As occupational hearing loss (OHL) is a concern among women, a cross-sectional study was conducted. Individual noise exposure energy and temporal structure were quantified using the 8 h continuous equivalent A-weighted sound pressure level (LAeq,8h) and kurtosis (β). High-frequency noise-induced hearing loss (HFNIHL) and noise-induced hearing impairment (NIHI) were calculated. The HFNIHL and NIHI prevalences were 13.45% and 13.20%, respectively. Hearing loss was symmetrically distributed, with the most significant threshold shifts occurring at 4.0 kHz. The OHL prevalence was significantly higher in individuals exposed to non-steady rather than steady noise. A marked increase in OHL prevalence was observed among women exposed to non-steady noise for 3 to 10 years. The steady noise group exhibited an increase, followed by a plateau or decline. Key influencing factors for women's OHL were LAeq,8h, age, and kurtosis, with odds ratios (ORs) ranked as follows: ORLAeq,8h > ORAge > ORKurtosis. After adjusting for kurtosis in LAeq,8h, the model fit (Akaike Information Criterion) of the dose-response relationship improved significantly. These findings suggested that female manufacturing workers were at high risk of OHL with significant clinical characteristics. Noise kurtosis could accelerate and exacerbate women's OHL development. Kurtosis adjustment for noise level could effectively evaluate women's OHL.
{"title":"Exploring primary characteristics of occupational hearing loss in female manufacturing workers: A cross-sectional study.","authors":"Changyan Yu, Yuwen Huang, Jinzhe Li, Hua Zou, Jiarui Xin, Anke Zeng, Xiaohan Li, Wei Qiu, Meibian Zhang","doi":"10.1121/10.0042446","DOIUrl":"https://doi.org/10.1121/10.0042446","url":null,"abstract":"<p><p>As occupational hearing loss (OHL) is a concern among women, a cross-sectional study was conducted. Individual noise exposure energy and temporal structure were quantified using the 8 h continuous equivalent A-weighted sound pressure level (LAeq,8h) and kurtosis (β). High-frequency noise-induced hearing loss (HFNIHL) and noise-induced hearing impairment (NIHI) were calculated. The HFNIHL and NIHI prevalences were 13.45% and 13.20%, respectively. Hearing loss was symmetrically distributed, with the most significant threshold shifts occurring at 4.0 kHz. The OHL prevalence was significantly higher in individuals exposed to non-steady rather than steady noise. A marked increase in OHL prevalence was observed among women exposed to non-steady noise for 3 to 10 years. The steady noise group exhibited an increase, followed by a plateau or decline. Key influencing factors for women's OHL were LAeq,8h, age, and kurtosis, with odds ratios (ORs) ranked as follows: ORLAeq,8h > ORAge > ORKurtosis. After adjusting for kurtosis in LAeq,8h, the model fit (Akaike Information Criterion) of the dose-response relationship improved significantly. These findings suggested that female manufacturing workers were at high risk of OHL with significant clinical characteristics. Noise kurtosis could accelerate and exacerbate women's OHL development. Kurtosis adjustment for noise level could effectively evaluate women's OHL.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1489-1500"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146180812","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Charles A Muirhead, Wendy E D Piniak, Douglas P Nowacek, Craig A Harms
Anthropogenic noise may pose a threat to Kemp's ridley sea turtles in nearshore and offshore waters of the western North Atlantic and Gulf of America, where shipping and energy industries are widespread. Understanding hearing sensitivity is necessary for the development of effective noise impact mitigation strategies. However, data gaps currently exist. Therefore, in this study, we measured auditory evoked potentials (AEP) to determine the underwater hearing sensitivities of 13 juvenile Kemp's ridley sea turtles using hearing test frequencies ranging from 50 to 1600 Hz. We detected AEPs for hearing test signals between 50 and 800 Hz. Peak hearing sensitivity occurred between 200 and 300 Hz, followed by a decline in sensitivity above 400 Hz. The lowest hearing threshold averaged across all test subjects was 100 dB re 1 μPa at 300 Hz. No responses were detected at 1200 Hz (max received level = 143 dB re 1 μPa) and 1600 Hz (max received level = 143-165 dB re 1 μPa). Our results averaged across multiple individuals at 100 Hz (n = 9), 200 Hz (n = 8), 300 Hz (n = 5), and 400 Hz (n = 8) reveal lower hearing thresholds (greater sensitivity) than those reported in a previous study of two Kemp's ridley sea turtles at these frequencies. The results presented here should be considered a conservative estimate of hearing sensitivity, as perceptual hearing thresholds are likely lower than what can be determined with AEPs.
在航运和能源工业广泛分布的北大西洋西部和美国湾的近岸和近海水域,人为噪音可能对坎普雷德利海龟构成威胁。了解听力敏感性对于制定有效的噪声影响缓解策略是必要的。然而,目前存在数据缺口。因此,在本研究中,我们通过测量听觉诱发电位(AEP)来确定13只肯普雷利海龟幼龟的水下听觉灵敏度,听力测试频率为50 ~ 1600 Hz。我们检测了听力测试信号在50 - 800 Hz之间的aep。峰值听力灵敏度出现在200至300赫兹之间,随后灵敏度在400赫兹以上下降。所有被试在300 Hz时平均最低听阈为100 dB / 1 μPa。在1200 Hz(最大接收电平= 143 dB re 1 μPa)和1600 Hz(最大接收电平= 143 ~ 165 dB re 1 μPa)下无响应。我们在100赫兹(n = 9), 200赫兹(n = 8), 300赫兹(n = 5)和400赫兹(n = 8)下对多个个体的平均结果显示,与之前对两只肯普雷利海龟在这些频率下的研究报告相比,听力阈值更低(灵敏度更高)。这里提出的结果应该被认为是对听力敏感性的保守估计,因为感知听力阈值可能低于用AEPs确定的阈值。
{"title":"Underwater hearing sensitivity of the Kemp's ridley sea turtle (Lepidochelys kempii).","authors":"Charles A Muirhead, Wendy E D Piniak, Douglas P Nowacek, Craig A Harms","doi":"10.1121/10.0041867","DOIUrl":"https://doi.org/10.1121/10.0041867","url":null,"abstract":"<p><p>Anthropogenic noise may pose a threat to Kemp's ridley sea turtles in nearshore and offshore waters of the western North Atlantic and Gulf of America, where shipping and energy industries are widespread. Understanding hearing sensitivity is necessary for the development of effective noise impact mitigation strategies. However, data gaps currently exist. Therefore, in this study, we measured auditory evoked potentials (AEP) to determine the underwater hearing sensitivities of 13 juvenile Kemp's ridley sea turtles using hearing test frequencies ranging from 50 to 1600 Hz. We detected AEPs for hearing test signals between 50 and 800 Hz. Peak hearing sensitivity occurred between 200 and 300 Hz, followed by a decline in sensitivity above 400 Hz. The lowest hearing threshold averaged across all test subjects was 100 dB re 1 μPa at 300 Hz. No responses were detected at 1200 Hz (max received level = 143 dB re 1 μPa) and 1600 Hz (max received level = 143-165 dB re 1 μPa). Our results averaged across multiple individuals at 100 Hz (n = 9), 200 Hz (n = 8), 300 Hz (n = 5), and 400 Hz (n = 8) reveal lower hearing thresholds (greater sensitivity) than those reported in a previous study of two Kemp's ridley sea turtles at these frequencies. The results presented here should be considered a conservative estimate of hearing sensitivity, as perceptual hearing thresholds are likely lower than what can be determined with AEPs.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1105-1112"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146113449","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Shitao Sun, Yuhan Bi, Xi Zhang, Donglai Yang, Wendi Zhang, Hongguang Li
To address the dual demands of high static load capacity and low resonance frequency in underwater electrodynamic transducers, this study introduces a nonlinear supporting mechanism based on a tension spring-roller-cam quasi-zero stiffness (QZS) structure. The mechanism effectively reduces the equivalent stiffness while maintaining high static load capacity, achieving lower resonance frequency and enhanced ultra-low-frequency vibration performance. A nonlinear dynamic model of the transducer is developed, and displacement and sound pressure level responses are analyzed using the harmonic balance method. Numerical simulations reveal the influence of mechanical damping and excitation amplitude on the system's vibration characteristics. Comparative analysis shows that the QZS-supported system exhibits a significantly lower resonance frequency and improved low-frequency vibration behavior than the conventional linear system. Experimental validation using impact hammer testing confirms a significant reduction in resonance frequency and enhanced acceleration response in the ultra-low-frequency range. These findings validate the capability of the proposed QZS suspension mechanism to achieve ultra-low resonance frequency, suggesting its potential for application in underwater ultra-low-frequency electrodynamic transducers.
{"title":"Quasi-zero stiffness suspension for reducing the resonance frequency of underwater electrodynamic transducers.","authors":"Shitao Sun, Yuhan Bi, Xi Zhang, Donglai Yang, Wendi Zhang, Hongguang Li","doi":"10.1121/10.0042383","DOIUrl":"https://doi.org/10.1121/10.0042383","url":null,"abstract":"<p><p>To address the dual demands of high static load capacity and low resonance frequency in underwater electrodynamic transducers, this study introduces a nonlinear supporting mechanism based on a tension spring-roller-cam quasi-zero stiffness (QZS) structure. The mechanism effectively reduces the equivalent stiffness while maintaining high static load capacity, achieving lower resonance frequency and enhanced ultra-low-frequency vibration performance. A nonlinear dynamic model of the transducer is developed, and displacement and sound pressure level responses are analyzed using the harmonic balance method. Numerical simulations reveal the influence of mechanical damping and excitation amplitude on the system's vibration characteristics. Comparative analysis shows that the QZS-supported system exhibits a significantly lower resonance frequency and improved low-frequency vibration behavior than the conventional linear system. Experimental validation using impact hammer testing confirms a significant reduction in resonance frequency and enhanced acceleration response in the ultra-low-frequency range. These findings validate the capability of the proposed QZS suspension mechanism to achieve ultra-low resonance frequency, suggesting its potential for application in underwater ultra-low-frequency electrodynamic transducers.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1385-1399"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146165330","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Giovanni Coco, Didier Dragna, Christophe Bailly, Hélène Posson
A formulation to introduce acoustic waves from a control surface using volumetric source terms is proposed for numerical simulations. A general expression of the source terms is derived from the non-linear Euler equations. The method is validated through three academic configurations: the injection of oblique plane waves and the radiation of a monopole source in two and three dimensions, in uniform flow. The governing equations are solved in a Cartesian grid using a low-dispersion and low-dissipation high order finite-difference numerical scheme. However, the control surface has an arbitrary shape, as demonstrated here with the use of a cylindrical surface. Numerical results show good agreement with analytical solutions in both phase and amplitude. The method is then applied to an open-fan aircraft engine configuration. The source terms are computed from a cylindrical control surface enclosing the rotor, based on data extracted from a previous fluid mechanics simulation. The radiated acoustic field is compared with the one obtained using the Ffowcs Williams-Hawkings integral formulation. The two solutions are again found in good agreement for this more realistic configuration.
提出了一种利用体积源项从控制面引入声波的数值模拟公式。源项的一般表达式是由非线性欧拉方程导出的。通过三种理论配置:斜平面波注入和单极子源在二维和三维均匀流动中的辐射,验证了该方法。控制方程采用低色散、低耗散的高阶有限差分格式在直角网格中求解。然而,控制面具有任意形状,如这里使用的圆柱形面所示。数值结果与解析解在相位和振幅上都吻合较好。然后将该方法应用于开式飞机发动机结构。源项是基于从先前流体力学模拟中提取的数据,从封闭转子的圆柱形控制面计算得到的。将辐射声场与采用Ffowcs - williams - hawkins积分公式得到的声场进行了比较。对于这种更现实的配置,这两种解决方案再次得到了很好的一致。
{"title":"Injection of acoustic waves via volumetric sources on a control surface for computational aeroacoustics.","authors":"Giovanni Coco, Didier Dragna, Christophe Bailly, Hélène Posson","doi":"10.1121/10.0042388","DOIUrl":"https://doi.org/10.1121/10.0042388","url":null,"abstract":"<p><p>A formulation to introduce acoustic waves from a control surface using volumetric source terms is proposed for numerical simulations. A general expression of the source terms is derived from the non-linear Euler equations. The method is validated through three academic configurations: the injection of oblique plane waves and the radiation of a monopole source in two and three dimensions, in uniform flow. The governing equations are solved in a Cartesian grid using a low-dispersion and low-dissipation high order finite-difference numerical scheme. However, the control surface has an arbitrary shape, as demonstrated here with the use of a cylindrical surface. Numerical results show good agreement with analytical solutions in both phase and amplitude. The method is then applied to an open-fan aircraft engine configuration. The source terms are computed from a cylindrical control surface enclosing the rotor, based on data extracted from a previous fluid mechanics simulation. The radiated acoustic field is compared with the one obtained using the Ffowcs Williams-Hawkings integral formulation. The two solutions are again found in good agreement for this more realistic configuration.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1151-1162"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146125437","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Elizabeth D Young, Shae D Morgan, Sarah Hargus Ferguson
Clear speech, a speaking style used to communicate with individuals with hearing loss and other communication difficulties, has been shown to sound "angry" more often than conversational speech [Morgan and Ferguson (2017). J. Speech. Lang. Hear. Res. 60, 2271-2280]. In this study, acoustic analyses of emotionally neutral sentences from a database of 41 talkers spoken both clearly and conversationally were analyzed in tandem with judgments of emotions for the same sentences to assess potential acoustic correlates of judgments of anger in clear speech. Principal component analyses were conducted to guide the selection of acoustic measures for statistical models. Decreases in speaking rate and increases in temporal fluctuations in amplitude centered at 1 Hz, both of which are prominent features of clear speech, were both associated with increases in judgments of anger. Increases in fundamental frequency variability, another common feature of clear speech, were associated with increases in judgments of any amount of anger but only in conversational speech. Finally, after controlling for speaking style and fundamental frequency variability, women were judged to sound angry more often than men. The results suggest that speaking rate, amount of word or phrase-level amplitude modulation, and fundamental frequency variability could possibly be manipulated to decrease judgments of anger in clear speech.
{"title":"Gender, pitch variability, speaking rate, and low-frequency modulation affect judgments of anger in clear speecha).","authors":"Elizabeth D Young, Shae D Morgan, Sarah Hargus Ferguson","doi":"10.1121/10.0042447","DOIUrl":"https://doi.org/10.1121/10.0042447","url":null,"abstract":"<p><p>Clear speech, a speaking style used to communicate with individuals with hearing loss and other communication difficulties, has been shown to sound \"angry\" more often than conversational speech [Morgan and Ferguson (2017). J. Speech. Lang. Hear. Res. 60, 2271-2280]. In this study, acoustic analyses of emotionally neutral sentences from a database of 41 talkers spoken both clearly and conversationally were analyzed in tandem with judgments of emotions for the same sentences to assess potential acoustic correlates of judgments of anger in clear speech. Principal component analyses were conducted to guide the selection of acoustic measures for statistical models. Decreases in speaking rate and increases in temporal fluctuations in amplitude centered at 1 Hz, both of which are prominent features of clear speech, were both associated with increases in judgments of anger. Increases in fundamental frequency variability, another common feature of clear speech, were associated with increases in judgments of any amount of anger but only in conversational speech. Finally, after controlling for speaking style and fundamental frequency variability, women were judged to sound angry more often than men. The results suggest that speaking rate, amount of word or phrase-level amplitude modulation, and fundamental frequency variability could possibly be manipulated to decrease judgments of anger in clear speech.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1359-1372"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146157157","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Yubo Han, Shuping Han, YaoHui Hu, Jingfeng Xu, Gang Yang
In underwater mobile spread spectrum communications, time-varying Doppler effects cause severe carrier phase jumps, significantly degrading spreading gain. Addressing the limitations of conventional compensation techniques under high relative velocities, this study investigates the correlation cost factor (CCF) during de-spreading in M-ary spread spectrum systems. Theoretical analysis reveals that CCF serves as an effective loss function for frequency offset compensation. Leveraging this, a high-resolution Doppler estimation method (HCCF-MSS) is proposed. HCCF-MSS employs the adaptive learning rate of the Adam optimizer to update step sizes, enabling rapid, high-precision convergence of the CCF loss function to the accurate frequency offset. To mitigate convergence to local minima in highly dynamic environments, the Multi-starting Point Parallel Gradient Search (MPGS) algorithm is introduced. MPGS initiates concurrent gradient searches from diverse starting points and selects the optimal solution by comparing CCF values across convergent paths. Numerical simulations and sea trials demonstrate that HCCF-MSS-9 (9 iterations) achieves performance comparable to CCF-MSS-0.02 (±6 Hz range, 0.02 Hz precision) with superior computational efficiency. Under accelerations up to 3 m/s2, HCCF-MSS-9+MPGS-6 (6 starting points) attains a Doppler estimation mean squared error of approximately -3.3 dB, outperforming other algorithms by 0.5-1.5 dB, demonstrating its effectiveness for precise frequency offset estimation under complex variable-motion conditions.
{"title":"Doppler compensation technique for M-ary spread spectrum signals with low complexity and high resolution in mobile underwater acoustic communication.","authors":"Yubo Han, Shuping Han, YaoHui Hu, Jingfeng Xu, Gang Yang","doi":"10.1121/10.0042445","DOIUrl":"https://doi.org/10.1121/10.0042445","url":null,"abstract":"<p><p>In underwater mobile spread spectrum communications, time-varying Doppler effects cause severe carrier phase jumps, significantly degrading spreading gain. Addressing the limitations of conventional compensation techniques under high relative velocities, this study investigates the correlation cost factor (CCF) during de-spreading in M-ary spread spectrum systems. Theoretical analysis reveals that CCF serves as an effective loss function for frequency offset compensation. Leveraging this, a high-resolution Doppler estimation method (HCCF-MSS) is proposed. HCCF-MSS employs the adaptive learning rate of the Adam optimizer to update step sizes, enabling rapid, high-precision convergence of the CCF loss function to the accurate frequency offset. To mitigate convergence to local minima in highly dynamic environments, the Multi-starting Point Parallel Gradient Search (MPGS) algorithm is introduced. MPGS initiates concurrent gradient searches from diverse starting points and selects the optimal solution by comparing CCF values across convergent paths. Numerical simulations and sea trials demonstrate that HCCF-MSS-9 (9 iterations) achieves performance comparable to CCF-MSS-0.02 (±6 Hz range, 0.02 Hz precision) with superior computational efficiency. Under accelerations up to 3 m/s2, HCCF-MSS-9+MPGS-6 (6 starting points) attains a Doppler estimation mean squared error of approximately -3.3 dB, outperforming other algorithms by 0.5-1.5 dB, demonstrating its effectiveness for precise frequency offset estimation under complex variable-motion conditions.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1471-1488"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146180796","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Clément Larcade, Laetitia Roux, Charles Cröenne, Monique Pouille, Anne-Christine Hladky-Hennion
The measurement of acoustic performance of underwater panels, such as their reflection and transmission coefficients, has always been a challenge. The finite size of the tank imposes a low frequency limit, while diffraction by the edges of the panel disturbs measurements. Despite these difficulties, it remains a valuable tool for comparison with numerical and analytical studies. In a previous paper [Roux, Pouille, Audoly, and Hladky, J. Acoust. Soc. Am 147(2), 1104-1112 (2020)], the three-point method has been proposed and tested on a homogeneous panel. The present paper proposes an extension of the method applicable to periodic metamaterials. First, the applicability and robustness of the three-point method are tested on a periodic panel. Then, since it behaves like a diffraction grating, above the grating cut-off frequency, the measurement method must separate the specular wave from the other propagative contributions. For that purpose, the five-point method is proposed as a solution to separate these contributions to retrieve the reflection and transmission coefficients. The three- and five-point methods are applied to a test panel made of steel bars. Limitations on these methods are discussed and a solution is proposed to reduce their impact. Finally, a correct measurement-simulation agreement is observed for the reflection and transmission coefficients for both the specular and the first-propagative diffraction order.
水下板的声学性能的测量,如反射系数和透射系数,一直是一个挑战。水箱的有限尺寸施加了低频限制,而面板边缘的衍射会干扰测量。尽管存在这些困难,它仍然是与数值和分析研究进行比较的有价值的工具。在之前的一篇论文中[Roux, Pouille, Audoly, and Hladky, J. Acoust]。Soc。[Am 147(2), 1104-1112(2020)],已经提出了三点法并在均匀面板上进行了测试。本文提出了一种适用于周期性超材料的扩展方法。首先,在一个周期面板上测试了三点法的适用性和鲁棒性。然后,由于它的行为像衍射光栅,在光栅截止频率以上,测量方法必须将镜面波从其他传播贡献中分离出来。为此,提出了五点法作为分离这些贡献以检索反射和透射系数的解决方案。三点法和五点法分别应用于钢筋制成的测试板。讨论了这些方法的局限性,并提出了减少其影响的解决方案。最后,对镜面衍射级和第一传播衍射级的反射系数和透射系数进行了正确的测量和模拟。
{"title":"Experimental characterization of periodic metamaterials in acoustic open water tank.","authors":"Clément Larcade, Laetitia Roux, Charles Cröenne, Monique Pouille, Anne-Christine Hladky-Hennion","doi":"10.1121/10.0042401","DOIUrl":"https://doi.org/10.1121/10.0042401","url":null,"abstract":"<p><p>The measurement of acoustic performance of underwater panels, such as their reflection and transmission coefficients, has always been a challenge. The finite size of the tank imposes a low frequency limit, while diffraction by the edges of the panel disturbs measurements. Despite these difficulties, it remains a valuable tool for comparison with numerical and analytical studies. In a previous paper [Roux, Pouille, Audoly, and Hladky, J. Acoust. Soc. Am 147(2), 1104-1112 (2020)], the three-point method has been proposed and tested on a homogeneous panel. The present paper proposes an extension of the method applicable to periodic metamaterials. First, the applicability and robustness of the three-point method are tested on a periodic panel. Then, since it behaves like a diffraction grating, above the grating cut-off frequency, the measurement method must separate the specular wave from the other propagative contributions. For that purpose, the five-point method is proposed as a solution to separate these contributions to retrieve the reflection and transmission coefficients. The three- and five-point methods are applied to a test panel made of steel bars. Limitations on these methods are discussed and a solution is proposed to reduce their impact. Finally, a correct measurement-simulation agreement is observed for the reflection and transmission coefficients for both the specular and the first-propagative diffraction order.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1543-1554"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146213500","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
The Reflections series takes a look back on historical articles from The Journal of the Acoustical Society of America that have had a significant impact on the science and practice of acoustics.
《反思》系列回顾了《美国声学学会杂志》上对声学科学和实践产生重大影响的历史文章。
{"title":"The launch of statistical energy analysis simulation of double panels.","authors":"Alexander Peiffer","doi":"10.1121/10.0042351","DOIUrl":"https://doi.org/10.1121/10.0042351","url":null,"abstract":"<p><p>The Reflections series takes a look back on historical articles from The Journal of the Acoustical Society of America that have had a significant impact on the science and practice of acoustics.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"R3-R4"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146105971","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Matthew A Dzieciuch, Hanne Sagen, Peter F Worcester, Espen Storheim, F Hunter Akins, Stein Sandven, John A Colosi, John N Kemp, Geir Martin Leinebø
Acoustic signals with a center frequency of 35 Hz and a full bandwidth of about 4 Hz were transmitted over various ranges along a path extending from north of Svalbard to north of Alaska during the 2019-2020 US-Norwegian Coordinated Arctic Acoustic Thermometry Experiment (CAATEX). Three moorings were installed in the Canada Basin and three in the Nansen Basin, with one mooring in each basin hosting a source. All moorings had vertical receiving arrays, enabling spatial separation of the low-order acoustic normal modes. The modal group delays varied significantly over the year but were roughly consistent with predictions for the decade 2015-2022 based on the World Ocean Atlas 2023. The CAATEX signals traversed nearly the same trans-Arctic acoustic path as the 19.6-Hz signals in the 1994 Transarctic Acoustic Propagation (TAP) experiment. The TAP and CAATEX group delays cannot be directly compared because of the differing carrier frequencies. Thus, an indirect method using the group delays computed using WOA 2023 as a convenient standard was employed, but the large TAP mode-2 travel-time uncertainty precluded definitive comparisons. Nonetheless, CAATEX demonstrated that long-range acoustic transmissions provide precise, year-round measurements of large-scale ocean sound-speed (temperature) variability under the ice.
{"title":"Transarctic acoustic transmissions during the coordinated Arctic acoustic thermometry experiment in 2019-2020a).","authors":"Matthew A Dzieciuch, Hanne Sagen, Peter F Worcester, Espen Storheim, F Hunter Akins, Stein Sandven, John A Colosi, John N Kemp, Geir Martin Leinebø","doi":"10.1121/10.0042233","DOIUrl":"https://doi.org/10.1121/10.0042233","url":null,"abstract":"<p><p>Acoustic signals with a center frequency of 35 Hz and a full bandwidth of about 4 Hz were transmitted over various ranges along a path extending from north of Svalbard to north of Alaska during the 2019-2020 US-Norwegian Coordinated Arctic Acoustic Thermometry Experiment (CAATEX). Three moorings were installed in the Canada Basin and three in the Nansen Basin, with one mooring in each basin hosting a source. All moorings had vertical receiving arrays, enabling spatial separation of the low-order acoustic normal modes. The modal group delays varied significantly over the year but were roughly consistent with predictions for the decade 2015-2022 based on the World Ocean Atlas 2023. The CAATEX signals traversed nearly the same trans-Arctic acoustic path as the 19.6-Hz signals in the 1994 Transarctic Acoustic Propagation (TAP) experiment. The TAP and CAATEX group delays cannot be directly compared because of the differing carrier frequencies. Thus, an indirect method using the group delays computed using WOA 2023 as a convenient standard was employed, but the large TAP mode-2 travel-time uncertainty precluded definitive comparisons. Nonetheless, CAATEX demonstrated that long-range acoustic transmissions provide precise, year-round measurements of large-scale ocean sound-speed (temperature) variability under the ice.</p>","PeriodicalId":17168,"journal":{"name":"Journal of the Acoustical Society of America","volume":"159 2","pages":"1071-1085"},"PeriodicalIF":2.3,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146105996","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}