Proceedings of the 2014 Symposium on Piezoelectricity, Acoustic Waves, and Device Applications 2014
DOI: 10.1109/spawda.2014.6998516
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Solid-state motion sensors on acoustic waves. Theory and experiment

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Cited by 4 publications
(7 citation statements)
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“…The authors note that a longitudinal wave propagating along the axis of rotation does not change its polarization, and a transverse wave is a combination of two circularly polarized waves with different velocities. This assumption was confirmed by a series of previous studies including a recent contribution by our research group [18,19].…”
Section: Introductionsupporting
confidence: 87%
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“…The authors note that a longitudinal wave propagating along the axis of rotation does not change its polarization, and a transverse wave is a combination of two circularly polarized waves with different velocities. This assumption was confirmed by a series of previous studies including a recent contribution by our research group [18,19].…”
Section: Introductionsupporting
confidence: 87%
“…For the first special case, several concepts were proposed, test models of the AMS SE were made and the experimental results confirmed the theoretical principles [18,19].…”
Section: Introductionmentioning
confidence: 89%
“…According to the expressions obtained by the authors earlier [ 16 , 17 ], in the presence of rotation, when the acoustic duct is exposed to centripetal and Coriolis accelerations, the phase velocity of CPAW is proportional to the rotation rate of the propagation medium, and depending on the direction of particles oscillation in waves (clockwise or counterclockwise), it either increases or decreases. As a result, when the set of CPAW propagates in a rotating medium, the displacement vector of the total linearly polarized wave rotates through an angle α proportional to the angular velocity and the wave propagation time, where V 0 is a total wave phase velocity without rotation.…”
Section: Theoretical Analysismentioning
confidence: 99%
“…According to the earlier calculations [ 16 , 17 ], the directions of particle motions in the emitted waves are the opposite. As a result, under rotation of the acoustic lines about the X -axis of CPAW propagation, the phase velocity of one of them receives a positive addition V 1 = V 0 /((1 + Ω/ω)), and the other—the negative one V 2 = V 0 /((1 − Ω/ω)).…”
Section: Experimental Researchmentioning
confidence: 99%
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