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Damping estimates of the fundamental modes increased with the increase of accelerations, while characteristics of mode-shapes were also found to be dependent on the wind speed.
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In addition, it is observed that the number of lasing peaks (i.e., random modes) increases with the reduction of θ.
The phase velocity of all modes increases with plasma frequency.
Separation of the pair orthogonal modes increases with growth of the eccentricity of the elliptical core.
As seen in these figures, the frequencies of all modes increase with plasma frequency for 0.5 < k < 0.8.
From the mentioned figures, it is clear that the phase velocity of four modes increases with the plasma density for 1.3 GHz < f < 2.4 GHz.
The frequencies of all modes increase with plasma frequency and the order of these frequencies is ωX-X > ωX-O > ωO-X > ωO O.
The zero solution is unstable versus modes with (vert kvert L c (the number of such modes increases with L).
Results indicate that the frequency and the phase velocity of (X bp − X p ) and (O bp − X p ) modes increase with cyclotron frequency and for (O bp − O p ) and (X bp − O p ) modes decrease.
Since the structural periods corresponding to the first few vibration modes increase with the increase of scour depth, this study finds that the sensitivity of the periods to the scour depth varies for different types of bridges.
From Fig. 7a and d, the phase velocity of (X bp − X p ) and (O bp − X p ) modes increases with the cyclotron frequency for 0.8 GHz < f < 2.8 GHz and Fig. 7b and c shows that the phase velocity of (O bp − O p ) and (X bp − O p ) modes decreases with the cyclotron frequency, for 1.9 GHz < f < 2.3 GHz.
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