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SH0导波在粘接结构中传播时的相位变化

丁俊才 吴斌 何存富

丁俊才, 吴斌, 何存富. SH0导波在粘接结构中传播时的相位变化[J]. 力学学报, 2017, 49(1): 202-211. doi: 10.6052/0459-1879-16-245
引用本文: 丁俊才, 吴斌, 何存富. SH0导波在粘接结构中传播时的相位变化[J]. 力学学报, 2017, 49(1): 202-211. doi: 10.6052/0459-1879-16-245
Ding Juncai, Wu Bin, He Cunfu. THE PHASE SHIFT OF SH0 GUIDED WAVE PROPAGATING IN BONDING STRUCTURE[J]. Chinese Journal of Theoretical and Applied Mechanics, 2017, 49(1): 202-211. doi: 10.6052/0459-1879-16-245
Citation: Ding Juncai, Wu Bin, He Cunfu. THE PHASE SHIFT OF SH0 GUIDED WAVE PROPAGATING IN BONDING STRUCTURE[J]. Chinese Journal of Theoretical and Applied Mechanics, 2017, 49(1): 202-211. doi: 10.6052/0459-1879-16-245

SH0导波在粘接结构中传播时的相位变化

doi: 10.6052/0459-1879-16-245
基金项目: 

国家自然科学基金资助项目 1132002,11372016,51245001,51475012

详细信息
    通讯作者:

    吴斌, 教授, 主要研究方向:波动力学及其应用和无损检测新技术.E-mail:wb@bjut.edu.cn

  • 中图分类号: O347.4

THE PHASE SHIFT OF SH0 GUIDED WAVE PROPAGATING IN BONDING STRUCTURE

  • 摘要: 对粘接结构进行超声导波无损检测与评估是一个有挑战性的前沿性课题.针对此问题,研究了SH0导波在界面为理想连接的三层板状粘接结构中传播时的相位变化情况.首先基于波传播的控制方程,建立了粘接结构中反射和透射SH0导波相对于入射SH0导波的相位差解析模型.然后利用数值模拟计算了铝/环氧树脂/铝粘接结构中反射和透射SH0导波的相位差曲线.最后分析了入射角度和频厚积的变化对反射和透射SH0导波相位差的影响.结果表明,对于具体的粘接结构,反射和透射SH0导波在其中传播时的相位差变化主要依赖于入射角度、频率等参数.在特定的频厚积下,当声波水平入射时,反射和入射SH0导波同相位.无论入射角度为多大,随着频厚积的增大,反射SH0导波的相位差曲线均会产生周期性谐振.对于透射SH0导波,当声波垂直入射时,其相位差曲线的改变无规律可循;但是随着入射角度逐渐增大,透射SH0导波的相位差曲线逐渐变规则.所得结果可为实验时研究板状粘接结构中SH0导波的传播特性以及提取SH0导波回波中的有用信息和定位提供一定的理论指导.

     

  • 图  1  粘接结构中SH波传播模式

    Figure  1.  SH wave propagation model in bonding structure

    图  2  入射角度对SH0 导波相位差的影响

    Figure  2.  The effect of incident angle on the phase-difference of SH0 guided wave

    图  3  入射角为0° 时频厚积对SH$_{0}$ 导波相位差的影响

    Figure  3.  The effect of frequency-thickness product on the phase-difference of SH$_{0}$ guided wave when the incident angle is 0°

    图  4  入射角为30° 时频厚积对SH$_{0}$ 导波相位差的影响

    Figure  4.  The effect of frequency-thickness product on the phase-difference of SH$_{0}$ guided wave when the incident angle is 30°

    图  5  入射角为60° 时频厚积对SH$_{0}$ 导波相位差的影响

    Figure  5.  The effect of frequency-thickness product on the phase-difference of SH$_{0}$ guided wave when the incident angle is 60°

    图  6  入射角为0° 时频率、粘接层厚度与反射SH$_{0}$ 导波相位差之间的关系

    Figure  6.  The relationship between the frequency, the thickness of adhesive layer and the phase-difference of reflection SH$_{0}$ guided wave when the incident angle is 0°

    图  7  入射角为60° 时频率、粘接层厚度与反射SH$_{0}$ 导波相位差之间的关系

    Figure  7.  The relationship between the frequency, the thickness of adhesive layer and the phase-difference of reflection SH$_{0}$ guided wave when the incident angle is 60°

    图  8  入射角为0° 时频率、粘接层厚度与透射SH$_{0}$ 导波相位差之间的关系

    Figure  8.  The relationship between the frequency, the thickness of adhesive layer and the phase-difference of transmission SH$_{0}$ guided wave when the incident angle is 0°

    图  9  入射角为60° 时频率、粘接层厚度与透射SH0 导波相位差之间的关系

    Figure  9.  The relationship between the frequency, the thickness of adhesive layer and the phase-difference of transmission SH0 guided wave when the incident angle is 60°

    表  1  常见材料的物理性质

    Table  1.   Physical properties of common materials

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出版历程
  • 收稿日期:  2016-09-05
  • 修回日期:  2016-10-28
  • 网络出版日期:  2016-10-31
  • 刊出日期:  2017-01-18

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