A threeDOF ultrasonic motor using four piezoelectric ceramic plates in bondedtype structure
Jipeng Yan^{1} , Yingxiang Liu^{2} , Shengjun Shi^{3} , Weishan Chen^{4}
^{1, 2, 3, 4}State Key Laboratory of Robotics and System, Harbin Institute of Technology, Harbin, China
^{2}Corresponding author
Journal of Vibroengineering, Vol. 20, Issue 1, 2018, p. 358367.
https://doi.org/10.21595/jve.2017.18523
Received 21 April 2017; received in revised form 22 October 2017; accepted 1 November 2017; published 15 February 2018
JVE Conferences
A threeDOF ultrasonic motor is presented in this paper. The proposed motor consists of four piezoelectric ceramic plates and a mental base with a flange that can fix the motor on a rack. The proposed motor takes advantage of a longitudinal mode and two bending modes, different hybrids of which can realize threeDOF actuation. Because of symmetric structure of the proposed motor, the resonance frequencies of the two bending modes are identical. And the resonance frequency of the longitudinal mode was tuned closed to the ones of the bending modes by adjusting the structural parameters in modal analysis. Then trajectories of nodes on the driving foot were obtained by the transient analysis to verify the feasibility of driving principle. Experiments including vibration shape test and output characteristic test were executed. The starting voltages of the rotation along horizontal axes are about 10 Vpp. Under driving voltages of 200 Vpp, the output velocities of three DOF can reach 280 rpm, 277 rpm and 327 rpm, respectively. The results of the experiments indicate that the proposed motor is characterized by low starting voltages and high output velocities.
Keywords: ultrasonic motor, three degrees of freedom, longitudinal mode, bending mode.
1. Introduction
Because ultrasonic motors exhibit some merits, such as quick response, high position accuracy, selflocking when power off and nonelectromagnetic radiation, they have replaced many electromagnetic motors in several fields such as MEMS (Microelectromechanical Systems), high precision machines and micro robots. Ultrasonic motors work on the principle that alternative electricity can be converted to mechanical vibration via converse piezoelectric effect of the piezoelectric elements, and the vibration of the stator can generate elliptical or oblique movement on the driving foot, and this movement can be converted into the continuous motions via frictional coupling on the interface between the runner and the stator [15].
According to the type of the output motion, ultrasonic motors can be classified into linear type, rotary type and multiDOF one. The linear actuation of ultrasonic motors can be realized by the hybrid of two independent vibration modes, such as a bending and a longitudinal vibration modes [610], two bending vibration modes and two longitudinal modes [1114]. The rotary actuation is usually realized by a traveling wave in a ringtype or cylindertype stator and can also be realized by the hybrid of two vibration modes [1519]. The multiDOF ultrasonic motors need the ability of actuations in several directions. And some of them can realize rotary driving in three different directions. The threeDOF ultrasonic motor proposed by Hoshina et al. [20] consists of three annular stators, each of which uses one traveling wave. The threeDOF ultrasonic motor proposed by Ishii et al. [21] consists of two Langevin transducers, each of which uses multi modes. The threeDOF ultrasonic motor proposed by Shen et al. [22] consists of four symmetric piezoelectric pusher elements, each of which uses three vibration modes. These three ultrasonic motors consist of at least two stators to realize the threeDOF actuations, which makes them much complex to be fabricated. On the other side, ultrasonic motors consist of a single stator have been studied and proposed [2325]: the ultrasonic motor proposed by Khoo et al. [23] is bonded type, whereas the ultrasonic motors proposed by Takemura et al. and Li et al. [2425] belong to the boltclamped type. And the former type is more easily to be fabricated and miniaturized than the latter one. The proposed motor in this paper can realize threeDOF actuations by only one single bondedtype stator, which can reduce the volume and mass of the motor. Because the frequencies of vibration modes this motor used are easy to be tuned closed, it is convenient to adjust the dimensions of the motor to be apply it in different situations, such as driving the ‘eyes’ of a robot.
2. Actuator concept
In order to realize threeDOF actuation, the proposed motor is designed to use different hybrids of three vibration modes: a longitudinal vibration mode and two orthogonal bending vibration modes.
2.1. Geometry
The structure of the proposed motor is shown in Fig. 1. The proposed motor consists of four pieces of piezoelectric ceramic plates and a metal base as shown in Fig. 1(a). It can be seen in Fig. 1(b) that the metal base is an integration of a cuboid to be attached with piezoelectric ceramic plates and a flange with eight holes to fix the motor on a rack. There is a throughhole in the metal base to tune the resonance frequencies of three vibration modes and to work as a driving foot. The polarization directions and serial numbers of the piezoelectric ceramic plates are shown in Fig. 1(c). These four pieces of piezoelectric ceramic plates are all polarized along the direction of thickness and each two parallel piezoelectric ceramic plates are polarized in same direction. Thus, the hybrid of two bending vibration modes can be excited by two driving signals. The hybrid of the longitudinal and a bending vibration mode need three driving signals.
Fig. 1. The structure of the proposed motor: a) the threedimensional model of the proposed stator, b) the metal base of the proposed motor, c) the polarizations of PZT ceramics
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b)
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2.2. Driving principle
The first order longitudinal vibration mode and two second order bending vibration modes are selected and their mode shapes are shown in Fig. 2(a), (b) and (c), respectively. The proposed motor will be excited by two or three driving signals shown in Fig. 3, with the metal base connected to ground. It can be seen from the Fig. 3 that there is a phase shift of 90 degrees between signal1 and signal2; the voltage change of signal3 is converse with the one of signal1.
Fig. 2. Selected vibration modes of the proposed motor: a) the first order longitudinal vibration mode, b) the second order bending vibration mode, c) the second order bending vibration mode
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b)
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Fig. 3. Driving signals of the proposed motor
The proposed motor can realize rotation along axis$Z$ by the hybrid of two orthogonal bending vibration modes. The driving signal1 and driving signal2 are applied on each two parallel pieces of piezoelectric ceramic plates, namely, the driving signal1 is applied to ceramic plate1, 3 and the driving signal2 is applied to ceramic plate2, 4, respectively. Under this circumstance, the bending vibration in plane$YOZ$ is excited by the ceramic plate1, 3 while the bending vibration in plane$XOZ$ is excited by the ceramic plate2, 4. Since there is a phase shift of 90 degrees between driving signal1 and driving signal2, an elliptical movement trajectory in plane$XOY$ of the driving foot can be accomplished by the superposition of these two bending vibrations, as shown in Fig. 4.
Fig. 4. Operating sequence of rotation along axis$Z$: a) the vibration state of the proposed motor when $t={t}_{0}$ or $t={t}_{4}$, b) the vibration state of the proposed motor when $t={t}_{1}$, c) the vibration state of the proposed motor when $t={t}_{2}$, d) the vibration state of the proposed motor when $t={t}_{3}$
When $t={t}_{0}$_{}or $t={t}_{4}$, $\left{V}_{1}\right=$ 0 and $\left{V}_{2}\right={V}_{m}$, the deformations of ceramic plate2, 4 reaches maximum with ceramic plate1, 3 getting no deformation and the vibration state of the proposed motor is shown in Fig. 4(a). Then, $\left{V}_{1}\right$ increases and $\left{V}_{2}\right$ decreases. The deformations of corresponding ceramic plates are in identical tendency with the voltage changes. At the same time, the vibration state of the proposed motor changes from what is shown in Fig. 4(a) to the one shown in Fig. 4(b). The next two states can be reached in rest part of a period. Finally, the rotation along axis$Z$ of a runner can be actuated.
The proposed motor can realize rotation along axis$Y$ by the hybrid of the bending vibration in plane$XOZ$ and the longitudinal vibration. The driving signal2 is applied on the two pieces of piezoelectric ceramic plates parallel with plane$YOZ$, namely, ceramic plate2, 4. The driving signal1and 3 are applied on the two pieces of piezoelectric ceramic plates parallel with plane$XOZ$, namely, ceramic plate1 and 3, respectively. In this condition, one of the ceramic plate2 and 4 extends with the other shrinking; both ceramic plate1 and 3 extend or shrink at the same time. Thus, the bending vibration in plane$XOZ$ and the longitudinal vibration are excited. With the phase shifts between these three driving signals, the elliptical movement trajectory in planeYOZ of the driving foot can be realized by the superposition of these two vibrations. When $t={t}_{0}$ or $t={t}_{4}$, $\left{V}_{1}\right=\left{V}_{3}\right=$ 0 and $\left{V}_{2}\right={V}_{m}$, the deformations of ceramic plate2 and 4 reaches maximum with ceramic plate1 and 3 getting no deformation. The state of the proposed motor is shown as Fig. 5(a). Then, $\left{V}_{2}\right$ decreases, $\left{V}_{1}\right$ and $\left{V}_{3}\right$ increase. The deformations of ceramic plate2, 4 and the degree of the bending vibration diminish. The deformations of ceramic plate1, 3 and the degree of the longitudinal vibration are enhanced. The state of the proposed motor changes from what is shown in Fig. 5(a) to the one shown in Fig. 5(b). In the rest of a period, states shown in Fig. 5(c) and (d) will be accomplished. Finally, the rotation along axis$Y$ of a runner can be actuated.
Fig. 5. Operating sequence of rotation along axis$Y$: a) the vibration state of the proposed motor when $t={t}_{0}$ or $t={t}_{4}$, b) the vibration state of the proposed motor when $t={t}_{1}$, c) the vibration state of the proposed motor when $t={t}_{2}$, d) the vibration state of the proposed motor when $t={t}_{3}$
In a similar way, the proposed motor can realize rotation along axis$X$ by the hybrid of the bending vibration in plane$YOZ$ and the longitudinal vibration. The driving signal2 is applied on the two pieces of piezoelectric ceramic plates parallel with plane$XOZ$, namely, ceramic plate1 and 3. The driving signal1 and 3 are applied on the two pieces of piezoelectric ceramic plates parallel with plane$YOZ$, namely, ceramic plate2 and 4, respectively.
3. FEM analyses
In order to verify the feasibility of the driving principle presented in last section, the FEM model of the proposed motor is established and analyzed. The material of metal base is aluminum alloy and the PZT ceramic elements are PZT4.
3.1. Modal analysis
The proposed motor takes advantage of three vibration modes a longitudinal vibration mode and two orthogonal bending vibration modes. The structural parameters of the proposed motor are adjusted to tune the resonance frequencies of these vibration modes close to each other. And it can be found out that the resonance frequencies of the two bending vibration modes will keep the same with the structure symmetric in plane$XOY$. Therefore, the main work in this part is simplified and just to tune the resonance frequency of the longitudinal vibration mode close to the one of the bending vibration mode. The resonance frequencies of the longitudinal vibration mode and the bending vibration mode are calculated to be about 40.95 kHz and 41.12 kHz, respectively, and the final dimensions are shown in Fig. 6.
3.2. Transient analysis
After establishing FEM model and accomplishing the parameter design of the proposed motor, it needs to verify the driving principle presented in second section. And the cardinal work in this part is to observe if the driving foot moves in the desired elliptical trajectory.
The transient analysis was executed by ANSYS. The driving signals were applied on the FEM model in the ways as shown in driving principle. The frequency and virtual voltage of the driving signals are 40.95 kHz and 100 V, respectively. There are four special points on the driving foot shown in Fig. 7 and the motion trajectories of these four points in last period of the simulation are shown in Fig. 8. The Fig. 8(a) and (b) show the motion trajectories of rotation along axis$Z$ and axis$Y$, respectively. Except the difference in direction, the driving principle of rotation along axis$X$ is same with the one of rotation along axis$Y$. Thus, the rotation along axis$X$ needn’t to be presented.
Fig. 6. Dimensions of the proposed motor (unit: mm)
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b)
Fig. 7. Selected nodes on the driving foot
Fig. 8. Motion trajectories of selected nodes in the last simulation period: a) trajectories of rotation along axis$Z$, b) trajectories of rotation along axis$Y$
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b)
It can be seen from the Fig. 8(a) that the motion trajectories of the four points are nearly circular. They aren’t overlapped because the selected points of elements in FEM model aren’t exactly at the points shown in Fig. 7. The amplitudes of the two bending vibrations are almost 2.1 um. It can be seen from the Fig. 8(b) that the trajectories of four points are elliptical. ${P}_{2}$ and ${P}_{4}$ are at the plane$YOZ$ and long axes of their motion trajectories are parallel with axis$X$. The long axes of the ${P}_{1}$ and ${P}_{3}$’s motion trajectories are a little inclined with the axis$X$. The minimal amplitude is the one of the longitudinal vibration, which is about 0.72 um. According to transient analysis, the driving principle is feasible.
4. Experiments
Only finishing FEM analyses is not sufficient to verify the feasibility of the proposed motor. A prototype of the proposed motor was fabricated, as shown in Fig. 9. The results of the experiments are presented in this section.
Fig. 9. Prototype of the proposed motor
4.1. Vibration shape test
The prototype of the proposed motor used the three vibration modes presented in the second section. The longitudinal vibration mode will be excited by ceramic plate1, 3 and ceramic plate2, 4, respectively. Therefore, there are four vibrations need to be tested two bending vibrations and two longitudinal vibrations. This experiment was executed by a scanning laser Doppler vibrometer (Psv400m2, Polytec, Germany), to obtain the actual resonance frequencies and vibration shapes. The vibration shapes and the frequencymagnitude curves of four exciting ways are shown in Fig. 10 and Fig. 11.
Fig. 10. Bending vibration scanning results of the prototype: a) vibration velocity response spectrums under bending mode excited by ceramic1 and ceramic3, b) second order bending vibration shape excited by ceramic1 and ceramic3, c) vibration velocity response spectrums under bending mode excited by ceramic2 and ceramic4, d) second order bending vibration shape excited by ceramic2 and ceramic4
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b)
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Fig. 10 shows that the practical resonance frequencies of two bending vibration modes are 38.04 kHz and 38.14 kHz, respectively, and their vibration shapes are all second order bending vibration. Fig. 11 shows that the vibration shapes of two longitudinal shapes and practical resonance frequencies are 38.19 kHz and 38.23 kHz, respectively. The resonance frequencies in this experiment are different from ones in the FEM analyses. It might result from the differences of materials and constraint condition in practice and the FEM, and also the fabricating and assembling errors. But the practical resonance frequencies of four vibrations are closed with each other and their vibration shapes are the same with the ones gained by the FEM analyses.
Fig. 11. Longitudinal vibration scanning results of the prototype: a) vibration velocity response spectrums under longitudinal mode excited by ceramic1 and ceramic3, b) first order longitudinal vibration shape excited by ceramic1 and ceramic3, c) vibration velocity response spectrums under longitudinal mode excited by ceramic2 and ceramic4, d) first order longitudinal vibration excited by ceramic2 and ceramic4
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b)
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4.2. Output characteristics test
In order to obtain practical actuating capacity of the proposed motor, output velocities in three directions of the prototype were tested. Actuation of each direction was excited as the driving principle. And the runner was a steel ball with the diameter of 25 mm. Firstly, the frequencyvelocity curves were obtained and shown in Fig. 12(a). The peaktopeak amplitudes of driving signals applied were 100 V and the frequencies of the driving signals ranged from 37.45 kHz to 39.05 kHz. Although the frequency corresponding to the highest velocity of rotation along axis$X$ is 0.1 kHz higher than the ones of the other two, the velocity of rotation along axis$X$ corresponding to 38.15 kHz is just 2 rpm lower than the one corresponding to 38.25 kHz. Thus, the frequencies of driving signals were chosen as 38.15 kHz. With excited by these driving signals, the velocities of rotation along axis$X$, $Y$ and $Z$ are 138 rpm, 135 rpm and 180 rpm, respectively.
Secondly, the voltagevelocity curves were obtained and shown in Fig. 12(b). The frequencies of driving signals were 38.15 kHz and the peaktopeak amplitudes of three driving signals ranged from zero to 200 V, to observe changes of velocity. It can be seen from the Fig. 11(b) that the velocities of rotation along three directions are in positive correlation with the amplitude of the driving signals. And the minimal amplitude needed to realize rotation along axis$X$ or $Y$ is about half of the one needed to realize the rotation along axis$Z$. Their starting voltages are 10 Vpp, 9 Vpp and 22 Vpp, respectively. But after the rotation along axis$Z$ was excited, its velocity increased swiftly than the other two. The trends of rotation along axis$X$ and $Y$ are similar. Under driving voltages of 200 Vpp, the output velocities of three DOF can reach 280 rpm, 277 rpm and 327 rpm, respectively.
Fig. 12. Mechanical output characteristics of the prototype: a) frequencyspeed curves tested under driving signals with peaktopeak voltages of 100 V, b) voltagespeed curves tested under driving signals with frequencies of 38.15 kHz
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b)
5. Conclusions
This paper proposes a novel threeDOF ultrasonic motor, which is based on the hybrids of two bending vibration modes and a longitudinal vibration mode. The driving principle is presented in this paper and verified to be feasible. In FEM analysis, fixed constraint was applied to the motor and resonance frequencies of selected vibration modes are 40.95 kHz and 41.12 kHz in finial dimensions, respectively. The proposed motor’s FEM and prototype are not identical, but the practical resonance frequencies are approximate. Through mechanical output tests, the proposed motor was found out to possess the characteristics of low starting voltages and high output velocities. And the piezoelectric ceramic plates in the proposed motor can be used to excite the bending vibration or the longitudinal vibration by different driving signals, which reduces the number of the piezoelectric ceramic plates, simplifies the structure of the proposed motor and make it easy to realize miniaturization. These characteristics make the proposed motor possesses practical utility.
Acknowledgements
This work was supported in part by the National Natural Science Foundation of China (No. 51622502 and No. 51475112), in part by the Foundation for the Author of National Excellent Doctoral Dissertation of China (No. 201428), in part by the Foundation for Innovative Research Groups of the National Natural Science Foundation of China (No. 51521003) and in part by the Fok Ying Tung Education Foundation (No. 151053).
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