However, since in these applications multiple wave modes are generally generated and the individual modes are usually dispersive, the received signals are very complex and difficult to interpret.
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As the angle of skew is increased, the natural frequency parameters of the modes are generally increased.
The two nonpolar E 2 branches are Raman active only, and the B 1 modes are generally inactive in Raman spectra and are called silent modes [49].
Since low-frequency modes are generally dominant in a flexible system, only the lowest two bending modes have been considered for the implemented spacecraft model.
Since the distinction among the wave mode types of thermoelastic waves in anisotropic plates is somewhat artificial, as the elastic wave modes are generally coupled, they are referred to as quasi-longitudinal, quasi-transverse, and quasi-shear horizontal modes.
If the uniform source assumption held exactly, only two modes (corresponding to uniform source polarization parameters) would have power above the incoherent noise level; additional modes are generally indicative of source complications (either natural or anthropogenic).
The same methodology is also adopted to show that the contribution of higher modes is generally negligible in designing a supplemental damping system and that the required damping level can be typically obtained with a limited number of supplemental devices.
The modes are generally well extended, but are more complex than simple molecular pictures that are sometimes invoked, in some cases even revealing mixing among modes of different type.
Global buckling modes are generally regarded to have no post-buckling reserve, and indeed all column design curves, including those used in North America for cold-formed steel columns limit the strength to 0.877Pcre (where Pcre is the global buckling load) or lower.
