Vibration wave driven motor

Abstract: A vibration wave driven motor includes a vibrator, a plurality of driving electro-mechanical energy conversion element portions disposed in the direction of lamination relative to the vibrator, frequency signals of different phases being applied to the conversion element portions, and a monitoring electro-mechanical energy conversion element provided in the vibrator in the direction of lamination relative to the conversion element portions.

Description: This invention relates to a motor generating mechanical power without resorting to electromagnetic power, and more particularly to a bar-shaped ultrasonic motor (vibration wave driven motor) which utilizes circular motion excited in a vibrator by the combination of expansive and contractive vibrations in the axial direction to rotate a driven member fitted coaxially with the vibrator by frictional driving. A motor as shown for example in Figure 13 of the accompanying drawings has heretofore been proposed as an ultrasonic motor (vibration type motor) of this type in EP-A-0420622 which describes the state of the art according to Article 54(3) EPC. In Figure 13, the reference numeral 1 designates a vibration member comprising a metallic round bar having a small-diametered shaft portion la forming a fore end portion, a large diametered shaft portion 1b forming a rear end portion, and a frusto-conical portion 1c formed between the small-diametered shaft portion la and the large-diametered shaft portion 1b and having a diameter progressively decreasing toward the fore end portion, the reference numeral 2 denotes a keep member comprising a metallic round bar formed to the same outer diameter as the large-diametered shaft portion 1b of the vibration memeber 1 and having a bolt insertion hole 2a formed along the axis thereof, the reference numerals 3 and 4 designate circular ring-shaped piezo-electric element plates formed to the same outer diameter as the large-diametered shaft portion 1b, and the reference numeral 5 denotes the electrode plate of the piezo-electric element plates 3 and 4. The piezo-electric element plates 3 and 4 with the electrode plate 5 interposed therebetween are disposed between the vibration member 1 and the keep member 2, and the keep member 2 is fixed to the vibration member 1 by a bolt 6, whereby the piezo-electric element plates 3 and 4 are fixed between the vibration member 1 and the keep member 2 to thereby constitute a vibrator A. The bolt 6 has its head in contact with the keep member 2 with a circular ring-shaped insulator 7 interposed therebetween and has its shank portion held in non-contact with respect to the piezo-electric element plates 3, 4 and the electrode plate 5. The piezo-electric element plates 3 and 4 each have on one surface thereof two electrodes (plus electrode a and minus electrode b) differing in the direction of polarization from each other and polarized in the direction of thickness, said two electrodes being symmetrically formed on the opposite sides of an insulating portion d formed on the center line, and have formed on the other surface thereof an electrode c common to the plus electrode a and the minus electrode b, and are disposed with a positional phase difference of 90° therebetween with respect to the axis of the vibrator A. The polarized electrodes (the plus electrode a and the minus electrode b) of the piezo-electric element plate 3 are in contact with the rear end surface of the vibration member 1 which is an electrical conductor, and the piezo-electric element plate 4 is in contact with the front end surface of the keep member 2 which is an electrical conductor. An AC voltage V 1 is applied to between the electrode plate 5 and the vibration member 1 and an AC voltage V 2 is applied to between the electrode plate 5 and the keep member 2, whereby the vibrator A is vibrated by the combination of vibration caused by the expansive and contractive displacement of the piezo-electric element plate 3 in the direction of thickness thereof and vibration caused by the expansive and contractive displacement of the piezo-electric element plate 4 in the direction of thickness thereof. The AC voltage V 1 and the AC voltage V 2 , as shown in Figure 14 of the accompanying drawings, are identical in amplitude and frequency and have a difference of 90° in time and spatial phases therebetween. Thus, the vibrator A makes circular motion like that of the rope of rope skipping (hereinafter referred to as the rope-skipping) about the axis thereof. The principle on which such circular motion occurs is described in detail in the above mentioned EP-A-0420622, and therefore need not be described herein. As shown in Figure 15 of the accompanying drawings, a rotor 8 is fitted coaxially with the axis ℓ of the vibrator A, and the rear end portion (hereinafter referred to as the frictional contact portion) 8b of the inner diameter portion of the rotor 8 extends to a location corresponding to a sliding portion B, and the frictional contact portion 8b is brought into contact with the sliding portion B of the frusto-conical portion 1c. The frustoconical portion is provided to obtain an appropriate frictional force in the sliding portion B by being subjected to an axial pressure force. This sliding portion B provides the loop of the rope-skipping in the vibration member 1. The bore of the inner diameter portion 8a of the rotor 8 is of such structure that in the vibration member 1, it contacts with the position of the mode of the rope-skipping with a member 8d of low coefficient of friction interposed therebetween, and the rotor 8 is provided with an escape 8c to prevent the inner diameter portion from contacting with any vibration created in the other portions than the sliding portion B and producing sounds. The frictional contact portion 8b of the rotor 8 diverges into such a shape that the inner diameter thereof conforming to the outer peripheral shape of the sliding portion B progressively increases, and surface-contacts with the sliding portion B during the rope skipping motion of the vibration member 1. The rotor 8 is pushed for example, in the direction of arrow in Figure 15 by a spring or the like, not shown, through a thrust bearing, not shown, thereby producing a predetermined frictional force in the portion of contact between the frictional contact portion 8b and the sliding portion B by the sliding portion having the aforedescribed appropriate progressively increasing diameter, and also is permitted axial rotation by the thrust bearing. From the above-described structure, there is realised an ultrasonic motor (a vibration wave driven motor) in which the vibration of the vibration member 1 is transmitted as a rotational force to the frictional contact portion 8b of the rotor to thereby rotate the rotor. Generally, however, the ultrasonic motor (vibration type motor) of this kind has a resonant frequency of the order of several tens of kilohertz, and unless it is driven in the vicinity of this frequency, a great amplitude will not be obtained and such motor will not operate as a motor. Also, the resonant frequency of the motor fluctuates in dependence upon environmental conditions such as temperature and humidity and load conditions. This leads to the problem that the rotational speed become unstable if the motor is driven at a predetermined frequency. DE-A-3634329 discloses a vibration wave driven motor comprising an electromechanical energy conversion element which is incorporated in a control circuit so that the motor can be controlled to operate at substantially its resonance frequency. According to the invention there is provided a rotary vibration wave driven motor having the features as recited in claim 1. One aspect of the application is to provide a cylindrical-shaped ultrasonic motor (vibration wave driven motor) in which an AC electric field is applied to an electro-mechanical energy conversion element disposed in the body of the vibrator, whereby the vibrator is caused to excite vibrations of bending modes of the same shape having a phase difference in terms of time therebetween in a plurality of planes, thereby causing the surface particles of a vibration member to make circular to elliptical motion and creating relative motion by frictional driving between the vibration member and a member pressed against the vibration member, and wherein the vibrator is provided with a vibration detecting electro-mechanical energy conversion element, whereby the vibrated state can be detected. The vibration detecting conversion elements and monitoring element are preferably of an annular shape of the same diameter. The annular conversion element is preferably bisected and the bisected elements are polarized in different directions to monitor the vibrated state. In the accompanying drawings:- Figure 1 is an exploded perspective view showing a first embodiment of the present invention. Figure 2 is a graph showing the relation between a vibration detection signal and a frequency in the first embodiment. Figure 3 is a graph showing the phase difference vs. frequency relation between the vibration detection signal and an input voltage in the first embodiment. Figure 4 is a block diagram of a control circuit in the first embodiment of the present invention. Figure 5 is an exploded perspective view showing a second embodiment of the present invention. Figure 6 is a graph showing the phase difference vs. frequency relation between a vibration detection signal and an input voltage in the second embodiment. Figure 7 is an exploded perspective view showing a third embodiment of the present invention. Figure 8 is a graph showing the phase difference vs. frequency relation between a vibration detection signal and an input voltage in the third embodiment. Figure 9 is a side view showing an arrangement included for reference only. Figure 10 is a side view showing a fourth embodiment of the present invention. Figures 11(a) - 11(d) show the electrode patterns of a vibration detecting piezo-electric element used in the motor of embodiments of the present invention. Figure 12 shows a system incorporating the bar-shaped ultrasonic motor of one embodiment of the present invention therein. Figure 13 is an exploded perspective view showing a prior art motor. Figure 14 shows the waveforms of AC voltages applied to piezo-electric element plates. Figure 15 is an assembly side view of the ultrasonic motor shown in Figure 13. First Embodiment Figure 1 is an exploded perspective view of a vibration wave driven motor according to a first embodiment of the present invention. In Figure 1, the reference numerals 1 - 8 are similar in significance to those in Figure 13. The reference numeral 9 designates a piezo-electric element as a vibration detecting element, the reference numeral 10 denotes an electrode plate for supplying electric power to the driving piezo-electric element 3, the reference numeral 11 designates an electrode plate for grounding the piezo-electric element 9, and the reference numeral 12 denotes an insulating member for holding the electrode plates 10 and 11 in a non-contact state. The piezo-electric element 9 is of the same structure as the piezo-electric elements 3 and 4, and is disposed so that the positional phase thereof may coincide with that of the piezo-electric element 3. The principle of driving is the same as that of the example shown in Figure 13 and therefore need not be described. Figure 2 shows the frequency in the vicinity of a resonant frequency fr in the first embodiment versus the amplitude of the output signal of the piezo-electric element 9. The output signal of the piezo-electric element 9 becomes maximum at the resonant frequency fr and decreases before and after it. Consequently, the resonant frequency fr can be found by detecting the frequency at which the amplitude of the output signal of the piezo-electric element 9 is maximum. Figure 3 shows the phase difference relation between the frequency vs. input voltage V 1 in the vicinity of the resonant frequency in the first embodiment and the output signal of the vibration detecting piezo-electric element 9. As can be seen from Figure 3, the phase difference between the input voltage V 1 and the output signal V S of the vibration detecting piezo-electric element 9 is 0° for a frequency higher than the resonant frequency, and gradually increases as the frequency approaches the resonant frequency, and becomes 90° for the resonant frequency fr, and increases to 180° for a frequency lower than the resonant frequency fr. As regards said phase difference, the same phase relation is obtained in both cases of the clockwise direction of rotation CW and the counterclockwise direction of rotation CCW because the piezo-electric element and the vibration detecting piezo-electric element 9 are disposed in a positional phase 0°. CW is a case where V 1 is advanced by 90° in terms of time with respect to V 2 , and CCW is a case where V 1 is delayed with respect to V 2 . From the above-described phase relation, the frequency can be adjusted to the resonant frequency by controlling the frequency so that the phase difference between the input voltage V 1 to the piezo-electric element 3 and the output signal of the vibration detecting piezo-electric element 9 may become 90°. Figure 4 shows a block diagram of a control circuit in the above-described bar-shaped ultrasonic motor (vibration wave driven motor). As oscillator 17 oscillates at a frequency determined by a signal generated by a frequency designator 24, and the output signal of the oscillator 17, together with a signal phase-shifted by 90° (or 270°) by phase shifter circuits 18 and 19, is amplified as two phases by amplifiers 20 and 21, whereafter it is input to the electrode plate 10 and the keep member 2. At this time, the keep member 2 must be an electrical conductor. A signal from the vibration detecting piezo-electric element 9 is obtained from the electrode plate 11, and the phase difference thereof from the signal V 1 from the amplifier 20 is found in a phase difference detector 22. Subsequently, how far said signal is from the resonant frequency fr is calculated by a calculation circuit 23, and the frequency designator 24 is varied. The above-described operation is repeated, whereby it becomes possible to drive the motor with the frequency kept at the resonant frequency. Also, the piezo-electric element 9 is circular and therefore can be provided with the resonant frequencies of vibrations in two directions kept coincident with each other, and the outer diameter thereof is equal to that of the vibrator or other driving piezo-electric element and therefore, by uniformizing the outer diameter during assembly, it is easy to keep the coaxiality with other parts. Further, the piezo-electric element 9 used is the same as the driving piezo-electric element and therefore, it is not necessary to make a discrete part as the vibration detecting piezo-electric element and thus, an increase in cost can be minimized. Second Embodiment Figure 5 is an exploded perspective view of a vibration wave driven motor according to a second embodiment of the present invention. In Figure 5, the vibration detecting piezo-electric element 9 is disposed at a position which is positionally 90° out of phase with respect to the piezo-electric element 3. That is, it lies at a position of positional phase 0° with respect to the piezo-electric element 4. In the other points, the construction of the second embodiment is the same as that of the first embodiment. In this embodiment, the amplitude of the frequency vs. the output of the piezo-electric element 9 is the same as that in the first embodiment. Figure 6 shows the relation of the phase difference  A-S between the frequency vs. input voltage V 1 in the vicinity of the resonant frequency in the second embodiment and the output signal V S of the vibration detecting piezo-electric element. As shown in Figure 6, the phase difference  A-S between the input voltage V 1 to the piezo-electric element 3 and the output signal of the vibration detecting piezo-electric element 9 describes such a curve that it becomes 0° for the resonant frequency fr and in the case of CW (-180° in the case of CCW). Consequently, when it is to be adjusted to the resonance frequency, the frequency can be controlled so that the phase difference  A-S may be 0° (-180° in the case of CCW). Also, the area of the phase difference  A-S entirely differs between CW and CCW and therefore, CW or CCW can be known from  A-S . The first and second embodiments have been respectively shown with respect to a case where the vibration detecting piezo-electric element 9 is positionally 0° out of phase with respect to the piezo-electric element 3 and a case where the vibration detecting piezo-electric element 9 is positionally 90° out of phase with respect to the piezo-electric element 3, but even in the case of any other positional relation, there is obtained a certain definite relation for the phase difference  A-S between the input voltage V 1 and the output signal of the vibration detecting piezo-electric element 9. Third Embodiment Figure 7 shows a third embodiment of the present invention. In Figure 7, the driving piezo-electric elements 3 and 4 each are laminated into two-sheet construction. It is known that if the driving piezo-electric elements are thus increased, the area used for the driving of the piezo-electric elements increases and low-voltage driving becomes possible. The vibration detecting piezo-electric element 9 is also constructed of two sheets, and with regard to the positional phase thereof, one sheet is disposed at a position which is 0° out of phase with respect to the piezo-electric element 3 and the other sheet is disposed at a position which is 90° out of phase with respect to the piezo-electric element 3. The phase difference  A-S between the output signal from the piezo-electric element 9 obtained from the electrode plate 15 at this time and the input voltage V 1 is such as shown in Figure 8. As can be seen from Figure 8, the phase difference  A-S between the input signal V 1 and the output signal of the vibration detecting piezo-electric element 9 describes such a curve that it becomes +45° for the resonant frequency fr and in the case of CW (+135° in the case of CCW). Such a curve is the same as the curve when the vibration detecting piezo-electric element is one sheet and the positional phase thereof with respect to the driving piezo-electric element 3 is 45° out of phase. However, it differs in amplitude. As described above, the vibration detecting piezo-electric element may be composed of a plurality of sheets, and in such case, various ways of taking out the output signal are possible depending on the way of determining the positional phase thereof. Also, as compared with the case where the vibration detecting piezo-electric element is one sheet, a great output voltage can be taken out. Moreover, if the driving and vibration detecting piezo-electric elements each are comprised of 2n sheets (n = 1, 2, ...), there is the advantage that the insulator is unnecessary and moreover power supply can all be effected through the electrode plate. Figure 9 is a side view of a bar-shaped ultrasonic motor (vibration wave driven motor) included for reference only. The reference numeral 16 designates a vibration detecting element formed, for example, of polyvinylidene fluoride and secured to the frusto-conical portion 1c of the vibration member 1 by an adhesive. As in the above-described embodiments, a signal of a certain amplitude and in a certain phase relation is obtained from the vibration detecting element 16, and the relation thereof is determined by the location on which the vibration detecting element 16 is stuck. Where the vibration detecting element as described above is to be stuck, its location may desirably be near the portion of contact between the vibration member and the movable member (rotor). Alternatively, the vibration detecting element may be stuck on the rotor side. In such case, the phase relation does not coincide with the signal being input to the stator for driving. Consequently, such a control method that the amplitude becomes maximum would occur to mind. Fourth Embodiment Figure 10 is a side view of a bar-shaped ultrasonic motor (vibration wave driven motor) according to afourth embodiment of the present invention. In this embodiment, the vibration detecting piezo-electric element 9 is provided in a portion of different diameter from the driving piezo-electric elements 3 and 4. Where as shown in Figure 10, the vibration detecting piezo-electric element 9 is provided in a portion of small diameter, the electrode area is small as compared with that in the first embodiment, etc. and therefore, the output voltage also becomes small. Consequently, where in the first embodiment, etc., the vibration detection output voltage is too great and must be made small on the circuit side, the vibration detecting piezo-electric element 9 can be provided in a small-diametered portion of the vibration member. Also, where conversely the vibration detection outut voltage is small, a great output voltage will be obtained if the vibration detecting piezo-electric element is provided in a large-diametered portion of the vibration member. Also, if in this case, a piezo-electric element of the same electrode pattern and having an outer diameter smaller than the inner diameter of the driving piezo-electric element or having an inner diameter greater than the outer diameter of the driving piezo-electric element is used for vibration detection, a driving piezo-electric element and a vibration detection piezo-electric element can be taken out from one sheet. Fifth Embodiment Figure 11 shows various examples of the electrode pattern of the vibration detecting piezo-electric element 9. The piezo-electric element 9 in the above-described first embodiment is of a doughnut-like shape having an electrode pattern as shown in Figure llD wherein two halves are polarized to plus (+) and minus (-), whereas where use is made of a piezo-electric element having an electrode pattern as shown in Figure 11A, the output voltage can be made small to thereby obtain an effect similar to that of the arrangement described hereinabove with reference to figure 9 because the electrode area is small. The electrode pattern of Figure 11B is an electrode pattern having, in addition to the above-described effect, a stress distribution which will hardly hamper the vibration of the vibration member. The electrode pattern of Figure 11C is polarized only in one half thereof, and has the advantage that the polarization of one half is only required when the piezo-electric element is made. Figure 12 shows the construction of a system which uses the motor according to one embodiment of the present invention to drive the lens barrel or the like of an optical lens. The reference numeral 25 designates a spring post portion, the reference numeral 26 denotes a rotation insulating member such as a bearing, and the reference numeral 27 designates a coil spring. The rotor 8 is pressed by the spring post portion 25 and the coil spring 27. The rotation of the rotor is insulated by the rotation insulating member 26, and the spring post portion 25 does not rotate. The reference numeral 28 denotes a gear joined coaxially with the rotor 8. The gears 28 transmits a rotational output to a gear 29 to rotate a lens barrel 30 having a gear meshing with the gear 29. An optical type encoder slit plate 31 is disposed coaxially with the gear 29 to detect the rotated positions and rotational speeds of the rotor 8 and the lens barrel 30, and the positions and speeds are detected by a photocoupler 32. The piezo-electric element as an electro-mechanical energy conversion element in each embodiment may be replaced by an electrostrictive element.

Claims: A vibration wave-driven motor comprising a plurality of plate-shaped electro-mechanical energy conversion elements (3, 4) disposed on a longitudinal axis of the motor, each plate shaped element (3,4) having at least a first polarisation portion (a) and a second polarisation portion (b) of different polarity from each other, said polarisation portions (a,b) of a first of said plate shaped elements (3,4) being adapted to receive a first frequency signal (V 1 ) and said polarisation portions (a,b) of a second of said plate shaped elements (3,4) being adapted to receive a second frequency signal (V 2 ) having a different phase to said first frequency signal to generate a driving force; a vibration member (1) arranged coaxially with said plate-shaped elements (3,4) to form a stack, said vibration member (1) being adapted to be vibrated by said driving force applied thereto by said plate shaped elements (3,4); and a plate-shaped monitoring electromechanical energy conversion element portion (9) disposed on the longitudinal axis for detecting vibrations in said vibration member (1), said plate-shaped monitoring element portion (9) comprising polarisation portions (a,b) arranged asymmetrically about a centre line substantially perpendicular to the longitudinal axis. A motor as claimed in claim 1, characterised in that an adjusting circuit (17-24) is provided for adjusting the frequency signals (V 1 , V 2 ). A motor as claimed in claim 2, characterised in that said adjusting circuit comprises a phase difference detector (22) connected to one of said plate-shaped elements (3,4) and said plate-shaped monitoring element portion (9), a frequency designator (24) connected to the output of said phase difference detector and serving to control the first and second frequency signals (V 1 , V 2 ), and phase shifting means (18, 19) for regulating the phase difference between the phases of said plate-shaped elements (3, 4). A motor as claimed in claim 1, 2 or 3, characterised in that there are provided two pairs of plate-shaped elements (3,4), each plate-shaped element (3,4) having said first and second polarisation portions (a,b) and two said plate shaped monitoring element portions (9), each plate shaped monitoring element portion (9) having a first and a second polarisation portion of different polarity from each other. A motor as claimed in any one of claims 1-4, characterised in that a keep member (2) is provided in the stack to hold the plate shaped elements (3,4) in the direction of the longitudinal axis, said plate shaped elements (3,4) being held between said vibration member (1) and said keep member (2). A motor as claimed in any one of claims 1-5, characterised in that said plate shaped elements (3,4) said vibration member (1), said keep member (2) and said plate shaped monitoring element portion (9) all have a circular profile of the same diameter so that the motor has a cylindrical configuration. An apparatus for driving the lens barrel of an optical lens, including a vibration wave-driven motor as claimed in any one of claims 1-6.

Inventors: ATSUTA AKIO, ATSUTA, AKIO, ATSUTA, AKIO, C/O CANON KABUSHIKI KAISHA
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1991
Main classification: H01L41
IPC codes: H02N2, H01L41