2013
DOI: 10.1063/1.4791711
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Reflection and transmission of Lamb waves at an imperfect joint of plates

Abstract: The reflection and transmission of Lamb waves at an imperfect joint of plates are analyzed numerically by the modal decomposition method and the hybrid finite element method. The joint is modeled as a spring-type interface characterized by distributed normal and tangential stiffnesses. The analysis is focused on a low-frequency range where the lowest-order symmetric and antisymmetric Lamb waves are the only propagating modes. The frequency-dependent reflection and transmission characteristics of these Lamb mod… Show more

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Cited by 32 publications
(40 citation statements)
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“…Recently, Mori et al [12] analyzed the reflection and transmission characteristics of Lamb waves at a butt joint of plates based on the spring-type interface model, which has been frequently used to analyze the interaction of ultrasonic waves with various imperfect interfaces [13][14][15][16][17][18][19][20][21][22]. They demonstrated that the reflection and transmission coefficients of the lowest-order symmetric (S0) and antisymmetric (A0) Lamb modes at the joint vary with the frequency and the interfacial stiffnesses.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, Mori et al [12] analyzed the reflection and transmission characteristics of Lamb waves at a butt joint of plates based on the spring-type interface model, which has been frequently used to analyze the interaction of ultrasonic waves with various imperfect interfaces [13][14][15][16][17][18][19][20][21][22]. They demonstrated that the reflection and transmission coefficients of the lowest-order symmetric (S0) and antisymmetric (A0) Lamb modes at the joint vary with the frequency and the interfacial stiffnesses.…”
Section: Introductionmentioning
confidence: 99%
“…31 In this approximation, the reflection and transmission coefficients of the extensional wave, jRj and jTj, are determined by the normalized parameter qc 1 x/K N ¼ (c 1 X)/(c T K) and do not depend on the tangential stiffness K T , where c 1 is the velocity of extensional waves in thin plates. In Fig.…”
Section: Reflection and Transmission Characteristics Of The S0 Modementioning
confidence: 99%
“…(9) serves as a measure of numerical errors such as the truncation error of the infinite series. 31,33 After some trials, the value of d was kept within 3.5% in the frequency range X ¼ xh/c T < X S1,S2 by setting the numerical parameters as N ¼ 7 and L ¼ 2.88 h (988 nodes and 900 elements). The out-of-plane (z direction) displacement amplitude at the corner of the free edge is plotted in Fig.…”
Section: B Setting Of Numerical Parametersmentioning
confidence: 99%
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