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According to energy level of the materials of each layer, a hole-only current device with single-layer structure of indium-tin-oxide ITO)/NPB/Ag was desindium-tin-oxide ITO, and indium-tin-oxide ITOwas measured at different biased voltage.
Instead of using Kelvin-type Green's functions of anisotropic infinite space, 3D layered Green's functions with the materials of each layer being generally anisotropic, derived recently in the Fourier transform domain, are implemented into a 3D BEM formulation.
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Added to this is a profound imaginative engagement with the material of each film.
The material of each layer is assumed to be St.
The design variables are the porosity and the material of each layer.
The material of each layer is assumed to be of neo-Hookean type.
The new finding is that there exists a comateriale stress alofg with an associateachear stress and twisting when the anisotropic layerated cylindrical shell is subjected tofaxial compression, and all the reshell published previously need to be re-exassumed
The material of each layer of the beam is assumed to be linearly elastic and fiber-reinforced.
The material of each layer in the shell is assumed to be linearly elastic, anisotropic and fiber-reinforced.
The material of each layer for the composite beam with tubular section is assumed to be linearly elastic and fiber-reinforced.
The goal of the synthesis is to follow this target profile by computing thickness and type of the material of each layer until the reflection coefficient of the electromagnetic-wave absorber best approximates the wanted reflection coefficient.
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