2009
DOI: 10.1088/0964-1726/18/11/115024
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Characteristic analysis of a traveling wave ultrasonic motor using an ellipsoidal static contact model

Abstract: A characteristic analysis of an ultrasonic motor (USM) at the design stage has thus far been impossible. Therefore, a characteristic analysis method is suggested on the basis of a proposed model describing the complex nonlinear contact condition between the rotor and stator. The proposed contact model and analysis method can guide theoretical research on the minimization of the main disadvantages of the USM, which mainly result from the contact mechanism. The validity and usefulness of the suggested analysis m… Show more

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Cited by 16 publications
(7 citation statements)
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“…where B mg and B r are the magnetic flux and residual flux densities, respectively. The number of magnet poles is determined using equation (2) [29]- [31]:…”
Section: Design Methods For the Conventional And Proposed Afpmsmsmentioning
confidence: 99%
“…where B mg and B r are the magnetic flux and residual flux densities, respectively. The number of magnet poles is determined using equation (2) [29]- [31]:…”
Section: Design Methods For the Conventional And Proposed Afpmsmsmentioning
confidence: 99%
“…During piezoelectric coupling, electrical energy is converted to high-frequency mechanical vibration and during frictional coupling, the mechanical vibration is converted to the revolution of rotor. 9,19 However, the explanation of energy conversion is rough and not enough to explain the test results. The energy transfer process should be discussed.…”
Section: Energy Transfer Process In Twusmmentioning
confidence: 99%
“…The magnetic vector potential, A (Wb/m 2 ), can be calculated by solving (1) by the FEM while applying the boundary condition [20][21][22][23] ∇×n ∇× A = J 0 +∇× nm 0 M…”
Section: Analysis Of the Magneto-static Fieldmentioning
confidence: 99%
“…The magnetic vector potential, A(Wb/m 2 ), can be calculated by solving (1) by the FEM while applying the boundary condition [20–23]×ν)(×A=J0+×)(νμ0Mwhich is subject toν=μ0μnormalr1=μ01+χnormalm1where v (m/H) is the reluctivity, J0(A/m 2 ) is the external current density vector, μ 0 (H/m) is the permeability of the free space, M(A/m) is the residual magnetisation vector, and χ m is the magnetic susceptibility.…”
Section: Analysis and Design Of The Spmamentioning
confidence: 99%