Pub Date : 2025-08-18DOI: 10.1134/S1063771024602450
L. Huang, R. Zeng
This study examines the performance of six different two-dimensional, 18-element microphone array geometries—BK, Ring, Reuleaux, Logarithmic, Triangle, and Starfish—for sound source localization. The arrays’ performances are systematically evaluated using beamforming algorithms and acoustic pressure reconstruction, focusing on key metrics such as main lobe width, side lobe magnitude, reconstruction error, and resolution quality over frequencies ranging from 0 to 3000 Hz. Additionally, the study investigates the adaptability of these configurations at various distances and explores their frequency-dependent behavior. The results indicate that array geometry substantially impacts localization accuracy, with the Starfish configuration demonstrating superior overall performance, exhibiting the narrowest main lobe width, highest main lobe amplitude, lowest reconstruction error, and consistently high resolution. Thus, the Starfish configuration is recommended as optimal for effective sound source localization applications.
{"title":"Geometry-Dependent Performance in Sound Localization: A Study of 18-Element Microphone Arrays","authors":"L. Huang, R. Zeng","doi":"10.1134/S1063771024602450","DOIUrl":"10.1134/S1063771024602450","url":null,"abstract":"<p>This study examines the performance of six different two-dimensional, 18-element microphone array geometries—BK, Ring, Reuleaux, Logarithmic, Triangle, and Starfish—for sound source localization. The arrays’ performances are systematically evaluated using beamforming algorithms and acoustic pressure reconstruction, focusing on key metrics such as main lobe width, side lobe magnitude, reconstruction error, and resolution quality over frequencies ranging from 0 to 3000 Hz. Additionally, the study investigates the adaptability of these configurations at various distances and explores their frequency-dependent behavior. The results indicate that array geometry substantially impacts localization accuracy, with the Starfish configuration demonstrating superior overall performance, exhibiting the narrowest main lobe width, highest main lobe amplitude, lowest reconstruction error, and consistently high resolution. Thus, the Starfish configuration is recommended as optimal for effective sound source localization applications<i>.</i></p>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"135 - 143"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861571","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-18DOI: 10.1134/S1063771025600329
I. A. Karpov, Yu. I. Bobrovnitskii
Abstract—Damping (dissipation, energy losses) is the most important parameter of all mechanical oscillatory systems, in addition to elasticity and inertia. Its special role is due to the fact that it directly determines the maximum amplitudes of free and forced vibrations of systems and, accordingly, their dynamic strength and reliability, noise and ecology. Due to the poor study of the physical processes of damping, it is measured experimentally. This article presents one of the new efficient methods for experimental determination of losses, characterized by simplicity, high accuracy and a wide range of applicability. The main attention is paid to substantiation of the method, its properties, and its verification in numerical and laboratory experiments. The method is recommended for measuring the losses of composite highly damped oscillatory systems, where known methods do not work or are too complex.
{"title":"Experimental Method for Determining Energy Losses in Oscillatory Systems Based on ARMA Modeling","authors":"I. A. Karpov, Yu. I. Bobrovnitskii","doi":"10.1134/S1063771025600329","DOIUrl":"10.1134/S1063771025600329","url":null,"abstract":"<p><b>Abstract</b>—Damping (dissipation, energy losses) is the most important parameter of all mechanical oscillatory systems, in addition to elasticity and inertia. Its special role is due to the fact that it directly determines the maximum amplitudes of free and forced vibrations of systems and, accordingly, their dynamic strength and reliability, noise and ecology. Due to the poor study of the physical processes of damping, it is measured experimentally. This article presents one of the new efficient methods for experimental determination of losses, characterized by simplicity, high accuracy and a wide range of applicability. The main attention is paid to substantiation of the method, its properties, and its verification in numerical and laboratory experiments. The method is recommended for measuring the losses of composite highly damped oscillatory systems, where known methods do not work or are too complex.</p>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"144 - 162"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861569","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-18DOI: 10.1134/S1063771024603091
A. Ya. Zverev, L. A. Lazarev, I. V. Pankratov
Reducing noise in the cabin of propeller aircraft is an urgent problem of internal acoustics, since traditional sound-insulating structures are insufficiently effective in the low-frequency region. One promising method for solving it is to use resonance systems, with which it is possible to significantly increase the sound insulation of the fuselage structure of aircraft in this frequency range. The study determined the effect of resonance systems on the sound-insulating ability of flat and cylindrical panels without and with cross stiffening simulating the body bulkhead frame was experimentally determined, as well as the effectiveness of facing the passenger compartment with resonance systems with different compositions. Tests were carried out in sound chambers and on a full-scale bench, which is a real passenger plane. The tested structures were faced with elastoacoustic compensators of various types with resonance elements made of foil, micalent paper, and thermopolyurethane. It is shown that the efficiency of resonance systems can reach 10–20 dB or more.
{"title":"Sound Insulation of Fuselage Aircraft Structures with Different Compositions of Resonance Elements","authors":"A. Ya. Zverev, L. A. Lazarev, I. V. Pankratov","doi":"10.1134/S1063771024603091","DOIUrl":"10.1134/S1063771024603091","url":null,"abstract":"<p>Reducing noise in the cabin of propeller aircraft is an urgent problem of internal acoustics, since traditional sound-insulating structures are insufficiently effective in the low-frequency region. One promising method for solving it is to use resonance systems, with which it is possible to significantly increase the sound insulation of the fuselage structure of aircraft in this frequency range. The study determined the effect of resonance systems on the sound-insulating ability of flat and cylindrical panels without and with cross stiffening simulating the body bulkhead frame was experimentally determined, as well as the effectiveness of facing the passenger compartment with resonance systems with different compositions. Tests were carried out in sound chambers and on a full-scale bench, which is a real passenger plane. The tested structures were faced with elastoacoustic compensators of various types with resonance elements made of foil, micalent paper, and thermopolyurethane. It is shown that the efficiency of resonance systems can reach 10–20 dB or more.</p>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"277 - 281"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861596","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-18DOI: 10.1134/S1063771024602954
A. V. Shatravin
The article presents the results of a full-scale experiment aimed at assessing the temporal variability of the impulse response of a hydroacoustic channel and efficiency of coherent underwater acoustic communications using bottom-mounted transmitters and receivers at frequencies of ~10 kHz on the Black Sea shelf in autumn. Three prominent maxima of variable amplitude were observed in the impulse response structure throughout the experiment (~36 h). The range of variability of the root-mean-square decoding error was ~11 dB; the bit error ratio varied from 0 to 0.10. A strong relationship was found between the values of decoding errors and the amplitude of the maximum arrival in the structure of the reference impulse response, corresponding to a group of rays with one reflection off the surface, as well as the coefficient of variation of high-frequency fluctuations of the amplitude of this arrival in the instantaneous estimate of the impulse response. Numerical modeling was used to confirm the hypothesis that in autumn conditions, characterized by the absence of a pronounced seasonal thermocline, the main hydrophysical cause of the variability of the amplitude of the main arrival, and, as a consequence, the effectiveness of underwater acoustic communications, consisted in an insignificant (fractions of a degree) change of temperature in the upper layer of sea water.
{"title":"Acoustic Impulse Response Fluctuations and Coherent Underwater Acoustic Communications in Shallow Water under Autumn Conditions","authors":"A. V. Shatravin","doi":"10.1134/S1063771024602954","DOIUrl":"10.1134/S1063771024602954","url":null,"abstract":"<div><p>The article presents the results of a full-scale experiment aimed at assessing the temporal variability of the impulse response of a hydroacoustic channel and efficiency of coherent underwater acoustic communications using bottom-mounted transmitters and receivers at frequencies of ~10 kHz on the Black Sea shelf in autumn. Three prominent maxima of variable amplitude were observed in the impulse response structure throughout the experiment (~36 h). The range of variability of the root-mean-square decoding error was ~11 dB; the bit error ratio varied from 0 to 0.10. A strong relationship was found between the values of decoding errors and the amplitude of the maximum arrival in the structure of the reference impulse response, corresponding to a group of rays with one reflection off the surface, as well as the coefficient of variation of high-frequency fluctuations of the amplitude of this arrival in the instantaneous estimate of the impulse response. Numerical modeling was used to confirm the hypothesis that in autumn conditions, characterized by the absence of a pronounced seasonal thermocline, the main hydrophysical cause of the variability of the amplitude of the main arrival, and, as a consequence, the effectiveness of underwater acoustic communications, consisted in an insignificant (fractions of a degree) change of temperature in the upper layer of sea water.</p></div>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"223 - 239"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861411","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-18DOI: 10.1134/S1063771025600317
M. A. Mironov
The propagation of torsional waves through rods with a variable cross section is considered. When the flattening of a rod is linearly increased, the propagation velocity of a torsional wave also linearly decreases to become zero at a finite rod length. Meanwhile, the time of propagation to the sharpened end is equal to infinity. In contemporary terminology, such a decelerating structure is called a vibrational black hole. Exact solutions are found for the equations of torsional vibrations in a sharpened rod with an inertia moment and a torsion moment in the form of power functions along with corresponding expressions for the input impedance at the initial cross section.
{"title":"A Vibrational Black Hole for Torsional Waves Propagating through a Rod with a Variable Cross Section","authors":"M. A. Mironov","doi":"10.1134/S1063771025600317","DOIUrl":"10.1134/S1063771025600317","url":null,"abstract":"<p>The propagation of torsional waves through rods with a variable cross section is considered. When the flattening of a rod is linearly increased, the propagation velocity of a torsional wave also linearly decreases to become zero at a finite rod length. Meanwhile, the time of propagation to the sharpened end is equal to infinity. In contemporary terminology, such a decelerating structure is called a vibrational black hole. Exact solutions are found for the equations of torsional vibrations in a sharpened rod with an inertia moment and a torsion moment in the form of power functions along with corresponding expressions for the input impedance at the initial cross section.</p>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"163 - 169"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1134/S1063771025600317.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861570","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-18DOI: 10.1134/S1063771024601754
Yu. V. Petukhov, E. L. Borodina
Using numerical modeling based on mode theory and the geometric-acoustic approximation, it was determined that in addition to classical quadruples of pulses present in the spatiotemporal field structure, the emergence of additional signals with relatively short delays is caused by the formation of weakly divergent multimode beams in the underwater sound channel of the Sea of Japan; these modes correspond to smooth extrema in the dependences of the spatial interference period of neighboring modes and their group velocity on the mode number. For one of the two sound speed profiles typical of the Sea of Japan, it was shown that at relatively high frequencies, it is possible to receive two groups of additional signals: weakly divergent beams formed by relatively low- and high-order modes.
{"title":"Theoretical Analysis of the Influence of Weakly Divergent Beams on the Formation of the Spatiotemporal Structure of Pulse Signals in the Sea of Japan","authors":"Yu. V. Petukhov, E. L. Borodina","doi":"10.1134/S1063771024601754","DOIUrl":"10.1134/S1063771024601754","url":null,"abstract":"<p>Using numerical modeling based on mode theory and the geometric-acoustic approximation, it was determined that in addition to classical quadruples of pulses present in the spatiotemporal field structure, the emergence of additional signals with relatively short delays is caused by the formation of weakly divergent multimode beams in the underwater sound channel of the Sea of Japan; these modes correspond to smooth extrema in the dependences of the spatial interference period of neighboring modes and their group velocity on the mode number. For one of the two sound speed profiles typical of the Sea of Japan, it was shown that at relatively high frequencies, it is possible to receive two groups of additional signals: weakly divergent beams formed by relatively low- and high-order modes.</p>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"216 - 222"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861400","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-18DOI: 10.1134/S1063771025600238
D. I. Zotov, O. D. Rumyantseva
A technique for correcting the fields detected by an array with nonideal placement of transmitting and receiving transducers has been developed and numerically tested. The displacements of the transducers from their ideal positions are preliminarily determined. The correction technique involves finding the angular harmonics based on the fields measured with the displaced transducers. Then these found angular harmonics make it possible to recalculate the fields at ideal positions of the transducers, as well as directly calculate the scattering amplitude. Such corrected data is the input one for the stage of reconstruction of acoustic tomograms, i.e., the internal structure of an object. Numerical simulation has been used to show that in the absence of the correction of the data measured in real conditions, the tomograms can be fractured.
{"title":"Compensating the Effect of the Displacement of Array Transducers on Tomography Data","authors":"D. I. Zotov, O. D. Rumyantseva","doi":"10.1134/S1063771025600238","DOIUrl":"10.1134/S1063771025600238","url":null,"abstract":"<p>A technique for correcting the fields detected by an array with nonideal placement of transmitting and receiving transducers has been developed and numerically tested. The displacements of the transducers from their ideal positions are preliminarily determined. The correction technique involves finding the angular harmonics based on the fields measured with the displaced transducers. Then these found angular harmonics make it possible to recalculate the fields at ideal positions of the transducers, as well as directly calculate the scattering amplitude. Such corrected data is the input one for the stage of reconstruction of acoustic tomograms, i.e., the internal structure of an object. Numerical simulation has been used to show that in the absence of the correction of the data measured in real conditions, the tomograms can be fractured.</p>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"282 - 299"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861597","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-08-18DOI: 10.1134/S1063771025600354
S. P. Aksenov, G. N. Kuznetsov, A. N. Stepanov
The spatial–frequency responses of the amplitudes and phases of the sound pressure in deep water have been studied. Analytical relationships have been obtained that make it possible to calculate and compare the amplitude–phase structures of water, leaky, and trapped modes, as well as the sound pressure field formed by the sum of the modes. The calculations were performed using the modified WKB (Wentzel–Kramers–Brillouin) approximation. It has been shown that in deep water, as in shallow water, there are stable equal phase lines along which, under certain conditions, coherent summation of complex Fourier components is possible. To describe the equal phase lines, a differential equation has been obtained that uses the phase invariant, already studied in shallow water, as a basic parameter. This has made it possible to study the properties of the phase invariant corresponding to water, leaky, and trapped modes in all zones of the sound field for deep water as well. It is established that at different distances in the field constructed from the sum of all modes, invariant properties are manifested, primarily, the modes that dominate at these distances. It is shown that leaky modes formed in the near illumination zone and in the shadow zone, formed by steep rays reflected from the bottom, have invariant properties only at large distances from the source. Water and trapped modes have invariant properties in full and at all distances. Recommendations are given on the use of equal phase lines and the phase invariant in processing experimental data and modeling.
{"title":"Equal Phase Lines and Phase Invariant in the Sound Field of Deep Water","authors":"S. P. Aksenov, G. N. Kuznetsov, A. N. Stepanov","doi":"10.1134/S1063771025600354","DOIUrl":"10.1134/S1063771025600354","url":null,"abstract":"<div><p>The spatial–frequency responses of the amplitudes and phases of the sound pressure in deep water have been studied. Analytical relationships have been obtained that make it possible to calculate and compare the amplitude–phase structures of water, leaky, and trapped modes, as well as the sound pressure field formed by the sum of the modes. The calculations were performed using the modified WKB (Wentzel–Kramers–Brillouin) approximation. It has been shown that in deep water, as in shallow water, there are stable equal phase lines along which, under certain conditions, coherent summation of complex Fourier components is possible. To describe the equal phase lines, a differential equation has been obtained that uses the phase invariant, already studied in shallow water, as a basic parameter. This has made it possible to study the properties of the phase invariant corresponding to water, leaky, and trapped modes in all zones of the sound field for deep water as well. It is established that at different distances in the field constructed from the sum of all modes, invariant properties are manifested, primarily, the modes that dominate at these distances. It is shown that leaky modes formed in the near illumination zone and in the shadow zone, formed by steep rays reflected from the bottom, have invariant properties only at large distances from the source. Water and trapped modes have invariant properties in full and at all distances. Recommendations are given on the use of equal phase lines and the phase invariant in processing experimental data and modeling.</p></div>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 2","pages":"201 - 215"},"PeriodicalIF":1.2,"publicationDate":"2025-08-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144861399","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-05-21DOI: 10.1134/S1063771024602309
A. V. Klemina, S. N. Gurbatov, V. A. Klemin
Acoustic methods of nonreactive medical laboratory diagnostics were developed using the BIOM acoustic analyzer as a measuring device. The device contains two ultrasmall ultrasonic resonators (about 100 µL) in volume. The device’s microprocessor system controls two ultrathermostats and maintains temperatures in the resonators in the range 20–38°C with an accuracy of ± 0.005°C. The developed special software makes it possible to determine the acoustic characteristics (rate and absorption of ultrasound) in blood serum, whole blood, and plasma with a relative error of ±5 × 10–4 in terms of speed of ultrasound and ±10–2 in terms of ultrasound absorption. This made it possible to determine the total protein, protein fractions, parameters of the lipid spectrum, and apolipoproteins A1 and B, as well as the elastic properties of patients' erythrocytes in vitro.The article presents a flowchart of the acoustic analyzer, an algorithm for its functioning, describes acoustic methods for determining total protein, protein fractions, lipid spectrum, and apolipoproteins A1 and B in blood serum and the elasticity of erythrocytes in whole blood in vitro.
{"title":"Acoustic Methods of Reagentless Medical Laboratory Diagnostics","authors":"A. V. Klemina, S. N. Gurbatov, V. A. Klemin","doi":"10.1134/S1063771024602309","DOIUrl":"10.1134/S1063771024602309","url":null,"abstract":"<div><p>Acoustic methods of nonreactive medical laboratory diagnostics were developed using the BIOM acoustic analyzer as a measuring device. The device contains two ultrasmall ultrasonic resonators (about 100 µL) in volume. The device’s microprocessor system controls two ultrathermostats and maintains temperatures in the resonators in the range 20–38°C with an accuracy of ± 0.005°C. The developed special software makes it possible to determine the acoustic characteristics (rate and absorption of ultrasound) in blood serum, whole blood, and plasma with a relative error of ±5 × 10<sup>–4</sup> in terms of speed of ultrasound and ±10<sup>–2</sup> in terms of ultrasound absorption. This made it possible to determine the total protein, protein fractions, parameters of the lipid spectrum, and apolipoproteins A1 and B, as well as the elastic properties of patients' erythrocytes in vitro.The article presents a flowchart of the acoustic analyzer, an algorithm for its functioning, describes acoustic methods for determining total protein, protein fractions, lipid spectrum, and apolipoproteins A1 and B in blood serum and the elasticity of erythrocytes in whole blood in vitro.</p></div>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 1","pages":"128 - 133"},"PeriodicalIF":1.2,"publicationDate":"2025-05-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145122220","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-05-21DOI: 10.1134/S1063771024603261
L. A. Ostrovsky
The article discusses nontrivial points related to the invention, theory, and applications of radiating and receiving parametric acoustic arrays (PAs) in the United States and Soviet Union.
本文讨论了美国和苏联有关辐射和接收参数声阵列(PAs)的发明、理论和应用的重要问题。
{"title":"On the History of Parametric Acoustic Arrays","authors":"L. A. Ostrovsky","doi":"10.1134/S1063771024603261","DOIUrl":"10.1134/S1063771024603261","url":null,"abstract":"<div><p>The article discusses nontrivial points related to the invention, theory, and applications of radiating and receiving parametric acoustic arrays (PAs) in the United States and Soviet Union.</p></div>","PeriodicalId":455,"journal":{"name":"Acoustical Physics","volume":"71 1","pages":"18 - 22"},"PeriodicalIF":1.2,"publicationDate":"2025-05-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145122204","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}