Amplitude modulation drive to rectangular-plate linear ultrasonic motors with vibrators dimensions 8 mm /spl times/ 2.16 mm /spl times/ 1 mm

In this paper, to exploit the contribution from not only the stators but also from other parts of miniature ultrasonic motors, an amplitude modulation drive is proposed to drive a miniature linear ultrasonic motor consisting of two rectangular piezoelectric ceramic plates. Using finite-element software, the first longitudinal and second lateral-bending frequencies of the vibrator are shown to be very close when its dimensions are 8 mm times 2.16 mm times 1 mm. So one single frequency power should be able to drive the motor. However, in practice the motor is found to be hard to move with a single frequency power because of its small vibration amplitudes and big frequency difference between its longitudinal and bending resonance, which is induced by the boundary condition variation. To drive the motor effectively, an amplitude modulation drive is used by superimposing two signals with nearly the same frequencies, around the resonant frequency of the vibrators of the linear motor. When the amplitude modulation frequency is close to the resonant frequency of the vibrator's surroundings, experimental results show that the linear motor can move back and forward with a maximum thrust force (over 0.016 N) and a maximum velocity (over 50 mm/s)

[1]  Neville H Fletcher,et al.  Principles of Vibration and Sound , 1994 .

[2]  Takeshi Morita,et al.  Miniature piezoelectric motors , 2003 .

[3]  Takaaki Ishii,et al.  Efficiency Improvement of an Ultrasonic Motor Driven with Rectangular Waveform , 1996 .

[4]  T. Hemsel,et al.  Survey of the present state of the art of piezoelectric linear motors , 2000, Ultrasonics.

[5]  Jean-François Manceau,et al.  Linear motor using a quasi-travelling wave in a rectangular plate , 1996 .

[6]  J. Wallaschek Contact mechanics of piezoelectric ultrasonic motors , 1998 .

[7]  Kouichi Kanayama,et al.  Multilayer Piezoelectric Motor Using the First Longitudinal and the Second Bending Vibrations , 1995 .

[8]  D Burkhoff,et al.  Maximizing hemodynamic effectiveness of biventricular assistance by direct cardiac compression studied in ex vivo and in vivo canine models of acute heart failure. , 2000, The Journal of thoracic and cardiovascular surgery.

[9]  R. Bansevicius,et al.  Vibromotors for Precision Microrobots , 1988 .

[10]  Meng-Shiun Tsai,et al.  Dynamic modeling and analysis of a bimodal ultrasonic motor. , 2003, IEEE transactions on ultrasonics, ferroelectrics, and frequency control.

[11]  G. Diana,et al.  The importance of rotor flexibility in ultrasonic traveling wave motors , 1998 .

[12]  E.A. Cheever,et al.  A versatile microprocessor-based multichannel stimulator for skeletal muscle cardiac assist , 1998, IEEE Transactions on Biomedical Engineering.

[13]  S. Ueha,et al.  Ultrasonic motors : theory and applications , 1993 .

[14]  M. Aoyagi,et al.  Ultrasonic Motors Using Longitudinal and Bending Multimode Vibrators with Mode Coupling by Externally Additional Asymmetry or Internal Nonlinearity , 1992 .

[15]  Takehiro Takano,et al.  A linearly moving ultrasonic motor using a longitudinal and bending multi-mode vibrator , 1990, [Proceedings] 1990 IEEE 7th International Symposium on Applications of Ferroelectrics.

[16]  Martin Levesley,et al.  Impedance control of a compression cardiac assist device , 2002, Proceedings of the International Conference on Control Applications.

[17]  K. Watterson,et al.  Performance improvement of rectangular-plate linear ultrasonic motors using dual-frequency drive , 2004, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.