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Journal articles on the topic 'Sound-waves'

Author: Grafiati

Published: 4 June 2021

Last updated: 25 July 2025

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1

Hults, Morris G. "Sound waves." Physics Teacher 39, no. 6 (2001): 377. http://dx.doi.org/10.1119/1.1531955.

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2

Wolf, Franz Josef. "Sound absorber for sound waves." Journal of the Acoustical Society of America 111, no. 6 (2002): 2535. http://dx.doi.org/10.1121/1.1492935.

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3

Dunkel, Jörn. "Rolling sound waves." Nature Materials 17, no. 9 (2018): 759–60. http://dx.doi.org/10.1038/s41563-018-0155-9.

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4

Jones, Willie. "Sound waves for brain waves - [update]." IEEE Spectrum 46, no. 1 (2009): 16–17. http://dx.doi.org/10.1109/mspec.2009.4734300.

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5

Kenyon, Kern E. "Momentum of sound waves." Physics Essays 21, no. 1 (2008): 68–69. http://dx.doi.org/10.4006/1.3000091.

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6

Eisenstein, Daniel J., and Charles L. Bennett. "Cosmic sound waves rule." Physics Today 61, no. 4 (2008): 44–50. http://dx.doi.org/10.1063/1.2911177.

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7

Swinbanks, Malcolm A. "Attenuation of sound waves." Journal of the Acoustical Society of America 80, no. 4 (1986): 1281. http://dx.doi.org/10.1121/1.394459.

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8

Swinbanks, Malcolm A. "Attenuation of sound waves." Journal of the Acoustical Society of America 81, no. 5 (1987): 1655. http://dx.doi.org/10.1121/1.395061.

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9

Ashley, Steven. "Sound Waves At Work." Mechanical Engineering 120, no. 03 (1998): 80–84. http://dx.doi.org/10.1115/1.1998-mar-2.

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Researchers have devised a new technique to use sound waves, opening the way for simple acoustic compressors, speedy chemical-process reactors, and clean electric-power generators. MacroSonix Corp. in Richmond, Vermont, has developed a technique by which standing sound waves resonating in specially shaped closed cavities can be loaded with thousands of times more energy than was previously possible. Company’s wave-shaping technology is known as resonant macrosonic synthesis (RMS). With some clever engineering, he said, the elevated acoustic-energy levels produced using RMS can be tapped for a

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10

Kann, K. B. "Sound waves in foams." Colloids and Surfaces A: Physicochemical and Engineering Aspects 263, no. 1-3 (2005): 315–19. http://dx.doi.org/10.1016/j.colsurfa.2005.04.010.

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11

Birkhoff, Garrett. "Sound waves in fluids." Applied Numerical Mathematics 3, no. 1-2 (1987): 3–24. http://dx.doi.org/10.1016/0168-9274(87)90003-1.

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12

Buckingham, Michael J. "Sound waves and shear waves in sediments." Journal of the Acoustical Society of America 119, no. 5 (2006): 3275. http://dx.doi.org/10.1121/1.4808893.

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13

Kim, Joo Yeol, Hyo-Jun Lee, Jin A. Kim, and Mi-Jeong Jeong. "Sound Waves Promote Arabidopsis thaliana Root Growth by Regulating Root Phytohormone Content." International Journal of Molecular Sciences 22, no. 11 (2021): 5739. http://dx.doi.org/10.3390/ijms22115739.

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Sound waves affect plants at the biochemical, physical, and genetic levels. However, the mechanisms by which plants respond to sound waves are largely unknown. Therefore, the aim of this study was to examine the effect of sound waves on Arabidopsis thaliana growth. The results of the study showed that Arabidopsis seeds exposed to sound waves (100 and 100 + 9k Hz) for 15 h per day for 3 day had significantly longer root growth than that in the control group. The root length and cell number in the root apical meristem were significantly affected by sound waves. Furthermore, genes involved in cel

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14

MKRTCHYAN, A. R., A. G. HAYRAPETYAN, B. V. KHACHATRYAN, and R. G. PETROSYAN. "TRANSFORMATION OF SOUND AND ELECTROMAGNETIC WAVES IN NON-STATIONARY MEDIA." Modern Physics Letters B 24, no. 18 (2010): 1951–61. http://dx.doi.org/10.1142/s021798491002433x.

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Transformation (reflection and transmission) of sound and electromagnetic waves are considered in non-stationary media, properties of which abruptly change in time. Reflection and transmission coefficients for both amplitudes and intensities of sound and electromagnetic waves are obtained. Quantitative relations between the reflection and transmission coefficients for both sound and electromagnetic waves are given. The sum of the energy flux reflection and transmission coefficients for both types of waves is not equal to one (for sound waves it is greater than one). The energy of both waves is

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15

Gingold, Harry, Jianming She, and William E. Zorumski. "Reflection of sound waves by sound‐speed inhomogeneities." Journal of the Acoustical Society of America 91, no. 3 (1992): 1262–69. http://dx.doi.org/10.1121/1.402509.

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16

Mawarni, L., R. R. Lahay, and A. Fajari. "The timing of sonic bloom application on cabbage (Brassica oleraceae) for foliar fertilizer effectiveness." IOP Conference Series: Earth and Environmental Science 977, no. 1 (2022): 012024. http://dx.doi.org/10.1088/1755-1315/977/1/012024.

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Abstract Sonic bloom was a technology that used sound waves at 07.00–11.00 a.m. in the western part of Indonesia with a particular frequency to stimulate plant growth. This study aims to determine the effectiveness and best time for applying the foliar fertilizer with sound waves to cabbage plants. This research was conducted in Kuta Gugung Village, Naman Teran District, Karo Regency, from September 1st, 2020, to December 9th, 2020. The research method was a non-factorial randomized block design with four treatments and five replications, namely: application sound waves without fertilization (

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17

Schmitz, Kai. "LISA Sensitivity to Gravitational Waves from Sound Waves." Symmetry 12, no. 9 (2020): 1477. http://dx.doi.org/10.3390/sym12091477.

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Gravitational waves (GWs) produced by sound waves in the primordial plasma during a strong first-order phase transition in the early Universe are going to be a main target of the upcoming Laser Interferometer Space Antenna (LISA) experiment. In this short note, I draw a global picture of LISA’s expected sensitivity to this type of GW signal, based on the concept of peak-integrated sensitivity curves (PISCs) recently introduced in two previous papers. In particular, I use LISA’s PISC to perform a systematic comparison of several thousands of benchmark points in ten different particle physics mo

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18

Berntsen, Jarle, Jacqueline Naze Tjo/tta, and Sigve Tjo/tta. "Interaction of sound waves. Part IV: Scattering of sound by sound." Journal of the Acoustical Society of America 86, no. 5 (1989): 1968–83. http://dx.doi.org/10.1121/1.398576.

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19

Pozinkevych, Ruslan. "“Presenting of Sound and Non-Sound Waves Signal Analysis “." ECS Meeting Abstracts MA2022-01, no. 32 (2022): 2392. http://dx.doi.org/10.1149/ma2022-01322392mtgabs.

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Our research is an attempt to derive mathematical formula to describe the state of a system created by to or more waves resulting in a shockwave production The shockwave produced is a carrier of an energy that can be used for motion in gases and liquids To be able to utilize this energy we must be able to describe the state of a system of two or more waves at any given time thus deriving a formula that links energy produced to the component characteristics of the wave e.g frequency amplitude etc A mathematical model is used which presents a system of waves as a sum or difference of two vectors

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20

Mulyaningsih, Rejeki Sri. "Effect of Amplitude and Frequency on the Speed of Sound Waves in Air and Water Using PhET Simulation." Jurnal Pendidikan dan Ilmu Fisika 4, no. 1 (2024): 40. http://dx.doi.org/10.52434/jpif.v4i1.3501.

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Sound waves can occur not only in solid medium but also in air and water mediums. The effect of amplitude and frequency on the speed of sound waves differs between air and water mediums. The speed of sound waves cannot be seen with the naked eye. A virtual lab is needed to determine the speed of sound wave propagation. The purpose of this study is to determine the effect of amplitude and frequency on the speed of sound waves in air and water medium. The research method used is a quantitative method by conducting experiments online using the PhET application. PhET is used because it can carry o

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21

Ikezaki, Yoto, Yuting Geng, Masato Nakayama, and Takanobu Nishiura. "Demodulated sound enhancement based on virtual multi-boosted amplitude modulation with parametric array loudspeaker." INTER-NOISE and NOISE-CON Congress and Conference Proceedings 268, no. 6 (2023): 2477–87. http://dx.doi.org/10.3397/in_2023_0362.

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A parametric array loudspeaker can achieve sharp directivity in the audible band by utilizing ultrasounds. Ultrasounds are emitted intensely from the parametric array loudspeaker and the difference frequency component self-demodulates due to the nonlinear interactions in the air. Therefore, the sound pressure of the audible sound reproduced by the parametric array loudspeaker is lower than that reproduced by the conventional electro-dynamic loudspeaker. This makes it difficult to use the parametric loudspeaker in a noisy environment. To solve this problem, we modify conventional modulations to

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22

Jitendra, Sunte. "Control of speak and talk of Human body in Physiology." Journal of Advances in Experimental Therapeutics and Neurotherapeutics 3, no. 1 (2025): 21–23. https://doi.org/10.5281/zenodo.14650654.

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<em>In playing guitar and many more musical instruments, one can sound a particular range of frequencies at the required amplitude of sound waves. Man, also says some tune of sound at the required level of sound amplitude and frequencies. Here one can make a difference in sound playing and speaking, talking of sound waves or sound words. In this paper, one can make and control sound waves irrespective of any environment, like in court, in a hall, or on any other platform. So, people can’t determine the truthiness of a person while judging; it is also different to give justice of hearing.

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23

Uberoi, C. "Interaction of Flux Tubes with Sound Waves." Symposium - International Astronomical Union 142 (1990): 239–43. http://dx.doi.org/10.1017/s0074180900088008.

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The Landau damping of sound waves in a plasma consisting of ensemble of magnetic flux tubes is discussed. It is shown that sound waves cannot be Landau damped in general but under certain restricted conditions on plasma parameters the possibility of absorption of these waves can exist. The possibility of radiative damping of the acoustic waves along the magnetic filaments is also discussed. It appears that the most plausible mechanism of damping of sound waves in a plasma consisting of magnetic filaments can be due to scattering of a sound wave by the filaments.

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24

Li, Fangfang, Han Cao, Yinghui Jia, Yu Guo, and Jun Qiu. "Interaction between Strong Sound Waves and Aerosol Droplets: Numerical Simulation." Water 14, no. 10 (2022): 1661. http://dx.doi.org/10.3390/w14101661.

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In this study, we attempted to eliminate atmospheric fog and aerosol particles by strong sound waves. The action of sound waves created an air disturbance, and the oscillation of the local air caused the micron-sized aerosol droplet particles to move. To provide guidance of the characteristics of the effective sound waves, this study numerically simulated aerosol droplet agglomeration under the action of sound waves, which was solved by coupling computational fluid dynamics (CFD) and discrete element methods (DEMs) as a typical two-phase flow problem in this study. The movements of aerosol dro

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25

Ogawa, Yuya, Ayumu Osumi, and Youichi Ito. "Basic investigation of sound field inside and outside ear canal under ultrasound irradiation." INTER-NOISE and NOISE-CON Congress and Conference Proceedings 265, no. 4 (2023): 3858–63. http://dx.doi.org/10.3397/in_2022_0547.

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In recent years, high-intensity airborne ultrasonic waves applied technology has been developed actively. Accordingly, there are concerns about the effects of sound wave exposure by high-intensity airborne ultrasonic waves. The sound wave intensity is different near the entrance of the ear canal and near the eardrum, because the wavelength is short in the ultrasonic region. Therefore, it is necessary to know accurately the sound pressure at the eardrum position in considering the effects of sound waves exposure by ultrasonic waves. However, it is difficult to measure sound pressure near the ea

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26

Shindo, Tomohiko, and Hiroaki Shimokawa. "Therapeutic Angiogenesis with Sound Waves." Annals of Vascular Diseases 13, no. 2 (2020): 116–25. http://dx.doi.org/10.3400/avd.ra.20-00010.

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27

Ho, Ai Phi Thuy. "The Beauty of Sound Waves." POCUS Journal 7, no. 1 (2022): 179. http://dx.doi.org/10.24908/pocus.v7i1.15314.

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28

Binh, Nguyen Dang. "Gestures Recognition from Sound Waves." EAI Endorsed Transactions on Context-aware Systems and Applications 3, no. 10 (2016): 151679. http://dx.doi.org/10.4108/eai.12-9-2016.151679.

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29

Wilk, Grzegorz, and Zbigniew Włodarczyk. "Sound waves in hadronic matter." EPJ Web of Conferences 172 (2018): 01002. http://dx.doi.org/10.1051/epjconf/201817201002.

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We argue that recent high energy CERN LHC experiments on transverse momenta distributions of produced particles provide us new, so far unnoticed and not fully appreciated, information on the underlying production processes. To this end we concentrate on the small (but persistent) log-periodic oscillations decorating the observed pT spectra and visible in the measured ratios R = σdata(pT) / σfit (pT). Because such spectra are described by quasi-power-like formulas characterised by two parameters: the power index n and scale parameter T (usually identified with temperature T), the observed logpe

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30

Kielpinski, Dave. "Quantum sound waves stick together." Nature 527, no. 7576 (2015): 45–46. http://dx.doi.org/10.1038/527045a.

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31

Aygün, Müge, and Funda Aydın-Güç. "Superposition of sound waves: beats." Physics Education 54, no. 4 (2019): 043007. http://dx.doi.org/10.1088/1361-6552/ab1cf5.

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32

Schewe, Philip F. "Helium crystallization with sound waves." Physics Today 54, no. 7 (2001): 9. http://dx.doi.org/10.1063/1.2405647.

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33

White, J. E. "Underground sound: Applied seismic waves." Journal of the Acoustical Society of America 89, no. 4B (1991): 1900. http://dx.doi.org/10.1121/1.2029438.

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34

Nuwer, Rachel. "Wireless Charging with Sound Waves." Scientific American 311, no. 6 (2014): 52. http://dx.doi.org/10.1038/scientificamerican1214-52b.

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35

Joshi, Amey S. "Sound waves in polarized fluids." Physics of Fluids 31, no. 7 (2019): 076105. http://dx.doi.org/10.1063/1.5096369.

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36

Riordan, James R. "Sound waves make filters finer." Physics Today 55, no. 1 (2002): 9. http://dx.doi.org/10.1063/1.4796515.

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37

Serdobolskaya, O. Yu, and G. P. Morozova. "Sound waves in polydomain ferroelectrics." Ferroelectrics 208-209, no. 1 (1998): 395–412. http://dx.doi.org/10.1080/00150199808014889.

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38

Suzuki, Yasuhiro. "Artificial Chemistry by Sound Waves." Proceedings of International Conference on Artificial Life and Robotics 22 (January 19, 2017): 599–602. http://dx.doi.org/10.5954/icarob.2017.os17-3.

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39

Khodusov, V. D., and A. S. Naumovets. "Second sound waves in diamond." Diamond and Related Materials 21 (January 2012): 92–98. http://dx.doi.org/10.1016/j.diamond.2011.10.005.

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40

Ratkiewicz, R., D. E. Innes, and J. F. McKenzie. "Characteristics and Riemann invariants for multi-ion plasmas in the presence of Alfvén waves." Journal of Plasma Physics 52, no. 2 (1994): 297–307. http://dx.doi.org/10.1017/s0022377800017918.

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In this paper the characteristics for a single- and a bi-ion plasma in the presence of Alfvén waves are given. In the single-ion case, the analysis is extended to the situation where Alfvén waves saturate and dissipatively heat the plasma. When there is no dissipation, there are three sound waves and one entropy wave in the single-ion plasma. Each sound wave is associated with two Riemann invariants relating the changes in density and wave pressure to changes in the flow. In the case when the Alfvén waves saturate and heat the plasma, there are two sound waves and one modified entropy sound wa

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41

Machorro, Roberto, and E. C. Samano. "How Does It Sound? Young Interferometry Using Sound Waves." Physics Teacher 46, no. 7 (2008): 410–12. http://dx.doi.org/10.1119/1.2981287.

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42

Zhang, Yun, and De Ge. "Researching Characteristics of the Interaction between Sound Waves and Water Layers with Different Thickness." Journal of Physics: Conference Series 2468, no. 1 (2023): 012165. http://dx.doi.org/10.1088/1742-6596/2468/1/012165.

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Abstract Effects of water layers of different thickness and different frequencies of sound for sound transmission intensity have been analyzed by calculations of sound waves propagating in air and water layer. The results have showed that, when water layer thickness is less than 5mm, the changes of thickness have a powerful effect on sound waves, while it is more than 5mm, there is nearly no effect with different thickness, however, frequency of sound waves play a decisive role, especially when the sound wave frequency is less than 100Hz.

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43

Anggelia, Shilvy, Rahmawati Rahmawati, Adinda Setiawati, and Wahyu Kurniawati. "Diving into the World of Sound and Light, Understanding Their Properties, Propagation and Uses." Jurnal Pendidikan Indonesia 3, no. 01 (2025): 10–16. https://doi.org/10.58471/ju-pendi.v3i01.405.

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The aim of this research is to introduce students to the basic concepts of sound and light during science learning. This abstract discusses the properties of sound, such as its source, propagation, and how the human ear receives sound. Apart from that, this abstract also discusses light as an energy source that allows us to see objects around us, including how the eye propagates and receives light. Once students understand these concepts, it is hoped that they will be able to understand between sound and light.Sound waves can modulate the amplitude and phase of light, bending it, focusing it,

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44

Jagtap, Harshal, and Uday Wankhede. "Experimental investigations of effect of sound waves on oscillation and startup characteristics of oscillating heat pipe at different orientations." Thermal Science 21, no. 6 Part A (2017): 2587–97. http://dx.doi.org/10.2298/tsci150804142j.

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This research deals with the effects of working fluid and use of sound waves on the startup and heat transfer characteristics in terms of thermal resistance of a closed loop oscillating heat pipe. The performance of the oscillating heat pipe is checked for different orientations as 90? (vertical position), 60?, and 30?. Initially water is used as working fluid and performance of the oscillating heat pipe is checked with and without sound waves. Then 0.1 wt.% Al2O3-water nanofluid is utilized as working fluid in oscillating heat pipe and its performance is analyzed with and without sound waves.

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45

Pushkina, N. I. "Nonlinear wave interactions on the surface of superfluid helium." Soviet Journal of Low Temperature Physics 13, no. 7 (1987): 389–92. https://doi.org/10.1063/10.0031732.

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The linear reflection of second sound from the surface of superfluid 4He bounded by vacuum is investigated with allowance for surface excitations. The results are used to analyze two nonlinear problems. The first nonlinear problem is the phase conjugation of second sound by the surface of superfluid 4He. An expression is obtained for the phase-conjugated wave at the boundary, and the conversion efficiency is estimated. The second nonlinear problem is the excitation of surface second-sound waves by bulk second-sound waves in superfluid solutions of 3He in 4He. An equation is derived for the amp

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46

Hunstad, I., A. Marsili, P. Casale, M. Vallocchia, and P. Burrato. "Seismic Waves and Sound Waves: From Earthquakes to Music." Seismological Research Letters 84, no. 3 (2013): 532–35. http://dx.doi.org/10.1785/0220120095.

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47

Buckingham, Michael J. "Sound waves and shear waves in saturated unconsolidated sediments." Journal of the Acoustical Society of America 120, no. 5 (2006): 3097. http://dx.doi.org/10.1121/1.4787524.

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48

Inoue, Kazuko, and Tomio Ariyasu. "Sound waves and shock waves in high-density deuterium." Laser and Particle Beams 9, no. 4 (1991): 795–816. http://dx.doi.org/10.1017/s026303460000656x.

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The possibility of compressing the cryogenic hollow pellet of inertial confinement nuclear fusion with multiple adiabatic shock waves is discussed, on the basis of the estimation of the properties of a high-density deuterium plasma (1024−1027 cm−3, 10−1−104 eV), such as the velocity and the attenuation constant of the adiabatic sound wave, the width of the shock wave, and the surface tension.It is found that in the course of compression the wavelength of the adiabatic sound wave and the width of the weak shock wave sometimes become comparable to or exceed the fuel shell width of the pellet, an

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49

Downie, Neil A. "Seeing sound waves: a simple method to see sound waves travelling through the open air." Physics Education 48, no. 2 (2013): 199–202. http://dx.doi.org/10.1088/0031-9120/48/2/199.

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50

Thejappa, G., and R. J. MacDowall. "High frequency ion sound waves associated with Langmuir waves in type III radio burst source regions." Nonlinear Processes in Geophysics 11, no. 3 (2004): 411–20. http://dx.doi.org/10.5194/npg-11-411-2004.

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Abstract. Short wavelength ion sound waves (2-4kHz) are detected in association with the Langmuir waves (~15-30kHz) in the source regions of several local type III radio bursts. They are most probably not due to any resonant wave-wave interactions such as the electrostatic decay instability because their wavelengths are much shorter than those of Langmuir waves. The Langmuir waves occur as coherent field structures with peak intensities exceeding the Langmuir collapse thresholds. Their scale sizes are of the order of the wavelength of an ion sound wave. These Langmuir wave field characteristic

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