Journal of Advanced Dielectrics, Volume. 12, Issue 6, 2241004(2022)

Influence of the prestressed layer on spherical transducer in sound radiation performance

Xiaofang Zhang1, Xiujuan Lin1, Rui Guo1, Changhong Yang1、*, Hui Zhao1、**, Mingyu Zhang2, Yan Wang2, Xin Cheng1, and Shifeng Huang1、***
Author Affiliations
  • 1Shandong Provincial Key Laboratory of Preparation and Measurement of Building Materials, University of Jinan, 336 Nanxinzhuang West Road, Jinan, Shandong 250022, P. R. China
  • 2Underwater Acoustic Transducer Lab, Shanghai Marine Electronic Equipment Research Institute, Shanghai 201108, P. R. China
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    To improve the acoustic radiation performance of the spherical transducer, a prestressed layer is formed in the transducer through fiber winding. The influence of the prestressed layer on the transducer is studied from the effects of the radial prestress (Tr) and acoustic impedance, respectively. First, a theoretical estimation of Tr is established with a thin shell approximation of the prestressed layer. Then, the acoustic impedance is measured to evaluate the efficiency of sound energy transmission within the prestressed layer. Further, the ideal effects of Tr on the sound radiation performances of the transducer are analyzed through finite element analysis (FEA). Finally, four spherical transducers are fabricated and tested to investigate their dependence of actual properties on the prestressed layer. The results show that with the growth of Tr, the acoustic impedance of the prestressed layer grows, mitigating the enormous impedance mismatch between the piezoelectric ceramic and water, while increasing attenuation of the acoustic energy, resulting in a peak value of the maximum transmitting voltage response (TVRmax) at 1.18 MPa. The maximum drive voltage increases with Tr, leading to a steady growth of the maximum transmitting sound level (SLmax), with a noticeable ascend of 3.9 dB at a 3.44 MPa Tr. This is a strong credibility that the prestressed layer could improve the sound radiation performance of the spherical transducer.To improve the acoustic radiation performance of the spherical transducer, a prestressed layer is formed in the transducer through fiber winding. The influence of the prestressed layer on the transducer is studied from the effects of the radial prestress (Tr) and acoustic impedance, respectively. First, a theoretical estimation of Tr is established with a thin shell approximation of the prestressed layer. Then, the acoustic impedance is measured to evaluate the efficiency of sound energy transmission within the prestressed layer. Further, the ideal effects of Tr on the sound radiation performances of the transducer are analyzed through finite element analysis (FEA). Finally, four spherical transducers are fabricated and tested to investigate their dependence of actual properties on the prestressed layer. The results show that with the growth of Tr, the acoustic impedance of the prestressed layer grows, mitigating the enormous impedance mismatch between the piezoelectric ceramic and water, while increasing attenuation of the acoustic energy, resulting in a peak value of the maximum transmitting voltage response (TVRmax) at 1.18 MPa. The maximum drive voltage increases with Tr, leading to a steady growth of the maximum transmitting sound level (SLmax), with a noticeable ascend of 3.9 dB at a 3.44 MPa Tr. This is a strong credibility that the prestressed layer could improve the sound radiation performance of the spherical transducer.

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    Xiaofang Zhang, Xiujuan Lin, Rui Guo, Changhong Yang, Hui Zhao, Mingyu Zhang, Yan Wang, Xin Cheng, Shifeng Huang. Influence of the prestressed layer on spherical transducer in sound radiation performance[J]. Journal of Advanced Dielectrics, 2022, 12(6): 2241004

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    Paper Information

    Category: Research Articles

    Received: Aug. 14, 2022

    Accepted: Oct. 16, 2022

    Published Online: Jan. 13, 2023

    The Author Email: Yang Changhong (mse_yangch@ujn.edu.cn), Zhao Hui (zhaohui0094@163.com), Huang Shifeng (huangshifeng_ujn@163.com)

    DOI:10.1142/S2010135X22410041

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