通过速度循环统计数据探索二维经典和量子流之间的等价性
Nicolás P Müller1,2, Giorgio Krstulovic1
1Université Côte d'Azur, Observatoire de la Côte d'Azur, CNRS, Laboratoire Lagrange, Boulevard de l'Observatoire CS 34229 - F 06304 NICE Cedex 4, France.
Physical review letters
|March 15, 2024
概括
我们使用模拟来比较量子和经典流. 量子流与反流和几乎不可压缩的直流相匹配,为它们的等价性建立了界限.
科学领域:
- 流体动力学 流体动力学
- 量子力学就是量子力学.
- 计算物理 计算物理
背景情况:
- 二维的流会呈现出明显的直接和反向的能量级联.
- 由Gross-Pitaevskii方程控制的量子流与经典流有相似之处.
- 了解速度循环的统计性质是描述流的关键.
研究的目的:
- 在二维经典和量子流中研究和比较速度循环的统计性质.
- 为了确定量子流在哪些条件下复制经典流的行为.
- 为了确定这两种类型的流之间的等价极限.
主要方法:
- 对于经典流的不压缩纳维埃-斯托克斯方程的数值模拟.
- 对于量子流的格罗斯-皮塔耶夫斯基方程的数值模拟.
- 对直接和反向级联的能量光谱和循环间歇性的分析.
主要成果:
- 格罗斯-皮塔耶夫斯基模拟显示了与二维经典流的双级联理论相一致的能量光谱.
- 量子流的逆级联中的循环间歇性与经典流中的循环间歇性相同.
- 对于循环的自相似缩放的等价性,对于几乎不可压缩的量子流,在直接级联中也是如此.
- 当压缩性变得显著时,与等效差异的偏差发生,近震产生量子.
结论:
- 量子流与经典流有很强的相似之处,特别是在反向流和几乎不可压缩的直接流中.
- 二维经典和量子流之间的等价性是有限的,并且在显著的可压缩性下分解.
- 本研究概述了古典和量子流之间的类比的条件和局限性.
相关概念视频
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
Poiseuille's Law and Reynolds Number
6.6K
Any fluid in a horizontal tube can flow due to pressure differences—fluid flows from high to low pressure. The flow rate (Q) is the ratio of pressure difference and resistance through a horizontal tube. The greater the pressure difference, the higher the flow rate. The flow resistance is expressed as:
6.6K
Steady, Laminar Flow in Circular Tubes
203
Hagen-Poiseuille flow describes a viscous fluid's steady, incompressible flow through a cylindrical tube with a constant radius R. This flow profile is often applied to understand fluid transport in narrow channels, such as capillaries. It serves as a foundational example of laminar flow. In this model, cylindrical coordinates (r,θ,z) are used to describe the radial (r), angular (θ), and axial (z) dimensions within the tube. For Hagen-Poiseuille flow, the velocity profile is...
203
Couette Flow
263
Couette flow represents the flow of fluid between two parallel plates, with one plate fixed and the other moving with a constant velocity. This configuration allows for a simplified analysis using the Navier-Stokes equations, which govern fluid motion under conditions of viscosity and incompressibility. For Couette flow, the assumptions include a steady, laminar, incompressible flow with a zero-pressure gradient in the flow direction. This flow type is beneficial for understanding shear-driven...
263
Velocity Potential
366
In steady, incompressible flow through a long, straight pipe with a uniform cross-section, the flow in the central region (far from the pipe walls) is irrotational. This irrotational nature means that fluid particles do not rotate around their axes, and a scalar function called the velocity potential, represented by ϕ, can be used to describe their movement. In irrotational flows, the velocity field V is defined as the gradient of the velocity potential:
366
Turbulent Flow
185
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...
185


