for the same initial data.
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