Received: date / Accepted: date 7 Abstract The phononic band structure of waves, which travel though composites, result from the geo-8 metric and mechanical properties of the materials and from the interaction of the different constituents.
9In this article, we study two different models to simulate imperfect bonding and their impact on the 10 phononic bands: (a) imperfect bonding is simulated by introducing an artificial interphase constituents 11 with properties which define the bonding quality; (b) imperfect bonding is described by conjugate 12 conditions in the interface, in which the difference in the displacement is proportional to the interfacial 13 stress. Viscoelastic behavior of the constituents has a crucial influence on the traveling signal, and the 14 wave attenuates with increasing viscosity. We study the interaction of the different bonding conditions properties of composites with coatings between fibers and the matrix over composites with uncoated 23 fibers after high temperature production.
24Imperfect bonding between components plays a crucial role in the functionality and reliability 25 of composites, and it might result from the lack of adhesion between the constituent and cracks.
26Imperfect bonding might also result from corrosion, as discussed in the work of Germain & Pamin
27[16]. In mechanical modeling, there exist different approaches to describe such imperfect conditions.
28One example is the so-called spring layer model, in which the differences in the displacements at the 29 common interface of two constituents are proportional to the stress in the interface. In the case of one-dimensional problems, e.g., for layered composites, it is usually possible to derive 57 the exact dispersion equations [7, 40]. In the case two-dimensional and three-dimensional problems, Another widely used approach to study wave propagation in periodic media is the finite difference time 64 domain method (see, for instance, the paper [35] and cited references therein).
65One of the first papers to discuss wave propagation in composites and the resulting frequency band example by the plane-wave expansion method, which will be treated in Sec. 4.
118The composite structure is periodically repeating and possessing layers of finite thickness in x-119 direction. The wave equation for a shear wave propagation in x-direction at time t has the form 120