在静电波场中围绕弹性散射器进行声
Khemraj Gautam Kshetri1, Nitesh Nama1
1Department of Mechanical & Materials Engineering, University of Nebraska-Lincoln, Lincoln, Nebraska 68588, USA.
Physical review. E
|November 18, 2023
概括
这项研究从数值上研究了声流体系统中的微粒子运动. 它确定了一个关键粒子大小,其中运动从流体流向声辐射力主导转移,受到频率和材料特性的影响.
科学领域:
- 声学流体学 声学流体学
- 微粒子操纵 微粒子操纵
- 计算物理 计算物理
背景情况:
- 声流流体系统利用声学散射器通过声相透来操纵微粒.
- 了解声流和辐射力之间的相互作用对于精确的控制至关重要.
研究的目的:
- 为了数值地调查声学散射器周围的时间平均流和辐射力场.
- 确定微粒子轨迹并确定运动主导的关键过渡大小.
- 分析声频,散射器材料和流体特性对微粒子行为的影响.
主要方法:
- 声流体系统的数值模拟.
- 计算时间平均流和辐射力场的计算.
- 基于模拟力场的微粒子轨迹分析.
- 参数研究不同颗粒大小,声频,散射器材料和流体特性.
主要成果:
- 确定了微粒子运动的关键过渡大小,从流向转向辐射力主导.
- 临界过渡尺寸随着声频的增加而减少.
- 增加的声学对比率和减少的动力粘度减少了关键过渡尺寸.
- 散射器材料和流体特性显著影响力场和临界过渡大小.
结论:
- 声频,散射器材料 (声差因子) 和流体粘度是控制微粒子操纵的关键参数.
- 这些发现为基于辐射力对声流体中小颗粒的操纵提供了设计策略.
- 优化这些参数允许使用声辐射力量有效操纵较小的粒子.
相关概念视频
Sound Waves: Interference
3.8K
Sound waves can be modeled either as longitudinal waves, wherein the molecules of the medium oscillate around an equilibrium position, or as pressure waves. When two identical waves from the same source superimpose on each other, the combination of two crests or two troughs results in amplitude reinforcement known as constructive interference. If two identical waves, that are initially in phase, become out of phase because of different path lengths, the combination of crests with troughs...
3.8K
Echo
514
The human ear cannot distinguish between two sources of sound if they happen to reach within a specific time interval, typically 0.1 seconds apart. More than this, and they are perceived as separate sources.
Imagine the sound is reflected back to the ears. Assuming that the source is very close to the human, the difference between hearing the two sounds—the emitted sound and the reflected sound—may be more than the minimum time for perceiving distinct sounds. If this is the case,...
Imagine the sound is reflected back to the ears. Assuming that the source is very close to the human, the difference between hearing the two sounds—the emitted sound and the reflected sound—may be more than the minimum time for perceiving distinct sounds. If this is the case,...
514
Standing Electromagnetic Waves
1.6K
Electromagnetic waves can be reflected; the surface of a conductor or a dielectric can act as a reflector. As electric and magnetic fields obey the superposition principle, so do electromagnetic waves. The superposition of an incident wave and a reflected electromagnetic wave produces a standing wave analogous to the standing waves created on a stretched string.
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
1.6K
Sound as Pressure Waves
2.4K
Sound waves, which are longitudinal waves, can be modeled as the displacement amplitude varying as a function of the spatial and temporal coordinates. As a column of the medium is displaced, its successive columns are also displaced. As the successive displacements differ relatively, a pressure difference with the surrounding pressure is created. The gauge pressure varies across the medium.
The pressure fluctuation depends on the difference in displacements between the successive points in the...
The pressure fluctuation depends on the difference in displacements between the successive points in the...
2.4K
Sound Waves
9.2K
Sound waves can be thought of as fluctuations in the pressure of a medium through which they propagate. Since the pressure also makes the medium's particles vibrate along its direction of motion, the waves can be modeled as the displacement of the medium's particles from their mean position.
Sound waves are longitudinal in most fluids because fluids cannot sustain any lateral pressure. In solids, however, shear forces help in propagating the disturbance in the lateral direction as well....
Sound waves are longitudinal in most fluids because fluids cannot sustain any lateral pressure. In solids, however, shear forces help in propagating the disturbance in the lateral direction as well....
9.2K
Standing Waves in a Cavity
936
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
936


