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As it follows from analysis of x3-x2-CDA modes for boundary 5 0 and 0 5 nanocomposites, unique As4S4-related trapping sites are rather o-Ps traps with τ int = 0.875 ns, which can be ascribed (due to bulk positron lifetime τ b ≈ 0.271 ns essentially increased in respect to τ b ≈ 0.223 ns proper for realgar α-As4S4 [19]) to interfacial TJ in a random network of loose-packed As4S4 NP (see Fig. 1a).
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Where φ is the fundamental mode shape for boundary conditions of beam and Ω is the dimensionless natural frequency.
First, we used PCA to measure the main modes of boundary motion.
Newton's method is used to find the complex wavenumbers of radial modes for the absorption boundary condition.
Frequency values have been given for different material and geometric parameters, modes and boundary cases for circular cylindrical panels with FGM and CNTR cases.
Then, using the DQ and DSC methods, the frequencies values have been calculated for different material and geometric parameters, modes and boundary cases for truncated conical panels with FGM.
The present method is based on the basic elasticity equations of the plate, and can give the symplectic analytical solutions for the wave modes for any combination of simple boundary conditions along the plate edges.
Both the primary and combination instability regions for various natural modes and boundary conditions are obtained numerically.
The resonance and antiresonance frequencies and the vibrating modes are calculated for the various resonance modes and boundary conditions, and the results are compared with those by the three-dimensional finite element methods.
Similar stability curves are obtained for each mode for these different boundary conditions.
In view of arriving at synthetic response and validate the assumptions that BSR works as mode conversion boundary we for the first time generate seismic reflections data and identify different conversion modes in relation gas hydrate exploration.
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