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The results show the influence of these modes and amplitudes on the resistance to patch loading.
The dispersion curves for symmetric and antisymmetric thermoelastic wave modes and amplitudes of displacement and temperature change in case of fundamental symmetric (S0) and skew symmetric (A0) modes are presented in order to illustrate and compare the theoretical results.
In the following simulations we use this simulated 2-D signal (y sim ) with the same modes and amplitudes, we only change the SNR value.
Application of the three dimensional Gaussian Axial Fluctuation (3DGAF) model to Ub 22 resulted in dynamic modes and amplitudes that were in good agreement with those determined by comparison to restraint-free accelerated MD (AMD) simulation.
The similarity between the results derived from the two very different approaches, in one case fitting motional modes and amplitudes to the experimental data using mathematical models, and in the other case comparing to restraint free MD simulation, is striking, and substantiates assumptions implicit to both approaches.
Independent analyses of RDCs, using analytical fitting of the mean orientation and associated modes and amplitudes of each peptide plane, or comparison with restraint-free AMD simulation, resulted in a comprehensive and remarkably convergent description of multi-timescale dynamics in this protein.
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For multiple parallel filled joints, the variation trend of the transmission coefficient versus the dimensionless joint spacing is similar to the analytical result obtained by Zhu et al. (2011) except that the loading mode and amplitudes have an important effect on the magnitude of the transmission coefficient.
Experimental results show the existence of 1 3 and 1 2 3 external and internal resonances, energy transfer from high-frequency modes to the first mode, and amplitude- and phase-modulation among several modes.
These differences alter the propagation conditions of different PW modes and their amplitudes (see Figs. 3c and 4c) and EP-fluxes (see Figs. 5c and 6c) at middle and high altitudes.
In order to settle this question we have performed experimental measurements of flexural normal-mode frequencies and amplitudes which are much more precise than what has been obtained up to now.
The properties of the vibration modes of the transducer, such as mode frequencies and amplitude ratios of the mode shapes, are determined following Galerkin method.
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