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    基于六端網絡法的壓電超聲換能器優化設計

    劉世杰 馮平法 查慧婷 馮峰

    劉世杰, 馮平法, 查慧婷, 馮峰. 基于六端網絡法的壓電超聲換能器優化設計[J]. 工程科學學報, 2022, 44(5): 933-939. doi: 10.13374/j.issn2095-9389.2020.11.24.008
    引用本文: 劉世杰, 馮平法, 查慧婷, 馮峰. 基于六端網絡法的壓電超聲換能器優化設計[J]. 工程科學學報, 2022, 44(5): 933-939. doi: 10.13374/j.issn2095-9389.2020.11.24.008
    LIU Shi-jie, FENG Ping-fa, ZHA Hui-ting, FENG Feng. Optimized design for a piezoelectric ultrasonic transducer based on the six-terminal network[J]. Chinese Journal of Engineering, 2022, 44(5): 933-939. doi: 10.13374/j.issn2095-9389.2020.11.24.008
    Citation: LIU Shi-jie, FENG Ping-fa, ZHA Hui-ting, FENG Feng. Optimized design for a piezoelectric ultrasonic transducer based on the six-terminal network[J]. Chinese Journal of Engineering, 2022, 44(5): 933-939. doi: 10.13374/j.issn2095-9389.2020.11.24.008

    基于六端網絡法的壓電超聲換能器優化設計

    doi: 10.13374/j.issn2095-9389.2020.11.24.008
    基金項目: 深圳市科技計劃基礎研究資助項目(學科布局)(JCYJ20180508152128308);深圳市科技計劃基礎研究資助項目(面上項目)(JCYJ20190813173607172)
    詳細信息
      通訊作者:

      E-mail: zhahuiting123@sz.tsinghua.edu.cn

    • 中圖分類號: TH122

    Optimized design for a piezoelectric ultrasonic transducer based on the six-terminal network

    More Information
    • 摘要: 壓電超聲換能器傳統四端網絡設計方法忽略了壓電陶瓷晶堆內部的機電耦合過程,使用該方法所設計的壓電超聲換能器尺寸誤差大,輸出的超聲振幅較小。為了提高壓電超聲換能器尺寸設計精度、增大換能器輸出的超聲振幅,本文將考慮壓電陶瓷晶堆內部機電耦合作用的六端網絡引入到壓電超聲換能器的設計中,分別采用四端網絡法和六端網絡法設計得到兩個不同尺寸的壓電超聲換能器A和B,通過有限元方法對比分析了兩個換能器的固有頻率和輸出振幅,并進一步通過實驗驗證了設計理論與仿真分析的有效性。研究結果表明,在相同激勵電壓下,采用六端網絡法設計得到的壓電超聲換能器B輸出的超聲振幅是換能器A輸出振幅的1.5倍,六端網絡法設計壓電超聲換能器可以提高所設計換能器的振動性能。

       

    • 圖  1  單一變截面桿及等其效四端網絡。(a)單一變截面桿;(b)等效四端網絡

      Figure  1.  Single rod with a variable cross section and its equivalent four-terminal network: (a) the rod; (b) the equivalent four-terminal network

      圖  2  壓電陶瓷晶堆的等效六端網絡

      Figure  2.  Equivalent six-terminal network of the SPCs

      圖  3  壓電超聲換能器結構

      Figure  3.  Structure of PUT

      圖  4  瞬態分析模型設置。(a)激勵施加方式;(b)前蓋板振動輸出點1

      Figure  4.  Model setup of the transient analysis: (a) application of the excitation voltage; (b) schematic illustration of point 1

      圖  5  換能器A和B端面點1處的輸出振幅仿真結果

      Figure  5.  Output amplitudes of transducer A and B at point 1 by FEM

      圖  6  壓電超聲換能器

      Figure  6.  Designed PUTs

      圖  7  壓電超聲換能器輸出位移測試

      Figure  7.  Experimental setup for measuring the displacement of the PUTs

      圖  8  換能器A和B端面輸出振幅實驗結果

      Figure  8.  Experimental results of the output amplitudes of transducer A and B

      表  1  壓電超聲換能器各部分材料參數

      Table  1.   Material parameters of each part of the PUT

      MaterialsDensity/
      (kg·m?3)
      Young’s modulus, E/
      (N·m?2)
      Poisson’s ratio
      Aluminum alloy 606127007.07×10100.33
      PZT-87600x: 7.407×1010xy: 0.303
      y: 8.696×1010yz: 0.356
      z: 8.696×1010xz: 0.322
      45 Steel78507.07×10110.31
      下載: 導出CSV

      表  2  壓電超聲換能器設計尺寸

      Table  2.   Designed dimensions of each part of the PUTs

      PartsLength/mmDiameter/mm
      Front cover58.6350
      piezoelectric ceramic slice6.550
      Cylindrical section of the back cover
      (four-terminal network method)
      9.9550
      Cylindrical section of the back cover
      (six-terminal network method)
      15.7850
      Conic section of back cover8Bottom surface: 50
      Top surface: 36
      Bolt1236
      下載: 導出CSV

      表  3  壓電超聲換能器縱振固有頻率仿真分析

      Table  3.   Natural frequency of the longitudinal vibration of the PUTs by FEM

      TransducerNatural frequency/HzDesign error/%Modal solution
      Transducer A200740.37
      Transducer B192703.65
      下載: 導出CSV
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    • 收稿日期:  2020-11-24
    • 錄用日期:  2022-01-05
    • 網絡出版日期:  2021-02-01
    • 刊出日期:  2022-05-25

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