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The power dominates in higher-order modes for cases (a), (b), (d) and (f).
The power is coupled predominantly in higher-order modes for cases (c), and (e).
Moreover, the curve of the channel impulse response is left-skewed with power dominating higher-order modes for cases Fig. 4(c), (d), and (e).
Moreover, the radiative and nonradiative powers of bi-dipole interacting with GNR at these induced odd/even modes for cases of φ = 0/180° are nearly four times the corresponding values for the cases of a single dipole.
For the triangular plate with apex angle (β = 60°), it is noted that the second and third modes are double modes for cases purely metal or purely ceramic, but varied the volume fraction exponent there is a small spacing between the two modes, the maximum spacing is the round of n = 1.
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Provisions for alternate operational modes for specific cases are included in the design.
Analytical predictions of natural frequencies, modal loss factors and complex modes for all cases are in excellent agreement with modal measurements.
Anyway, it has been shown that the overestimation can be alleviated by using a formulation with more modes for these cases.
On the contrary, the spontaneous ignition mode prevails for cases with small T′ or ϕ′, especially for cases with negative T ϕ correlations, and hence, simultaneous auto-ignition occurs throughout the entire domain, resulting in an excessive rate of heat release.
The GYSELA code is found to be stable over long simulation times (more than 20 times the linear growth rate of the most unstable mode), including for cases with a high resolution mesh (δr ∼ 0.1 Larmor radius, δz ∼ 10 Larmor radius).
This paper also examines the convergence of the POD and DMD modes for this case.
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