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Physically speaking, a minimally rotational wave undergoes the least attenuation, thus corroborating in part the importance of light spins.
The second objective is to create a rotational wave packet that aligns two directions specified by y = ±x simultaneously.
When small longitudinal oscillations are enabled, a rotational wave motion is established that this study attempts to analyse.
Opposite to this the rotational wave is strongly dispersive: its velocity increases proportionally to the wavelength, but marginally depends upon the propagation direction.
It is found that the 2D Cosserat continuum supports propagation of waves of three types: usual longitudinal and transverse (shear) waves and a new one – the rotational wave.
A prominent feature of the rotational wave is its extremely high velocity that can be considerably greater than the velocity of longitudinal wave propagating in the material of the layers.
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The classical topic of wave propagation in a rotating gas is revisited by deducing scalar wave equations for propagation of acoustic and rotational waves through a plug flow of gas in rigid-body rotation with arbitrary intensities of the radial stratification.
In the faster type, called longitudinal, dilational, or irrotational waves, the particle motion is in the same direction as that of wave propagation; in the slower type, called transverse, shear, or rotational waves, it is perpendicular to the propagation direction.
In comparison, the non-rotational wave with m = 0 is more radiative than any other rotational waves with m > 1 [32].
In microfluidics, rotational waves are utilized for determining fluid viscosity as well [36].
This high velocity can be used to distinguish the rotational waves.
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