粘弹性材料包覆弹性板中剪切水平波传播特性研究

F. Simonetti, P. Cawley
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引用次数: 44

摘要

利用远程超声导波无损检测技术检测金属结构的衰减层是一种极具吸引力的方法。然而,材料的阻尼可能会导致声信号的严重衰减,从而导致测试范围的缩小。本文研究了剪切水平波在涂有粘弹性层的金属板中传播时的频散问题。结果表明,如果粘弹性层夹紧在粘弹性层的下表面,双层模态可以看作是自由弹性板模态与粘弹性层模态之间的相互作用。对于低衰减材料,相互作用强,随着频率的增加,两族之间的双层色散曲线轨迹跳变。然而,随着材料阻尼的增加,相互作用变弱,大部分能量被限制在金属板或衰减层中,模态不再跳变。导波衰减与粘弹性层中每单位面内功率流的应变能通过能量平衡的方式联系起来。能量主要在弹性板中传播的模态的导波衰减在频域中呈现周期性峰值,这些峰值出现在间隔大致相等的临界频率处。这些频率接近无夹紧粘弹性层的全厚度共振频率,如果它被认为是弹性的。导波衰减的最小值出现在洛夫跃迁频率附近。
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On the nature of shear horizontal wave propagation in elastic plates coated with viscoelastic materials
The possibility of using long–range ultrasonic guided–wave non–destructive testing for the inspection of metallic structures coated with attenuative layers is extremely attractive. However, the material damping may cause severe attenuation of the acoustic signal, resulting in reduction of the test range. This paper addresses the dispersion of shear horizontal waves propagating in metallic plates coated with viscoelastic layers. It is shown that the bilayer modes can be viewed as an interaction between the free elastic plate modes and the modes of the viscoelastic layer if it were clamped on its lower surface. For low–attenuation materials the interaction is strong and the trajectories of the bilayer dispersion curves jump between the two families as the frequency increases. However, as the material damping increases the interaction becomes weak and most of the energy is confined in either the metallic plate or in the attenuative layer, and modes no longer jump. The guided–wave attenuation is related to the strain energy in the viscoelastic layer per unit in–plane power flow by means of an energy–balance argument. The guided–wave attenuation of the modes whose energy travels primarily in the elastic plate exhibits periodic peaks in the frequency domain, which occur at roughly equally spaced critical frequencies. These frequencies are close to the through–thickness resonance frequencies of the clamped–free viscoelastic layer if it is considered to be elastic. Minima of the guided–wave attenuation occur around the Love transition frequencies.
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