扭曲的线调整了纳维埃-斯托克斯流
Dhawal Buaria1,2, John M Lawson3, Michael Wilczek2,4
1Department of Mechanical Engineering, Texas Tech University, Lubbock, TX 79409, USA.
Science advances
|September 13, 2024
概括
研究人员发现了一种隐形的机制,可以防止流体动力学中的奇点. 线中的这种自我调节的反扭曲,通过分析不可压缩的纳维埃-斯托克斯方程 (INSE),即使没有粘度,也能确保平稳的流.
科学领域:
- 流体动力学和流动力学
- 数学物理学的数学物理.
- 非线性动力学是一种非线性动力学.
背景情况:
- 流体流的特点是线拓和动态.
- 由不可压缩的纳维埃-斯托克斯方程 (INSE) 描述的动荡,涉及线自我拉伸.
- 在流中INSE的规律性和奇点预防没有得到证实,通常归因于粘度.
研究的目的:
- 揭示流体流动力学中一个隐蔽的调节机制.
- 为了研究线自我拉伸如何防止没有粘度的奇点.
- 直接将旋动态与流统计数据联系起来.
主要方法:
- 从与旋转向量对齐的观察者的角度分析流动拓.
- 线自我拉伸和扭曲动态的数学研究.
- 隔离一个,以证明观察到的现象的通用性.
主要成果:
- 一个隐蔽的自我调节机制,称为"反扭曲",从自行拉伸的线中出现.
- 这种反扭曲自发地发展,以防止无限的旋转放大.
- 这种自我调节的反扭曲的通用性通过隔离一个旋来证明.
结论:
- 纳维尔-斯托克斯动力学可以通过固有的不透明的规范化机制来避免奇点的发展.
- 线动力学,特别是自我调节的反扭曲,在保持流规律性方面发挥着至关重要的作用.
- 粘度不仅仅是防止流流体流动中的奇点的原因.
相关概念视频
Navier–Stokes Equations
439
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
439
Laminar and Turbulent Flow
8.5K
Fluid dynamics is the study of fluids in motion. Velocity vectors are often used to illustrate fluid motion in applications like meteorology. For example, wind—the fluid motion of air in the atmosphere—can be represented by vectors indicating the speed and direction of the wind at any given point on a map. Another method for representing fluid motion is a streamline. A streamline represents the path of a small volume of fluid as it flows. When the flow pattern changes with time, the...
8.5K
Bernoulli's Equation for Flow Normal to a Streamline
811
Bernoulli's equation for flow normal to a streamline explains how pressure varies across curved streamlines due to the outward centrifugal forces induced by the fluid's curvature. The pressure is higher on the inner side of the curve, near the center of curvature, and decreases outward to balance these centrifugal forces.
The pressure difference depends on the fluid's velocity and radius of curvature. The pressure variation is minimal in flows with nearly straight streamlines.
The pressure difference depends on the fluid's velocity and radius of curvature. The pressure variation is minimal in flows with nearly straight streamlines.
811
Irrotational Flow
426
Irrotational flow is characterized by fluid motion where particles do not rotate around their axes, resulting in zero vorticity. For a flow to be irrotational, the curl of the velocity field must be zero. This imposes specific conditions on velocity gradients. For instance, to maintain zero rotation about the z-axis, the gradient condition:
426
Turbulent Flow
150
Turbulent flow is characterized by unpredictable fluctuations in velocity and pressure, which result in a chaotic fluid movement distinct from the orderly patterns of laminar flow. While laminar flow is governed by smooth, parallel layers with minimal mixing, turbulent flow exhibits highly irregular, three-dimensional patterns. This behavior arises due to instabilities in the fluid's velocity profile, and amplifies as the flow velocity increases. Minor disturbances, known as turbulent...
150
Bernoulli's Equation for Flow Along a Streamline
913
Bernoulli's equation relates the energy conservation in a fluid moving along a streamline. The equation applies to incompressible and inviscid fluids under steady flow. For such a flow, Newton's second law is applied to a small fluid element, which experiences forces due to pressure differences, gravity, and velocity variations. The force balance leads to the following form of Bernoulli's equation:
913


