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For general material laws and general finite element types a prediction of the wave speed and of the suitable grid size parameter leads to numerous case studies.
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The contact angle which is the angle on the contact interface between the liquid and solid is a popular index for expressing surface wettability of general materials such as metals, glasses, and resins [22].
The presented neural network learning method could be applied to other areas in materials science for accelerating general materials discovery and functional coating design.
The solutions derived here can serve as benchmark solutions for certain classes of anisotropic micropolar medium, and also can be used as an approximate solution for a micropolar medium with general material properties without any constraint conditions.
Unlike the commonly used perfectly matched layers (PML), the super-grid technique is stable for general anisotropic material, because it is based on a coordinate stretching combined with an artificial dissipation.
In the previous paper by Yu and Diab (2013), several sets of boundary integral equations are derived for general anisotropic materials and corresponding equations for materials with different classes of symmetry are deduced.
But it was only during the 1950s that these concepts found their way into the theory of constitutive relations for general viscoelastic materials; independently, a few years later, properly invariant stress rates were adopted in continuum formulations of elastic-plastic response.
An exact solution for general anisotropic materials under arbitrary uniform loading conditions is derived.
Explicit expressions for the elements of these four matrices are expressed in terms of elastic stiffness for general anisotropic materials.
Furthermore, we show how the coupling behavior of the four subproblems can be derived directly from the sparsity scheme of the stiffness tensor for general anisotropic materials.
In this paper, a solution procedure is presented for thermo-viscoelastic analysis of composites in a general form which can be used for general orthotropic materials with simple flat to complicated geometries with thickness change and curvature.
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