Vibration driven motor

Abstract: In an ultrasonic motor wherein a driving signal is applied to an electro-mechanical energy conversion element provided in a vibration member to thereby excite flexural vibrations of the same shape in the two different planes of the vibration member with a phase difference in time and thereby create rotational motion on the surface of the vibration member, thus frictionally driving a movable member which is in pressure contact with the vibration forming surface, electro-mechanical energy conversion elements for exciting the flexural vibrations are each disposed at a position whereat the sum totals of strains created in the electromechanical energy conversion elements are substantially equal to each other.

Description: This invention relates to an ultrasonic motor in which electrical energy is supplied to an electro-mechanical energy conversion element provided on a bar-like resilient member to thereby vibrate the resilient member as a bar-like vibration member and cause circular or elliptical motion at the surface particle of the vibration member, thus frictionally driving a movable member pressed against the vibration member, and particularly to an ultrasonic motor suitable for use in optical instruments such as camera and business machines such as printers. Ultrasonic motors of the type in which flexural vibration is caused in a circular ring-like resilient member and a lens driving movable member is driven by a frictional force have heretofore been put into practical use in AF mechanisms of cameras. However, the ultrasonic motor of this conventional type is of a ring-like shape and therefore is relatively high in cost as a unit including a pressing mechanism and disadvantageous in cost as a motor which is required to be hollow. So, a motor of the type as shown in Figures 2 to 4 of the accompanying drawings which is solid and easy to construct a pressing system has been proposed in recent years. This proposed motor will hereinafter be described briefly with reference to Figures 2 to 4. Figure 2 is a perspective view of the vibration member of a bar-like ultrasonic motor, and Figure 3 is a vertical cross-sectional view showing the construction of the motor. A vibration member creates primary flexural vibration as shown in Figure 4 by electro-mechanical energy conversion elements (hereinafter referred to as PZTs) a 1 and a 2 . PZT a 1 and PZT a 2 have a phase difference of 90° in position therebetween, and PZT a 1 and PZT a 2 each are comprised of two piezo-electric element plates (polarization-processed into different polarities with the diametrical portion thereof as a boundary). The letter C designates a bolt having a thin pillar-like shape in the upper portion thereof. PZT a 1 and PZT a 2 are sandwiched and fixed between a fore metal block b 1 and a rear metal block b 2 which are vibration member constituting members made of a metal relatively small in attenuation such as brass or stainless steel. The shape and dimensions of a pillar portion C-1 are determined such that the displacement during the vibration of the vibration member becomes small near the upper part of the pillar portion which is coupled to a vibration member fixing member g. A movable member d is given the spring force of a coil spring k in a spring case f through a bearing e and is in pressure contact with the upper surface of the vibration member. Now, the primary flexural mode created by PZTs a 1 and a 2 is excited in two kinds in a direction having a positional phase difference of 90° relative to a direction  (an angle in a plane orthogonal to the axis) and with a deviation of 90° in terms of time and therefore, the point A of the portion of contact with the movable member (shown in Figure 4) effects elliptical motion. The direction of this motion is determined by the shape of the vibration member, and the point A effects elliptical motion in a plane inclined by an angle α with respect to the Z-axis. At this time, the movable member which is in pressure contact is frictionally driven. In such an ultrasonic motor, AC voltages of the kinds corresponding to the number of flexural vibrations excited become necessary. Also, these AC voltages should desirably be of the same voltage amplitude from the convenience of a driving circuit, and this also holds true of the circular ring type ultrasonic motor of the prior art. In the bar-like ultrasonic motor, however, it has been found that when two sets of flexural vibrations by the A phase and B phase piezo-electric elements a 1 and a 2 are driven by the same voltage, the amplitudes of the vibrations differ from each other and elliptical motions differing in shape are created on the circumference of the vibration member. This state is shown in Figure 5 of the accompanying drawings. Two sets of flexural vibrations are excited by PZTs a 1 and a 2 in Figure 3. If at this time, the amplitudes of the vibrations differ from each other, uniform circular motion will not take place on the circumference, as shown in Figure 5. Here, each ellipse is a displacement locus, and becomes such as shown when the amplitude excited by PZT a 1 is smaller than the amplitude excited by PZT a 2 . At this time, the circumferential speed at a point B is greater than the value at a point C, and the movable member is driven at a different feed speed while the vibration of the vibration member makes one round. On the other hand, the movable member rotates at a certain constant speed by the inertial mass of itself and therefore, does not follow this speed difference but slips, and this provides a sliding loss which reduces the efficiency of the motor. Generally, the equivalent circuit of one phase (e.g. A phase) of the driving circuit of the ultrasonic motor is shown as in Figure 6 of the accompanying drawings when for example, the vibration speed of the portion of contact with the movable member is the standard. In Figure 6, cd is the electrostatic capacity of PZT used, A is the force coefficient, C m is the equivalent attenuation constant (including the load output), k is the equivalent spring constant, and m is the equivalent mass. That is, in order that speeds Ve iwt created in two phases (two flexural modes) when a voltage Ve icost is applied to the input terminal of the piezo-electric element of one phase of the driving circuit for the vibration member may be equal to each other, these constants can become equal to each other. cd is determined by the dielectric constant, shape, etc. of PZTs. Accordingly, the make cd equal, the materials and shapes of PZTs can be made coincident with each other. This condition is generally satisfied and in the prior art as well, as shown in Figure 4, two PZTs having a thickness of 0.5 mm are used for PZT a 1 and two PZTs of the same thickness and shape are used for PZT a 2 , and this condition is satisfied and irregularity is small. Also, C m , k, m, etc. are coincident between PZT a 1 and PZT a 2 because flexural vibrations of the same shape are utilized in the vibration member having an axis-symmetrical shape. Accordingly, the reason why the speeds, i.e., displacements, between the two phases are made incoincident (because frequencies are equal) is that the force coefficient A differs. Also, the force coefficient A is given by the ratio between the vibration speed and the electric current and therefore, the reason is considered to be that this coefficient differs. On the other hand, the electric current is determined by the materials, shapes and strains of PZTs, but since the materials, shapes, etc. of PZTs are made the same in order to make the electrostatic capacities cd of PZTs equal, the difference between the electric currents flowing through the two PZTs is considered to be due to the difference in strain, that is, considered to be because the strains created in PZT a 1 and PZT a 2 when equal vibration displacements are obtained in directions a 1 and a 2 shown in Figure 5 differ from each other. Now, a bar-like ultrasonic motor of the both end surface (surface t 1 and surface t 2 ) driving type shown in Figure 12 of the accompanying drawings is generally made in a symmetrical shape with the central surface in the lengthwise direction (the axial direction) in order to equalize the vibration speeds on the both end surfaces. However, in a bar-like ultrasonic motor of the type which is driven only on one end surface (e.g. surface t 1 ), it is desirable to make only the amplitude on the driving surface side great. The reason for this is that by making the vibration amplitudes on the portions other than the driving portion small and thus, making the strain created in the vibration member small, it is possible to make the energy loss in the vibration member small. Paying attention to such a fact, the applicant has previously proposed an arrangement in which a constriction is provided near the driving surface. Such a vibration member is shown in Figure 13 of the accompanying drawings. With regard to this vibration member, the admittance when the A phase piezo-electric element a 1 is driven and the admittance when the B phase piezo-electric element a 2 is driven superposed one upon the other are shown in Figure 8 of the accompanying drawings. As will be seen from this figure, in the case of this vibration member, the admittance Y at a resonance point F is considerably greater when the A phase piezo-electric element a 1 is driven. Now, when the angular frequency is ω, the admittance Y can be expressed as follows by the use of the aforementioned symbols: Y = 1 j(ω m A 2 - A 2 k ω ) + C m A 2 During the resonance of the vibration member, the imaginary number portion in the parentheses is zero and therefore, Y = A 2 /C m , that is, Y is proportional to the square of the force coefficient. Accordingly, in the vibration member shown in Figure 13, it is foreseen that the strains when driving flexural vibrations are created in the A phase pizeo-electric element a 1 and the B phase piezo-electric element a 2 differ greatly from each other. The result of the actual calculation of the strains created in the vibration member effected by the use of FEM is shown in Figure 14 of the accompanying drawings. From this result, it is seen that the strain created in the B phase piezo-electric element a 1 is considerably smaller than the strain created in the A phase piezo-electric element a 1 . That is, in Figure 14, the strain in the A phase piezo-electric element a 1 is greater than the strain in the B phase piezo-electric element a 2 and therefore, even if voltages of the same level are applied to the A and B phases, a greater electric current will flow through the A phase piezo-electric element a 1 with a result that a difference will occur between the amplitudes of flexural vibrations. JP-A-6292779 discloses an ultrasonic motor having one pair of piezo-electric elements for forward rotation and another pair of piezo-electric elements for reverse rotation. The pairs of piezo-electric elements separately vibrate a vibration member to drive a rotor in one direction. This arrangement does not address the problem of differential strain in the piezo-electric elements caused by the use of a vibration member of a symmetric shape along its axis. JP-A-6315677 discloses an ultrasonic motor enabling mutual conversion between electric energy and mechanical energy. Two torsional vibration generating piezo electric elements are provided either side of a vertical vibration generating piezo-electric element in a vibrator stack. Once again this arrangement does not address the problem of differential strain in the piezo-electric elements caused by the use of a vibration member of symmetric shape along its axis. The present invention provides a vibration driven actuator, comprising: a vibration member elongated along an axis and having an asymmetrical shape along said axis and a substantially symmetrical shape about said axis; a first electro-mechanical energy conversion member functionally and coaxially coupled to an intermediate portion of said vibration member substantially symmetrically about said axis, and arranged for generating a first flexural vibration having a first direction in said vibration member in response to a first electrical signal; and a second electro-mechanical energy conversion member functionally and coaxially coupled to an intermediate portion of said vibration member substantially symmetrically about said axis, arranged at a rotated position about said axis with respect to said first energy conversion member, and arranged for generating a second flexural vibration having a second direction different from said first flexural vibration in response to a second electrical signal, thereby to generate a rotating vibration as a result of the combination of the first flexural vibration and the second flexural vibration in said vibration member and an asymmetrical strain distribution along said axis in said vibration member and said first and second energy conversion members; characterized in that said first energy conversion member and said second energy conversion member are located at predetermined positions along said axis whereat strains created in said first and second energy conversion members by the application of said first and second electrical signals are substantially equal to each other. In one embodiment an ultrasonic motor is provided wherein a driving signal is applied to an electro-mechanical energy conversion element provided in a vibration member to thereby excite flexural vibrations of the same shape in the two different planes of said vibration member with a phase difference in time and thereby create rotational motion on the surface of said vibration member, thus fictionally driving a movable member which is in pressure contact with the vibration forming surface, electro-mechanical energy conversion elements for exciting the flexural vibrations are each disposed at a position whereat the strains created in the electro-mechanical energy conversion elements are substantially equal to each other. Embodiments of the present invention will now be described with reference to the accompanying drawings in which: Figure 1 shows a first embodiment of an ultrasonic motor according to the present invention. Figure 2 is a pictorical perspective view of an ultrasonic motor according to the prior art. Figure 3 is a cross-sectional view of the ultrasonic motor according to the prior art. Figure 4 shows the state of the flexural vibration of the ultrasonic motor according to the prior art. Figure 5 shows the vibration displacement locus of a vibration member according to the prior art. Figure 6 diagrammatically shows the equivalent circuit of the vibration member according to the prior art. Figure 7 shows the positional relation between the strain distribution of the vibration member and the piezo-electric elements according to the prior art. Figure 8 is a graph showing the vibration characteristic of the prior art. Figure 9 shows a modification of the first embodiment. Figure 10 shows a modification of the first embodiment. Figure 11 is a schematic view of a driving apparatus using an ultrasonic motor as a drive source. Figure 12 is a schematic view of a vibration member according to the prior art. Figure 13 is a schematic view of a vibration member according to the prior art. Figure 14 shows the positional relation between the strain distribution of the vibration member of Figure 13 and piezo-electric elements. Figure 15 shows the positional relation between the strain distribution of a vibration member according to a second embodiment and piezo-electric elements. Figure 16 is a graph showing the vibration characteristic of the vibration member of Figure 15. Figure 17 shows the positional relation between the strain distribution of a vibration member according to a third embodiment and piezo-electric elements. Figures 18A - 18F show an embodiment of an ultrasonic motor according to the present invention, Figure 18A being a side view of the motor, Figure 18B showing the amplitude distribution in the radial (r) direction, Figure 18C showing the strain distribution in the axis (z) direction of the side of the vibration member, Figures 18D and 18E being plan views of piezo-electric element plates, and Figure 18F showing the expanded and contracted state of the piezo-electric element plate when a voltage is applied thereto. Figure 19 is a diagram of the electric equivalent circuit of the vibration member. Figures 20A - 20C show a modification of the embodiment shown in Figures 18A - 18F, Figure 20A being a side view of a motor, Figure 20B showing the amplitude distribution in the radial (r) direction, and Figure 20C showing the strain distribution in the axial (z) direction of the side of a vibration member. Figures 21A - 21D show another embodiment, Figure 21A being a side view of a motor, Figure 21B showing the amplitude distribution in the radial (r) direction, Figure 21C showing the strain distribution in the axial (z) direction of the side of a vibration member, and Figure 21D showing the vibrated state of the vibration member. Figures 22A - 22C show another embodiment, Figure 22A being a side view of a motor, Figure 22B showing the amplitude distribution in the radial (r) direction, and Figure 22C showing the strain distribution in the axial (z) direction of the side of a vibration member. Figure 23 is a partly cut-away side cross-sectional view showing another embodiment. Figure 24 is a cross-sectional view of an apparatus using an ultrasonic motor. Figures 25A - 25F show an embodiment of the ultrasonic motor according to the present invention, Figure 25A being a schematic side view of a vibration member, Figure 25B showing the amplitude distribution in the radial (r) direction, Figure 25C showing the strain distribution in the axial (z) direction of the side of a vibration member, Figures 25D and 25E being plan views of piezo-electric element plates, and Figure 25F showing the deformed state of the piezo-electric element plate. Figures 26A - 26C show another embodiment, Figure 26A being a schematic cross-sectional view of a vibration member, Figure 26B showing the amplitude distribution in the radial (r) direction, and Figure 26C showing the strain distribution in the axial (z) direction of the side of the vibration member. Figures 27A and 27B and Figures 28A and 28B show the shapes and the amplitude distributions in the radial (r) direction, respectively, of further vibration members. Figure 29 shows an apparatus using the ultrasonic motor of one embodiment of the present invention as a drive source. Figure 1 shows a first embodiment of an ultrasonic motor according to the present invention, and more particularly shows the relation between a vibration member and the vibration mode thereof. Elements functionally similar to those of the motor according to the prior art are given similar reference characters and need not be described. This embodiment is one applied to a vibration member in the front portion of which there is formed a circumferential groove b 1 -1 and in which the vibration amplitude in this circumferential groove b 1 -1 is made great so that the portion forward thereof may be greatly displaced. Accordingly, the strain (ε z ) during driving of the vibration member formed rearwardly of the circumferential groove b 1 -1 of the vibration member is smaller than the strain formed in the circumferential groove portion. If the sum totals of the flexural vibrations of A phase piezo-electric element a 1 (comprised of two piezo-electric element plates) and B phase piezo-electric element a 2 (comprised of two piezo-electric element plates) constituting the vibration member are equal, flexural vibrations of equal amplitudes are obtained when voltages of the same magnitude are applied and therefore, in the present embodiment, the A phase piezo-electric element a 1 and the B phase pizeo-electric element a 2 are disposed on the opposite sides of the peak of a strain curve (the region in which maximum strain is created). The groups of PZTs for providing flexural vibration need not be disposed in spaced apart relationship with each other as shown in Figures 12 -14. Rather, it is more advantageous in manufacturing that the groups are closely adjacent to each other. The reason is that a metal block b 3 shown in Figures 12 - 14 becomes unnecessary, that the electrode on the boundary surface between the groups can be made common to the groups because the groups are closely adjacent to each other and that the groups can be assembled with the electrode phases of the PZTs of the groups brought into a desired positional relation in advance, and in this case, if necessary, metal blocks b 1 and b 2 can be joined together for formation before they are coupled together by a bolt. Examining the conditions hitherto described with respect to the vibration member of this type, the strain distribution of the vibration member shown in Figure 4 is as shown in Figure 7. In this case, the B phase piezo-electric element a 2 is disposed at a position whereat strain is great as compared with that of the A phase piezo-electric element a 1 , and the admittance during the driving of the B phase piezo-electric element a 2 is always great as compared with the admittance during the driving of the A phase piezo-electric element a 1 . In the present embodiment (Figure 1), in order to correct this, E (see Figure 7) which is the boundary surface between the A phase and B phase piezo-electric elements a 1 and a 2 is moved to the maximum point D of the strain distribution (i.e., the maximum point D of the vibration amplitude), and the rear metal block b 2 is made short and the fore metal block b 1 is made long. An embodiment shown in Figure 9, like the embodiment shown in Figure 1, achieves the coincidence between the maximum value position of the vibration member utilizing a secondary flexural moment and the boundary surface between the A phase piezo-electric element a 1 and the B phase piezo-electric element a 2 , and in this embodiment, as compared with the embodiment shown in Figure 1, the maximum value position of strain is formed on the rear end side of the vibration member. In an embodiment shown in Figure 10, conversely from the embodiment shown in Figures 1 and 9, the minimum value position of the vibration member and the boundary surface between the A phase piezo-electric element a 1 and the B phase piezo-electric element a 2 are made coincident with each other. In the case of the present embodiment, the strain created in the boundary surfaces between fore end rear metal blocks b 2 and b 11 for obtaining a predetermined amplitude in the vibration member and the piezo-electric elements a 1 and a 2 and in the boundary surface between the piezo-electric elements is small and the mechanical loss therein decreases and thus, the motor efficiency is improved. Figure 15 shows a second embodiment of the present invention. In the present embodiment, like the vibration members shown in Figures 13 and 14, the A phase piezo-electric element a 1 is disposed between the fore metal block b 1 and the middle metal block b 3 and the B phase piezo-electric element a 2 is disposed between the middle metal block b 3 and the rear metal block b 2 , and the A phase piezo-electric element a 1 and the B phase piezo-electric element a 2 are disposed at positions equal in the longitudinal direction from the maximum position of the strain formed in the vibration member. The strains at these two positions are equal and thus, the amplitudes of flexural vibrations excited by the A phase and B phase piezo-electric elements a 1 and a 2 become equal to each other. Figure 16 shows the admittances during the driving of the A phase piezo-electric element a 1 and the B phase piezo-electric element a 2 . In this case, the two admittances substantially coincide with each other, and the vibration displacement locus at each point on the vibration member when the A phase piezo-electric element a 1 and the B phase piezo-electric element a 2 are driven by the same voltage becomes circular, and the sliding loss between the movable member and the vibration member decreases and the motor efficiency is improved. Figure 17 shows a third embodiment of the present invention. In each of the above-described embodiments, electro-mechanical energy conversion elements for exciting a flexural vibration have been considered to be unit comprising one set of two elements, but a similar effect will be obtained even if they are separately disposed. That is, assuming that a flexural vibration is excited by piezo-electric element plates a 1 -1 and a 1 -2 and a flexural vibration is excited by piezo-electric element plates a 2 -1 and a 2 -2, if these four piezo-electric element plates are disposed at a position of the construction shown in Figure 17 wherein the strain distribution varies substantially linearly, the strain in the piezo-electric element plate a 1 -1 is great and the strain in the piezo-electric element plate a 1 -2 is small and thus, the strain per one phase, i.e., the sum of the strains in the two piezo-electric element plates becomes substantially equal to the strain per the other phase, i.e., the sum of the strains in the piezo-electric element plates a 2 -1 and a 2 -2. Figure 11 shows a driving apparatus for the photo-taking lens of a camera utilizing the bar-shaped ultrasonic motor of one embodiment of the present invention as a drive source. In Figure 11, the letter i designates an output take-out gear which is coupled to a movable member d through anti-vibration butyl rubber o. A connection gear j has mounted thereon an encoder slit plate k and a photocoupler m for detecting the position of said lens, and these detect the rotated position of the gear. Figures 18A - 18F show an embodiment of the ultrasonic motor according to the present invention, Figure 18A being a schematic view of the vibration member thereof. In the present embodiment, a vibration member 100A is formed in a construction similar to the example of the prior art, and piezo-electric element plates 103 and 104 shown in Figures 18D and 18E are sandwiched and fixed between vibratory resilient members 100 and 102 made of a metal (SUS, Bs, Al, INVAR or the like). The piezo-electric element plates 103 and 104, as shown in Figures 18D and 18E, each have positive and negative polarized patterns formed on the opposite sides of the diametrical portion thereof, and are disposed with a phase difference of 90° therebetween. When magnetic fields of the same direction are applied to these piezo-electric element plates 103 and 104 in the direction of the thickness thereof, the piezo-electric element plates 103 and 104 are deformed as indicated by broken line in Figure 18F. Accordingly, if the electric fields are alternating ones and the frequencies thereof are adjusted to the natural frequency of the flexure of the vibration member, the vibration member will make flexural resonation (the amplitude distribution in the radial (r) direction shown in Figures 18A and 18B). Also, since the piezo-electric element plate 104 is disposed with a phase difference of 90° with respect to the piezo-electric element plate 103, the flexural vibration created thereby is flexural vibration having a phase difference of 90° in a direction  with respect to the flexural vibration created by the piezo-electric element plate 103. Further, by a time phase difference of 90° being provided between the flexural vibration created by the piezo-electric element plate 104 and the flexural vibration created by the piezo-electric element plate 103, the particles on the surface of the vibration member make circular or elliptical motion. Figure 18C shows the strain distribution in the z direction of the side of the vibration member corresponding to the amplitude distribution in the r direction. The position at which the piezo-electric element plates 103 and 104 are sandwiched and fixed is selected to the antinode position of the inherent vibration mode for driving shown in Figure 18B at which the strain becomes greatest. Now, considering the equivalent circuit of the vibration member, there is only a resistance component on the mechanical arm side during resonation, as shown in Figure 19. Accordingly, supplied electric power is P = Vi 1 , but i 1 is determined by the total amount of strain of the piezo-electric element plates (the piezo-electric elements create charges by strain). That is, by the piezo-electric element plates 103 and 104 being disposed at a position whereat strain is great, as shown in Figure 18C, i.e., the antinode position of the strain, the electric current becomes great and the voltage becomes small and thus, there is provided a construction of low voltage. Even where as shown in Figures 20A - 20C, a piezo-electric element plate 110 for vibration detection is provided, it is necessary in the construction of the low voltage type to provide the piezo-electric element plates 103 and 104 for driving at the maximum strain position as in the case shown in Figures 18A - 18F. Figures 21A-21D show another embodiment. This embodiment is one in which the vibration member has a constricted portion, and in the vibration mode shown in Figure 21D, the maximum strain position and the vibration antinode position are not coincident with each other as shown in Figures 21B and 21C, but the piezo-electric element plates 103 and 104 are disposed in the constricted portion which is the maximum strain position. Again in this case, as in the embodiment shown in Figures 18A - 18F, there is the effect as the low voltage type. When in actual mounting or manufacturing, it is difficult to dispose the piezo-electric element plates 103 and 104 in the constricted portion, the piezo-electric element plates 103 and 104 may be provided on the opposite sides of the antinode in which strain is next greatest, as shown in Figures 22A - 22C. Figure 23 shows still another embodiment. This embodiment is similar in outward appearance to the embodiment of Figures 22A - 22C, but the inner diameters of the piezo-electric element plates 103 and 104 are made large and these piezo-electric element plates are disposed on the outer peripheral portion of the vibration member in which strain is great. In the present embodiment, the total amount of strain somewhat decreases, but since the piezo-electric element plates 103 and 104 are disposed only on the opposite sides of the maximum strain position in the axial and radial directions of the vibration member, the strain per unit volume of the piezo-electric element plates 103 and 104 becomes greatest, and such location of disposition can be effectively utilized and the number of piezo-electric elements required may be small. Also, the area of contact between the piezo-electric element plate 103 and the fore vibratory resilient member 100 and the area of contact between the piezo-electric element plate 104 and the rear vibratory resilient member 102 decrease and therefore, the friction loss resulting from sliding therebetween can be made small. Figure 24 shows an embodiment in which the barrel of an optical lens is driven by the use of the motor according to one embodiment of the present invention. The reference numeral 112 designate a gear joined coaxially with a movable member 108 to transmit the rotational output of the motor to a gear 113 and rotate the lens barrel 114 of a camera which has a gear meshing with the gear 113. An optical type encoder slit plate 115 is disposed coaxially with the gear 113 to detect the rotated positions and rotational speeds of the movable member 108 and the lens barrel 114, and detects the positions and speed by a photocoupler 116. Figures 25A - 25F show an embodiment of the ultrasonic motor according to the present invention. The vibration member A of the present embodiment, as shown in Figure 25A, is similar in basic construction to the example of the prior art, and piezo-electric element plates 203 and 204 shown in Figures 25D and 25E are sandwiched and fixed between resilient members made of a metal (SUS, Bs, Al, ZNUAR or the like). The piezo-electric element plates 203 and 204 each are polarized in opposite directions with the non-electrode portion of the diametrical part thereof as a boundary, and when electric fields of the same direction are applied to the two polarized areas in the direction of the thickness thereof, the piezo-electric element plates are deformed into a shape as indicated by dotted line in Figure 25F. Accordingly, if the electric fields are alternating ones and the frequencies thereof are adjusted to the natural frequency of the flexure of the vibration member, the entire vibration member will make resonation of flexural mode, as shown in Figure 25B. On the other hand, the piezo-electric element plates 203 and 204 are disposed with a phase difference of 90° therebetween and therefore, flexural vibrations created by these two piezo-electric element plates 203 and 204 have a phase difference of 90° therebetween in a direction . Accordingly, by a time phase difference of 90° being provided between the flexural vibration created by the piezo-electric element plate 204 and the flexural vibration created by the piezo-electric element plate 203, the particles on the surface of the vibration member make circular or elliptical motion and at that time, the strain distribution in the z (axial) direction of the side of the vibration member corresponding to the amplitude distribution in the r direction shown in Figure 25B becomes such as shown in Figure 25C. Description will now be made of the position at which a piezo-electric element plate for enhancing the efficiency of the motor is disposed. To obtain a certain constant motor output, if energy dispersed by the other members than the vibration member is made constant with the other conditions such as the support of the vibration member, the structure of the movable member (rotor) and the sliding material being fixed, the vibration energy being accumulated (created) by the vibration member need be of a certain predetermined amount. Now, the energy to be supplied in order to obtain a certain amount of vibration energy is determined by the attenuation constant of the entire vibration member. The vibration member is comprised of a combination of a vibration structure made of a metal (such as aluminum, brass or stainless steel) and a piezo-electric element plate. Also, the attenuation constant inherent to a material is small for metals, and the attenuation constant of the piezo-electric element plate having the piezo-electric property is relatively great. Q of metals is of the order of 3000 - 10000, and Q of the piezo-electric element plate is of the order of 20 - 1800. Accordingly, to decrease the loss in the vibration member, i.e., the internal friction loss caused by the material being distorted (although there are other losses including the radiation loss into the air and the dielectric material loss in the piezo-electric element plate, these losses are small), it is desirable that the piezo-electric element plate having a relatively great attenuation constant be disposed in a portion of small strain. So, in the present embodiment, the position of the antinode of vibration at which strain is great is avoided and piezo-electric element plates are disposed before and behind the position of the middle node. In fact, Q of the vibration member when the piezo-electric element plates 203 and 204 were disposed at the antinode position of vibration was of the order of 1000, but in the present embodiment, it has been improved to the order of 1500. Also, at the node of vibration near the opposite ends of the vibration member A, strain is not zero but is small as compared with that near the antinode of vibration and therefore, even if the piezo-electric element plates 203 and 204 are disposed at this node position, some improvement in the motor efficiency can be expected. Strain is zero at the opposite ends of the vibration member, but it is impossible in the structure of the present motor to dispose the piezo-electric element plates at these positions. Figures 26A - 26C show another embodiment. In this embodiment, as in the embodiment described above, the piezo-electric element plates 203 and 204 are disposed before and behind the node position of vibration, but the outer diameters of the piezo-electric element plates 203 and 204 are made small and the piezo-electric element plates 203 and 204 are disposed inside the vibration member of small strain. By adopting such structure, the internal loss in the vibration member becomes smaller than in the embodiment of Figures 25A - 25F. In the present invention, the shape of the vibration member is not limited to the pencil-like shape, but may also be a shape having a constricted portion in the intermediate portion, as shown in Figures 26A and 26B, or a shape having a large diameter in the opposite end portions, as shown in Figures 27A and 27B. Also, where as shown in Figures 28A and 28B, the vibration member is supported at the node position of vibration by a support member comprising a resilient bar or a resilient plate, there will be substantially no problem even if the piezo-electric element plates 203 and 204 are disposed somewhat off the node position of vibration. Figure 29 shows an example of the construction in a case where the barrel of an optical lens is driven by the use of the motor according to one embodiment of the present invention. The reference numeral 209 denotes a gear joined coaxially with a movable member R to transmit the rotational output of the motor to a gear 210 and rotate the lens barrel 211 of a camera which has a gear meshing with the gear 210. As described above, according to one embodiment of the present invention, the motor efficiency can be improved by simple structure in which electro-mechanical energy conversion elements such as piezo-electric element plates are disposed at or near the node position of vibration for driving.

Claims: A vibration driven actuator, comprising: a vibration member (b 1 ,b 2 ,b 3 ,100,102,101,201,202,1,2) elongated along an axis and having an asymmetrical shape along said axis and a substantially symmetrical shape about said axis; a first electro-mechanical energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3) functionally and coaxially coupled to an intermediate portion of said vibration member (b 1 , b 2 , b 3 , 100,102,101,201,202,1,2) substantially symmetrically about said axis, and arranged for generating a first flexural vibration having a first direction in said vibration member in response to a first electrical signal; and a second electro-mechanical energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) functionally and coaxially coupled to an intermediate portion of said vibration member (b 1 ,b 2 ,b 3 ,100,102,101,201,202,1,2) substantially symmetrically about said axis, arranged at a rotated position about said axis with respect to said first energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3), and arranged for generating a second flexural vibration having a second direction different from said first flexural vibration in response to a second electrical signal, thereby to generate a rotating vibration as a result of the combination of the first flexural vibration and the second flexural vibration in said vibration member (b 1 ,b 2 ,b 3 ,100,102,101,201,202,1,2) and an asymmetrical strain distribution along said axis in said vibration member (b 1 ,b 2 ,b 3 ,100,102,101,201,202,1,2) and said first and second energy conversion members (a 1 ,a 2 ,a 1-2 , a 1-2 ,a 2-1 ,a 2-2 ,103,104,203,204,3,4); characterized in that said first energy conversion member (a 2 ,a 2-1 , a 2-2 ,104,204,4) and said second energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) are located at predetermined positions along said axis whereat strains created in said first and second energy conversion members (a 1 ,a 2 ,a 1-1 ,a 1-2 , ,a 2-1 ,a 2-2 ,103,104,203,204,3,4) by the application of said first and second electrical signals are substantially equal to each other. A vibration driven actuator according to claim 1, wherein said first energy conversion member (a 1 ,a 1-1 , ,a 1-2 ,103,3) is arranged for generating the first flexural vibration at a first phase in response to said first electrical signal and said second energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) is arranged for generating the second flexural vibration at a second phase in response to said second electrical signal, wherein said second electrical signal has a phase difference in time with respect to said first electrical signal. A vibration driven actuator according to claim 2, wherein said phase difference in time is 90°. A vibration driven actuator according to claim 1, 2 or 3, wherein said second energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) is arranged rotated at 90° about said axis relative to said first energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3). A vibration driven actuator according to any one of claims 1 to 4, wherein said first energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3) includes a linear insulation portion extending diametrically from said axis for insulating a first section lying to one side of said axis and a second section lying to another side of said axis, and said second energy conversion member (a 2 ,a 1-2 ,a 2-2 , 104,204,4) includes a linear insulation portion extending diametrically from said axis for insulating a first section lying to one side of said axis and a second section lying to another side of said axis. A vibration driven actuator according to any preceding claim, wherein said first energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3) and said second energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) are arranged on said axis either side of an axial position at which the strain in said vibration member (b 1 ,b 2 ,b 3 , 100,102,101,201,202,1,2) generated by said flexural vibration is substantially a maximum. A vibration driven actuator according to any of claims 1 to 5 wherein said first energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3) and said second energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) are arranged on said axis symmetrically either side of an axial position at which the strain in said vibration member (b 1 ,b 2 ,b 3 , 100,102,101,201,202,1,2) generated by said flexural vibrations is substantially a minimum. A vibration driven actuator according to any one of claims 1 to 5 wherein said vibration member (b 1 ,b 2 ,b 3 ,100,102,201,202,1,2) is arranged to have a strain distribution in the direction of said axis which is in part substantially linear, the strain being generated by said flexural vibrations; and said first energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3) comprises two first energy conversion elements (a 1-1 ,a 1-2 ) arranged axially spaced and said second energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) comprises two second energy conversion elements (a 2-1 ,a 2-2 ), said first energy conversion element (a 1-1 ,a 1-2 ) being arranged along said axis either side of said second energy conversion elements (a 2-1 ,a 2-2 ) at a position where said strain distribution in said vibration member (b 1 ,b 2 ,b 3 ,100,102,101, 201,202,1,2) is substantially linear. A vibration driven actuator according to any preceding claim wherein said first energy conversion member (a 1 ,a 1-1 ,a 1-2 ,103,203,3) and said second energy conversion member (a 2 ,a 2-1 ,a 2-2 ,104,204,4) are arranged adjacently. A vibration driven motor comprising the vibration driven actuator according to any preceding claim, and a contact member (d,R) having a centre of rotation, said contact member (d,R) being driven to rotate about its centre of rotation by said vibration member (b 1 ,b 2 ,100,102).

Inventors: MAENO TAKASHI, TSUKIMOTO TAKAYUKI, MAENO, TAKASHI, TSUKIMOTO, TAKAYUKI, MAENO, TAKASHI, C/O CANON KABUSHIKI KAISHA, TSUKIMOTO, TAKAYUKI, C/O CANON KABUSHIKI KAISHA
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1991
Main classification: H01L41
IPC codes: H01L41, H02N2