Titlebook: Anisotropic Elastic Plates; Chyanbin Hwu Book 2010 Springer-Verlag US 2010 Anisotropic elasticity.Boundary Element Analysis.Chyanbin Hwu.L

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https://doi.org/10.1007/978-3-030-96577-8prised that there are a great many constitutive laws describing an almost infinite variety of materials. What is surprising is that a simple idealized stress–strain relationship gives a good description of the mechanical properties of many elastic materials around us. In this chapter, we present the

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https://doi.org/10.1007/978-3-030-65200-5inear elastic solid. The difference is that Lekhnitskii formalism begins with the two-dimensional stresses, while Stroh formalism starts with the two-dimensional displacements. Due to this difference, Lekhnitskii formalism is in terms of the reduced elastic compliances while Stroh formalism to be pr

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https://doi.org/10.1007/978-3-030-65200-5kii formalism or Stroh formalism. Most of the works published in the earlier literature were based on Lekhnitskii formalism (1968). Due to the mathematical difficulties involved for the generalized two-dimensional problems, when employing Lekhnitskii formalism one usually considers the state of gene

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https://doi.org/10.1007/978-981-10-0545-9liptic shape and its geometric limits such as circles and cracks have evoked the most interest among researchers. If the stress concentration is of more concern, the optimization in a class of hole shapes has shown that the optimized hole is not necessarily the elliptic type. However, due to the req

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Road Capacity with Efficient Tollsabilities are increasingly becoming important. It is well known that piezoelectric materials produce an electric field when deformed and undergo deformation when subjected to an electric field. Because of this intrinsic coupling phenomenon, piezoelectric materials are widely used as the sensors and

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