弹性板倾斜端面兰姆波模态转换研究

Z. Minghui, Sun Hui, S. Tielin, Chen Wenjian, Zhang Tian-hang
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引用次数: 1

摘要

水下目标声散射是水声研究的一个重要方面。弹性散射波的研究与波的色散曲线和出射角有关,但在弹性板的背景下很少讨论兰姆波的激发条件。在弹性板的端面反射形成其他反对称模的兰姆波时,几种模式的反射兰姆波的能量分布也很少被讨论。然而,集中研究兰姆波的激励条件和水下弹性板端面的模态转换可以作为目标识别的基础。基于R.D. Mindlin Hamilton原理,利用正交完全特征,导出了真空中弹性板兰姆波的频散方程;得到了水、相速度、衰减系数和群速度色散曲线。分析了单模态下,在平板端面入射一个反对称兰姆波时,由模式转换引起的两个反对称模式后向兰姆波之间的能量比。实验测量了水下弹性板的散射波,结果表明,只有在某一模态的临界角处入射的反对称Lamb波才能在弹性板中直接激发出该模态的Lamb波,其他反对称模态的Lamb波都是在弹性板的端面反射形成的。对称兰姆波和反对称兰姆波之间也没有能量变化,即使有模式转换,如果波在弹性板的末端反射。结合水下弹性板的辐射效率,对单模态下入射到板端面的反对称兰姆波发生模态转换后产生的反对称兰姆波能量比进行分析,验证了分析结果的有效性。
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Research on mode conversion of lamb wave at dip end face of elastic plate
Underwater target acoustic scattering is an important aspect of underwater acoustic research. Research on the elastic scattering wave is related to the wave dispersion curves and the exit angle, but the excited condition of a Lamb wave is rarely discussed in the context of elastic plates. The energy distribution for the reflected Lamb waves of several modes when Lamb waves of other anti-symmetric modes are formed by reflection at the end face of an elastic plate is also rarely discussed. However, the research concentrating on the excitation condition of Lamb waves and mode conversion at the end face of a submerged elastic plate can be the basis for target recognition. Based on R.D. Mindlin Hamilton's principle and using an orthogonal complete feature, the frequency dispersion equation of a Lamb wave is derived for an elastic plate in a vacuum; and water, phase velocity, attenuation coefficients and group velocity dispersion curves are obtained. Analysis of the energy ratio between each of two anti-symmetric mode backward Lamb waves resulting from mode conversion when an anti-symmetric Lamb wave is incident at the end face of the plate in single mode is derived. The scattering wave of a submerged elastic plate is measured experimentally, which shows that only the incident anti-symmetric Lamb wave at the critical angle of one mode can directly excite a Lamb wave of this mode in the elastic plate, Lamb waves of other anti-symmetric modes are formed by reflection at the end face of the elastic plate. There is also no energy change between a symmetric Lamb wave and an anti-symmetric Lamb wave, even with mode conversion, if the waves are reflected at the end of the elastic plate. Combined with radiation efficiency of submerged elastic plate energy ratio between each two anti-symmetric mode backward lamb waves resulted from mode conversion when anti-symmetric lamb wave incident at the end face of plate in single mode confirmed validity of the analysis results.
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