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Impact of the tribological characteristics on the dynamics of the ultrasonic piezoelectric motor.

1. Introduction

The ultrasonic motor (USM) characteristics driven by piezoelectric transducer strongly depend on the mechanical properties of the components stator, rotor and contact layer [1]. The methodology of contact zone parameters' control of USM is very important. The main tribological surface characteristics influencing the speed regularity of USM in steady regimen are macro- and microasperities and friction coefficient fluctuations between rotor surface and friction element. They are depend on contacting materials and its surface characteristics of the USM rotor [2]. The research show that the changes of rotor surface rigidity (in case if the contact between rotor surface and contacting element is not disturbed) and the fluctuations of diagonal impact recovering coefficient (when the contact between rotor surface and contacting element is regularly changing) have less influence on speed steadiness of USM [3, 4].

2. The synthesis of dynamic and tribological characteristics of piezoelectric motor

The research were performed at the prototype of the ultrasonic piezoelectric motor with the piezoelectric plate-shaped transducer (Fig. 1a), in which the alternating strain is excited by an AC electrical field, preferably operating at the mechanical resonance frequency.

Fig. 1 presents the schemes of rotation and translation motion, which enables the diagnostics of tribological properties of USM contact zone. The diagnostic system signals correlating with tribological properties of contact zone are:

* macro- and micro-asperities of rotor surface and stochastic oscillation in contact zone arising because of friction coefficient fluctuation between rotor surface and contacting friction element which will generate electric charges in central electrode 9 because of direct piezo-effect;

* besides the electric charges in central electrode 9 (which value will correlate with the stochastic oscillation in contact zone) the longitudinal oscillation of piezoelectric plate at the oscillatory node (I form, [[delta].sub.x] = 0) will generate intensive electric charges of main frequency (with the lagging) which will be filtered at filter 12;

* oscillations of piezoelectric plate bending (II form) will not generate the electric charges in central measurement electrode (they will have opposite charge in bottom and upside of electrode 9 and the sum of their charges will be equal to zero).

The scheme of USM (Fig. 1, a) enables to get the interesting regimen of rotor's motion--continuous motion with rotation oscillations which is realised by the connecting electric voltages [U.sub.1] (t) and [U.sub.2] (t) to the electrodes 6, 8 and 5, 7.

In order to excite specific rotational type oscillations within the rotor two harmonic signals ([U.sub.1] and [U.sub.2]) of different frequency and amplitude are supplied to both groups of control electrodes. Signal expressions are presented in Eqs. (1) and (2) [3]:

[U.sub.1] (t) = [U.sub.01] cos ([[omega].sub.1] t - [[phi].sub.1]), (1)

[U.sub.2] (t) = [U.sub.02] cos ([[omega].sub.2]t - [[phi].sub.2]), (2)

where [U.sub.01], [U.sub.02] are voltage amplitudes, [[omega].sub.1], [[omega].sub.2] are angular frequencies, t is time and [[phi].sub.1], [[phi].sub.2] are phases of harmonic signals. Here [[omega].sub.2] > [[omega].sub.1] and [[omega].sub.2] - [[omega].sub.1] [much less than] [[omega].sub.1].

In the presence of such conditions, the moving member (i.e. rotor) performs a periodic motion, which is defined by the following law [5]:

A = [A.sub.max] cos ([[[omega].sub.2] - [[omega].sub.1]/2] t), (3)

where [A.sub.max] is the maximal amplitude and t is time of rotational type vibrations.

In this case harmonic oscillations are excited in frequency range from 0 Hz at [[omega].sub.2] = [[omega].sub.1], A = [A.sub.max].

The example of such rotor's rotational oscillations is displayed in Fig. 2 [5]. It presents the case when [U.sub.1](t) = = [U.sub.2] (t), i.e. the average speed of rotor is equal to zero.

In order to determine the resonance frequency of the designed piezoelectric transducer, an impedance analyzer Wayne Kerr 6520 A (Fig. 3, a) is used to measure the impedance characteristics of the prototype, and the measurement plot of electric impedance within the measured frequencies is used (shown in Fig. 3, b).

By observing the measured impedance vs. frequency characteristic, shown in Fig. 3b, there are three resonant frequencies (around 44 kHz, 92 kHz and 132 kHz) when the impedance reaches a maximum. The operation frequency of the USM is 44.1 kHz and was determined experimentally.

The feedback synthesis between the parameters of diagnostic system and the oscillation parameters of USM transducer is realised by:

* controlling the oscillation amplitude of signals generator--it is the simplest way to regulate the rotor's speed in wide range. Fig. 4 presents the example of such control [6]. It is evident that the condition [[omega].sub.max]/[[omega].sub.min] = 3 ... 5; is realised easily, especially at lower loading of the rotor;

* controlling the frequency of harmonic signals which is in the operational resonance zone of USM transducer. Such example is presented in Fig. 5 [6]. This method is used less often, because the time quiescent of frequency change is usually higher than the amplitude change of the harmonic voltage;

* there is the method used in piezoelectric step motors -controlling the filling coefficient of the supply impulses completed with the harmonic resonance signals;

* another method is the use of both signals of same resonance frequency [U.sub.1](t) and [U.sub.2](t), but changing the phase of second signal to zero. In that case (Fig. 1) only transducer's longitudinal oscillations are generated and the speed of USM is equal to zero.

3. Rotary speed stabilisation system of USM

The outside ring 1 of rotor (Fig. 6, a) should be made of the low acoustic resistance material (steel, ceramic etc.). It is mounted on internal part of rotor 2, which is made from composite material with high acoustic resistance. Outside ring is contacting with the plate of piezoelectric transducer 3 (having the polarisation vector perpendicular to the plate) through the intermediate frictional element 4. One electrode of piezoelectric transducer is earthed and other is divided in sectors 5 and 6. Acoustic contact between transducer and rotor is made by the spring 7.

The transducer's electrodes are connected to the electric signal generator 8 through the controller 9. Generator's voltage U cos2[pi][lambda]t is connected to the electrodes' groups 5 and 6 through the switcher 10, which is steered by the controller also connecting the free electrode to the and the filter of higher frequency harmonics 11. Filtered signal pass to the detector 12, which exit is connected to controller.

The measurements [h.sub.1] and [h.sub.2] of rotor's outside ring 1 (Fig. 6, a) should be significantly lower than the wavelength of excited oscillation (frequency [lambda]) at the material of outside ring (for the reflection minimisation of diffusive waves).

The voltage of generator Ucos2[pi][lambda]t is exciting in piezo-transducer two types of oscillations because of the asymmetry of electrodes' groups: longitudinal first form oscillations (distribution of amplitudes in length [delta]x of the plate is presented in scheme) and bending oscillations (second form, [delta]y). There is not big difference between the resonance frequencies of both forms causing the elliptic oscillation trajectory of contact element 4 and consequently the rotor's revolution which direction decides the switcher 10.

Complicated dynamic processes are taking place during the oscillations in contact zone (dependently on the oscillation amplitudes--from high frequency diagonal impacts to the sliding which is regularly changing friction force in contact zone) between rotor's outside ring 1 and intermediate frictional element 4. It causes generation of harmonic oscillations of main frequency [lambda] and higher frequencies. Because of direct piezo-effect the electric charges are excited in piezo-transducer, which are filtered in the filter 11 of [lambda] and higher frequency harmonics.

Excited [lambda] frequency oscillations pass also to outside ring 1 where they are channelized into two sides: clockwise and counter clockwise. When the direction of rotation speed [omega] is as in fig. 6a, counter clockwise in the rotating ring 1 diffused oscillations (U11) are reaching the contact zone with the delay and its frequency registered by the free electrodes is reduced (Doppler Effect):

[[lambda].sub.11] = [V/(V + [omega] R)] [lambda],

here V is sound speed in rotor's outside ring, 2R is diameter of outside ring.

When the oscillations are diffusing in outside ring clockwise ([U.sub.12]) its frequency increase:

[[lambda].sub.12] = [V/(V - [omega] R)] [lambda].

The summary signal [U.sub.1](t) after the filter 11 of [lambda] and higher frequency harmonics is passing to detector 12 and controller 9 forms the signal U([omega]), which is proportional to the rotation speed m of frequency [f.sub.m] = [absolute value of ([[lambda].sub.11] - [[lambda].sub.12])]. Dependently on the size of this signal, the controller 9 changes the amplitude of signal generator 8 stabilizing the rotation speed [omega].

The acoustic measurement oscillations could be excited by the separate transducer enabling the extension of its frequency range and the increase of the preciseness of the measurement. Such scheme presented in Fig. 7 where the range of [lambda] frequency could reach up to 5 MHz.

Thus using the feedback between the parameters of diagnostic system and the parameters of piezoelectric transducer oscillations there is possible to control the speed of USM at the impact of the external disturbances: temperature, wear, rheological changes of the surface etc.

4. Conclusions

The following conclusions on the influence of contact zone tribological parameters on the stabilisation of rotation speed of piezoelectric motors could be formed:

* created speed control schemes of rotation and translation motion piezoelectric motors allows to diagnose the tribological properties of USM contact zone;

* experimental results show the possibility to excite the rotary low frequency oscillations at USM rotor when two ultrasonic frequency harmonic signals are supplied to the piezo-transducer;

* presented three USM schemes enable the regulation of speed control parameters of piezo-transducer: amplitude, frequency and phase;

* two rotor speed stabilisation schemes with the use of Doppler Effect were analysed.

http://dx.doi.org/10.5755/j01.mech.21.1.10136

Received November 03, 2014

Accepted February 02, 2015

Acknowledgement

This research was funded by the Research Council of Lithuania (Project TriboPjezo, contract No MIP-079/2012 and Project PiezoTable, contract No MIP 094/12).

References

(1.) Storck, H.; Wallaschek, J. 2003. The effect of tangential elasticity of the contact layer between stator and rotor in travelling wave ultrasonic motors, International Journal of Non-Linear Mechanics 38: 143-159. http://dx.doi.org/10.1016/S0020-7462(01)00048-8.

(2.) Padgurskas, J.; Bansevicius, R.; Zinnia, A.; Rukuiza, R.; Andriusis, A. 2013. Investigation of Tribological Properties in Piezoelectric Contact, Surface Engineering and Applied Electrochemistry 49(5): 401-407. http://dx.doi.org/10.3103/S1068375513050104.

(3.) Ragulskis, K.; Bansevicius, R.; Barauskas, R.; Kulvietis, G. 1988. Vibromotors for Precision Microrobots. Hemisphere Publ. Corporation, New York, ISBN 0-89116-549-5. 310p.

(4.) Grybas, I.; Bansevicius, R.; Bubulis, A.; Jurenas, V.; Kulvietis, G. 2013. Development of two modifications of piezoelectric high resolution rotary table, Journal of Vibroengineering 15(4): 2203-2208.

(5.) Grybas, I.; Bubulis, A.; Bansevicius, R.; Jurenas, V. 2014. Research of rotary piezotable driven by two harmonic signals, Mechanika 20(6): 573-576.

(6.) Final Report of High Technology PiezoAdapt Project "R&D of Mechatronic Nano Resolution Actuators/ Sensors Systems". Kaunas University of Technology, 2009 (compiled by R. Bansevicius, V. Jurenas, et al.) (in Lthuanian).

J. Padgurskas *, R. Rukuiza **, R. Bansevicius ***, V. Jurenas ****, A. Bubulis *****

* Institute of Power and Transport Machinery Engineering, Aleksandras Stulginskis University, Studentu 15, Akademija, LT-53362 Kauno r., Lithuania, E-mail: juozas.padgurskas@asu.lt

** Institute of Power and Transport Machinery Engineering, Aleksandras Stulginskis University, Studentu 15, Akademija, LT-53362 Kauno r., Lithuania, E-mail: raimundas.rukuiza@asu.lt

*** Kaunas University of Technology, Kestucio 27, LT-44025 Kaunas, Lithuania, E-mail: ramutis.bansevicius@ktu.lt

**** Kaunas University of Technology, Kestucio 27, LT-44025 Kaunas, Lithuania, E-mail: algimantas.bubulis@ktu.lt

***** Kaunas University of Technology, Kestucio 27, LT-44025 Kaunas, Lithuania, E-mail: vytautas.jurenas@ktu.lt
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Author:Padgurskas, J.; Rukuiza, R.; Bansevicius, R.; Jurenas, V.; Bubulis, A.
Publication:Mechanika
Article Type:Report
Geographic Code:4EXLT
Date:Jan 1, 2015
Words:1987
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