nav emailalert searchbtn searchbox tablepage yinyongbenwen piczone journalimg journalInfo journalinfonormal searchdiv searchzone qikanlogo popupnotification paper paperNew
一种高频宽带压电叠堆换能器元器件研究
基金项目(Foundation): 广东省基础与应用基础研究基金资助项目(181003); 国家重点研发计划基金资助项目(2021YFB3702002)
邮箱(Email): 1052099473@qq.com;
DOI:
发布时间: 2026-05-11
出版时间: 2026-05-11
网络发布时间: 2026-05-11
移动端阅读
摘要:

基于有限元模拟仿真技术,对不同厚度压电陶瓷的品质因子Q、表面总声压、振型进行分析.选取厚度为2.5 mm和5.0 mm的陶瓷片,制备不同叠堆结构的2-2型多层压电复合材料.通过测试电学性能及导纳曲线,研究叠堆模型对换能器的阻抗(|Z|)、谐振频率(fs)和带宽的影响,并首次系统比较阶梯型与交替叠堆结构对多模态耦合的影响.结果表明,不同厚度压电陶瓷阶梯型叠堆更易引起多模态耦合,而交替叠堆多模耦合效果不明显.此外,树脂层厚度太大会形成阻尼,引起谐振频率(fs)降低,阻抗(|Z|)增大.适当厚度的陶瓷片和环氧树脂胶阶梯型叠堆复合,可以提高叠堆换能器的谐振频率,并保持带宽不衰减.当2.50 mm和5.00 mm厚的陶瓷片阶梯型叠堆复合,树脂层厚度为0.15 mm时,换能器的谐振频率提升至446.24 kHz,带宽基本保持不变为7.27 kHz.这为高频宽带水声换能器设计与制作提供一种参考.

Abstract:

Based on finite element simulation technology, the quality factor Q, total surface sound pressure and vibration mode of piezoelectric ceramics with different thicknesses were analyzed. Ceramic sheets with thicknesses of 2.50 mm and 5.00 mm were selected to fabricate 2-2 type multilayer piezoelectric composite with different stack structures. By testing electrical performance and admittance curve, the impact of the stack model on the impedance(, resonant frequency(fs) and bandwidth of the transducer was studied. The impact of stepped and alternating stacked structures on multi-modal coupling was compared systematically for the first time. The results showed that stepped stacks of piezoelectric ceramics with different thicknesses were more likely to cause multi-mode coupling, while the multi-mode coupling effect of alternating stacks was not obvious. In addition, an excessively thick resin layer introduces damping, leading to a decrease in resonant frequency(fs) and an increase in impedance(. The ladder-type stacking of ceramic sheets with appropriate thickness and epoxy resin glue would increase the resonant frequency of the stacked transducer and maintain the bandwidth without attenuation. When 2.50 mm and 5.00 mm thick ceramic sheets were stacked in a stepped manner and the resin layer thickness was 0.15 mm, the resonant frequency of the transducer increased to 446.24 kHz, and the bandwidth remained basically unchanged at 7.27 kHz. This provides a reference for the design and fabrication of high-frequency and broadband underwater acoustic transducers.

参考文献

[1]毛宇宸,沈建东,刘涛,等.基于压电超声换能器的被动声学发展及应用综述[J].压电与声光,2024, 46(5):617-633+643.

[2]叶鲜艳,王雪菲,许博成,等.超声换能器微机电系统的研究现状及发展趋势[J].微纳电子技术,2026, 63(1):30-39.

[3]HE Y S, WAN H T, JIANG X N, et al. Piezoelectric micromachined ultrasound transducer technology:Recent advances and applications[J]. Biosensors, 2023, 13(1):55.

[4]BIRJIS Y, SWAMINATHAN S, NAZEMI H, et al. Piezoelectric micromachined ultrasonic transducers(PMUTs):Performance metrics, advancements, and applications[J]. Sensors, 2022, 22(23):9151.

[5]MISHRA A K, JANANI KAVI PRIYA V S, PRADEEP K, et al. Smart materials for ultrasonic piezoelectric composite transducer:A short review[J]. Materials Today:Proceedings, 2022, 62:2064-2069.

[6]莫喜平.水声换能器发展中的技术创新[J].陕西师范大学学报(自然科学版),2018, 46(3):1-12.

[7]桑永杰.低频宽带水声换能器研究[D].哈尔滨:哈尔滨工程大学,2015.

[8]孔凡国,陈然然,段文科.高频医用超声换能器的研究现状及发展趋势[J].功能材料与器件学报,2015, 21(5):133-138.

[9]彭友霖,周艳红.医用超声换能器的现状与发展前景[J/OL].中华医学超声杂志(电子版),2009, 6(1):87-91.

[10]付丽媛,李发琪.高强度聚焦超声换能器[J].生物医学工程学杂志,2009, 26(3):667-670.

[11]张凯.高频宽带压电复合材料换能器研究[D].哈尔滨:哈尔滨工程大学,2011.

[12]鲜晓军,林书玉,王登攀,等.基于1-3-2型压电复合宽频带水声换能器研究[J].压电与声光,2014, 36(4):491-493+497.

[13]黄启国.高频宽带指向性可控的圆柱阵换能器的研究[D].北京:北京信息科技大学,2021.

[14]季博成.超宽带中高频换能器研究[D].哈尔滨:哈尔滨工程大学,2022.

[15]纪跃波,杨宇恒,蒙晨琛,等.一种压电换能器的动态阻抗匹配方法与频率跟踪[J].郑州大学学报(工学版),2025, 46(3):111-117.

[16]LEE D J, KWAK M S, KANG H Y. Design and development of a broadband ultrasonic transducer operating over the frequency range of 40 to 75 kHz[J]. Korean Journal of Fisheries and Aquatic Sciences, 2014, 47(3):292-301.

[17]JI B C, HONG L J, LAN Y. Ultra-wide operation band of the highfrequency underwater acoustic transducer realized by two-layer 1–3piezoelectric composite[J]. The Journal of the Acoustical Society of America, 2021, 150(5):3474-3484.

[18]魏博文.基于声谐振超声的宽频激励技术研究[D].沈阳:沈阳工业大学,2024.

[19]王颖颖.基于弛豫铁电单晶的超宽带纵振动换能器平面阵研究[D].哈尔滨:哈尔滨工程大学,2024.

[20]臧柳菲.弛豫铁电单晶水声发射换能器的带宽拓展研究[D].哈尔滨:哈尔滨工程大学,2024.

[21]BRUNGART D S, DAVIDSON A J. Transducer variability in speechin-noise testing:Considerations related to stimulus bandwidth[J].American Journal of Audiology, 2024, 33(3):1070-1076.

[22]YANG Y X, ZHU K, SUN E W, et al. Ultrabroad-bandwidth ultrasonic transducer based on Sm-doped PMN-PT ceramic/epoxy 1-3composite[J]. Sensors and Actuators A:Physical, 2022, 346:113873.

[23]苏晋涛,王宏伟.宽带高灵敏水声换能器的研究[J].压电与声光,2023, 45(5):759-768.

[24]魏彤,王宏伟,苏晋涛.一种高频宽带横向叠堆型换能器的研制[J].电子元件与材料,2024, 43(4):474-480.

[25]朱棵.基于声阻抗梯度匹配层的宽带高灵敏度超声换能器研究[D].哈尔滨:哈尔滨工业大学,2023.

[26]孙瑛琦.匹配层对1-3型压电复合材料聚焦换能器带宽影响的研究[D].重庆:重庆医科大学,2019.

[27]田欣.打孔型宽频带换能器的研究[D].哈尔滨:东北林业大学,2009.

[28]张军,李向东,任奕菲. PMN-PZT压电陶瓷的制备与电学性能研究[J].湖北理工学院学报,2022, 38(3):28-34.

[29]王晨青,马建敏.大功率夹心式压电换能器结构参数计算分析及设计[J].振动与冲击,2021, 40(4):130-137+220.

[30]董尊成.超声探伤用换能器中阻尼材料匹配的考虑[J].无损探伤,1996, 20(1):39-40.

基本信息:

中图分类号:TN384;TB565.1

引用信息:

[1]张军,罗福康,王祥达.一种高频宽带压电叠堆换能器元器件研究[J].西南民族大学学报(自然科学版)().

基金信息:

广东省基础与应用基础研究基金资助项目(181003); 国家重点研发计划基金资助项目(2021YFB3702002)

发布时间:

2026-05-11

出版时间:

2026-05-11

网络发布时间:

2026-05-11

引用

GB/T 7714-2015 格式引文
MLA格式引文
APA格式引文
检 索 高级检索