在极端一维的汉堡流中三元相的对齐
Bartosz Protas1, Di Kang1, Miguel D Bustamante2
1Department of Mathematics and Statistics, <a href="https://ror.org/02fa3aq29">McMaster University</a>, Hamilton, Ontario, Canada, L8S 4L8.
Physical review. E
|June 22, 2024
概括
汉堡流中的非线性模态相互作用显示了相对齐,最大限度地将能量转移到较小的尺度上. 一些关键的相互作用主导着这种能量流,这表明了流体动力学的缩小模型.
科学领域:
- 流体动力学 流体动力学
- 非线性动力学是一种非线性动力学.
- 计算物理 计算物理
背景情况:
- 汉堡流作为欧勒和纳维埃-斯托克斯方程的简化模型,对于理解流体动力学至关重要.
- 非线性模态相互作用,特别是三元相互作用,控制流体系统中跨尺度的能量转移.
- 了解这些相互作用中的相位对齐是预测能量流和系统行为的关键.
研究的目的:
- 分析无和粘性Burgers流中的非线性模态相互作用的细结构.
- 在三元相互作用中研究福里埃模式的偏好相位对齐.
- 开发诊断工具,探测三元相互作用的连贯性及其对能量流的影响.
主要方法:
- 分析1D无粘性和粘性汉堡流,具有各种初始条件 (单模,极端,通用).
- 开发和应用诊断工具来量化三元相互作用中的连贯性.
- 确定主导三合体,负责不同波数的能量流.
主要成果:
- 涉及含有能量的里叶模式的三合体始终对齐相位,以最大限度地使能量流向小尺度.
- 一个普遍的统计分布显示,少数三合体实现了大部分的能量流.
- 主导三合体包括局部和非局部相互作用的混合物,随着时间的推移,非局部相互作用变得越来越重要.
结论:
- 结果表明,有可能构建具有较少自由度的 Burgers 流动的减少模式表示.
- 在初始数据中随机化空间连贯性不会显著改变三元交互动态或能量流.
- 这些发现提供了关于乱和混乱系统中能量转移的基本机制的见解.
更多相关视频
11:00Experimental Investigation of Secondary Flow Structures Downstream of a Model Type IV Stent Failure in a 180° Curved Artery Test Section
Published on: July 19, 2016
11.6K
09:17Experimental Investigation of the Flow Structure over a Delta Wing Via Flow Visualization Methods
Published on: April 23, 2018
10.7K
相关概念视频
Steady, Laminar Flow Between Parallel Plates
172
Understanding steady, laminar flow between parallel plates is essential for analyzing and designing flow in narrow rectangular channels, commonly found in various water conveyance and drainage systems. The Navier-Stokes equations govern fluid motion and are generally challenging to solve due to their nonlinearity. However, simplifications are possible in certain cases, like the steady laminar flow between parallel plates. For this scenario, we assume steady, incompressible, laminar flow.
172
Irrotational Flow
443
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:
443
Couette Flow
244
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...
244
Steady, Laminar Flow in Circular Tubes
186
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...
186
Turbulent Flow
167
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...
167
Unsymmetric Bending - Angle of Neutral Axis
297
Unsymmetrical bending occurs when a structural member is subjected to bending moments in a plane that does not align with the member's principal axes. This scenario typically arises in beams and other structural components when loads are applied at non-ideal angles, introducing complexities in stress analysis.
When a bending moment is applied at an angle θ concerning the vertical axis of a symmetrical member, it can be resolved into components along the member's principal...
When a bending moment is applied at an angle θ concerning the vertical axis of a symmetrical member, it can be resolved into components along the member's principal...
297
