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弯张换能器的尺寸远小于波长, 从而阻碍了紧凑型水声换能器产生定向波束. 针对传统的指向性弯张换能器电路驱动的幅度相位调控的复杂性问题, 本文提出一种指向性弯张换能器结构, 采用外凸型弯曲梁与内凹型弯曲梁复合而成的非对称壳体结构实现低频指向性发射, 可简化换能器的配套电路系统, 便于应用且成本更低. 本文从换能器的振动和辐射特性分析入手, 揭示了指向性形成机理并建立了等效双球源模型. 采用数值模拟的方法分析了主要结构参数对换能器谐振频率、发送电压响应、前后声压比及指向性的影响. 通过优化设计, 换能器在1240—1660 Hz的工作频段内最大发送电压响应为145.9 dB, 可在单电路驱动下产生前后声压比最大27 dB的心型指向性波束, 并且大大降低了有源材料的剪切应力, 可有效避免大功率发射时有源材料的疲劳失效, 为低频水声定向发射提供了一种更便捷的方法.The dimensions of flextensional transducers are much smaller than the wavelength, thereby hindering the generation of directional beams by compact underwater acoustic transducers. To address the complexities of amplitude and phase modulation in circuit-driven traditional directional flextensional transducers, a directional flextensional transducer structure is proposed in this work. By implementing an asymmetric composite shell configuration combining concave and convex curved beams, the low-frequency directional radiation is achieved while simplifying peripheral driving circuits, thereby improving the operational convenience and cost-effectiveness. Through an analysis of the vibration characteristics and radiation mechanisms, this study elucidates the principle of directional generation. The concave and convex beams of the flextensional transducer exhibit an intrinsic operational characteristic of opposite-phase normal displacement in their vibration modes. By adjusting structural parameters, the amplitude output from the two beams under a single actuator drive can satisfy a specific differential relationship, effectively resulting in the modal superposition of a monopole and a dipole, thereby achieving directional radiation. By using a Lorentzian resonance fitting function and a linear fitting function, the relationship between the frequency-dependent amplitude ratio and phase difference of sound pressure for the concave and convex beams is established, forming an unequal amplitude, unequal phase dual-spherical source radiation model for the transducer, thereby providing a theoretical framework for controlling the directivity of the transducer. Through numerical simulations, the effects of the transducer sidewall parameters, as well as the thicknesses and curvature radii of the concave and convex beams, on the transducer’s resonance frequency, transmitting voltage response, front-to-back sound pressure ratio, and directivity are analyzed. Sensitivity ranking of the structural parameters is also presented. Finally, the optimization of transducer’s performance is discussed and compared with that in other existing research, showing the advantages of this design. Specifically, the transducer achieves a maximum transmitting voltage response of 145.9 dB within the operating frequency band from 1240 Hz to 1660 Hz. Under single-circuit drive, a cardioid-shaped directional beam with a maximum front-to-back sound pressure ratio of 27 dB is produced. Furthermore, the shear stress on the active material is significantly reduced, effectively preventing fatigue failure of the active material during high-power emission. This provides a more convenient method for achieving low-frequency underwater acoustic directional emission.
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Keywords:
- flextensional transducer /
- low-frequency directional beam /
- cardioid directivity /
- modal coupling
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图 3 换能器在(a)空气中和(b)水中的凹凸梁辐射面中心点法向位移
Fig. 3. Normal displacement at the center of the radiating surface of the arched beam for the transducer in (a) air and (b) water.
图 4 换能器水中凹侧和凸侧距离声中心10 m处的(a)声压及(b)相位频响曲线
Fig. 4. (a) Sound pressure and (b) phase frequency response curves at 10 m from the acoustic center for the concave and convex sides of the transducer in water.
图 5 凹凸梁型低频指向性弯张换能器等效双球源模型
Fig. 5. Equivalent dual-spherical source model of the concave-convex beam low-frequency directional flextensional transducer.
图 6 侧壁长度$ l $ 对换能器的影响 (a) TVR; (b) FBR; (c) 最大指向性
Fig. 6. Effect of sidewall length $ l $ on the transducer: (a) TVR; (b) FBR; (c) maximum directivity.
图 7 侧壁宽度$ w $对换能器的影响 (a) TVR; (b) FBR; (c) 最大指向性
Fig. 7. Effect of sidewall width $ w $ on the transducer: (a) TVR; (b) FBR; (c) maximum directivity.
图 8 侧壁高度 $ h $对换能器的影响 (a) TVR, (b) FBR; (c) 最大指向性
Fig. 8. Effect of sidewall height $ h $ on the transducer: (a) TVR; (b) FBR; (c) maximum directivity.
图 9 凸梁曲率半径$ {r}_{1} $对换能器的影响 (a) TVR; (b) FBR; (c) 最大指向性
Fig. 9. Effect of convex beam curvature radius $ {r}_{1} $on the transducer: (a) TVR; (b) FBR; (c) maximum directivity.
图 10 凸梁厚度 $ {t}_{1} $对换能器的影响 (a) TVR; (b) FBR; (c) 最大指向性
Fig. 10. Effect of convex beam thickness $ {t}_{1} $on the transducer: (a) TVR; (b) FBR; (c) maximum directivity.
图 11 凹梁曲率半径$ {r}_{2} $ 对换能器的影响 (a) TVR; (b) FBR; (c) 最大指向性
Fig. 11. Effect of concave beam curvature radius $ {r}_{2} $on the transducer: (a) TVR; (b) FBR; (c) maximum directivity.
图 12 凹梁厚度 $ {t}_{2} $对换能器的影响 (a) TVR; (b) FBR; (c) 最大指向性
Fig. 12. Effect of concave beam thickness $ {t}_{2} $on the transducer: (a) TVR; (b) FBR; (c) maximum directivity.
图 13 (a) 换能器z方向和y方向的TVR曲线对比; (b) 换能器在1480 Hz处的xy平面和xz平面指向性图; (c) 换能器xy平面示意图; (d) 换能器xz平面示意图
Fig. 13. (a) Comparison of TVR curves in the z-direction and y-direction of the transducer; (b) directivity patterns in the xy-plane and xz-plane at 1480 Hz; (c) schematic diagram of the xy-plane of the transducer; (d) schematic diagram of the xz-plane of the transducer.
图 14 (a) 优化后的换能器凹侧、凸侧、z方向、y方向的TVR曲线; (b) 1480 Hz处的指向性图
Fig. 14. (a) TVR curves of the concave side, convex side, z-, and y-directions of the optimized transducer; (b) directivity pattern at 1480 Hz.
图 15 (a) 优化后的换能器空气中导纳曲线; (b) 优化后的换能器水中导纳曲线
Fig. 15. (a) Admittance curve of the optimized transducer in air; (b) admittance curve of the optimized transducer in water.
图 16 (a) 优化后的换能器和传统Ⅳ型、Ⅶ型弯张换能器的TVR对比; (b)优化后的换能器和传统采用双激励法实现低频指向性的Ⅳ型弯张换能器的压电振子径向位移对比
Fig. 16. (a) Comparison of TVR between the optimized transducer and traditional Class IV and Class VII flextensional transducers; (b) comparison of radial displacement of piezoelectric vibrators between the optimized transducer and the traditional Class IV flextensional transducer achieving low-frequency directivity using dual-drive excitation.
表 1 换能器结构参数优化范围
Table 1. Optimization range of the transducer structure parameters.
参数 取值范围/mm 步长/mm $ l $ 155—170 5 $ w $ 130—160 10 $ h $ 35—50 5 $ {r}_{1} $ 150—300 50 $ {t}_{1} $ 6—12 2 $ {r}_{2} $ 150—300 50 $ {t}_{2} $ 6—12 2 
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表 2 换能器优化后的结构参数
Table 2. Structural parameters of the transducer after optimization.
参数 值/mm 参数 值/mm $ l $ 160 $ {t}_{1} $ 7 $ w $ 160 $ {r}_{2} $ 300 $ h $ 40 $ {t}_{2} $ 13 $ {r}_{1} $ 200 换能器总高度 236
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