在接口附近的声学点源的发射
Rong Zhou1, Beibei Li1, Liying Zhang1
1East China Normal University, State Key Laboratory of Precision Spectroscopy, Shanghai 200062, China.
Physical review letters
|August 12, 2025
概括
这项研究将光学点源理论扩展到声学,揭示了更丰富的远场模式和在接口附近的声波中出现新的极化现象. 它推进了对固体-流体边界的波相互作用的理解.
科学领域:
- 物理 物理学 物理
- 声学 声学 声学 声学
- 光学是什么?光学是什么?光学是什么?
背景情况:
- 点源辐射在波浪物理学中是基本的,光学理论已经确立,但声学对应物尚未发展.
- 需要一个统一的声学框架来理解在接口附近的波辐射.
研究的目的:
- 将光学点源框架扩展到固体流体接口的声学.
- 为了研究声波发射行为和极化现象.
主要方法:
- 开发了一个基于光学类比的理论声学框架.
- 分析了靠近固体流体界面的点源的远场模式和旋转角动量.
主要成果:
- 与光学相比,声学预测了更丰富的远场模式,包括多个峰值.
- 观察到超临界辐射对源深度的非单调依赖.
- 发现了深度依赖的横旋旋转角动量在漏水的雷利波中,不同的峰值有相反的方向.
结论:
- 扩展的声学框架为在接口附近的点源辐射提供了统一的洞察力.
- 结果揭示了声学近场,光学和声学之间的新两极化现象.
- 进步了对声学系统中波-物质相互作用的理解.
更多相关视频
相关概念视频
Echo
601
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,...
601
Atomic Emission Spectroscopy: Interference
274
In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...
274
Sound Intensity
4.2K
The loudness of a sound source is related to how energetically the source is vibrating, consequently making the molecules of the propagation medium vibrate. To measure the loudness of a source, the physical quantity of interest is the intensity. This is defined as the energy emitted per unit of time per unit of area perpendicular to the sound wave's propagation direction. Since the total energy is greater if the source vibrates for a longer duration and over a larger area, dividing the...
4.2K
Shock Waves
2.2K
While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...
2.2K
Sound Waves: Interference
3.9K
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...
3.9K
Interference: Path Lengths
1.4K
Consider two sources of sound, that may or may not be in phase, emitting waves at a single frequency, and consider the frequencies to be the same.
Two special sources may be considered when they are in phase. This can be easily achieved by feeding the two sources from the same source. An example would be synchronizing the two speakers by feeding them with the same source, such as the sound waves produced by a tuning fork. This setup ensures that the two sources have the same frequency and are...
Two special sources may be considered when they are in phase. This can be easily achieved by feeding the two sources from the same source. An example would be synchronizing the two speakers by feeding them with the same source, such as the sound waves produced by a tuning fork. This setup ensures that the two sources have the same frequency and are...
1.4K


