Vibration wave driven motor

Abstract: In a vibration wave driven motor wherein an AC electric field is applied to an electro- mechanical energy conversion element secured to an elastic member to thereby excite a plurality of standing waves differing in phase from each other in the elastic member and a travelling wave is formed in the elastic member by the combination of the standing waves, whereby a member which is in pressure contact with the elastic member and the elastic member are moved relative to each other by a frictional force, provision is made of means for making the contact pressure on the surface of contact between the elastic member and the member which is in pressure contact with the elastic member non-uniform, and means for making the dynamic rigidity of a vibration member non-uniform in an unnecessary vibration mode created by the means for making the contact pressure non-uniform, whereby the occurrence of noise is prevented by simple and inexpensive means.

Description: This invention relates to a vibration wave driven motor in which electrical energy is converted into vibration energy by an electro-mechanical energy conversion element and a mechanical output is obtained from the vibration energy through friction. Generally, a vibration wave driven motor is comprised of a vibration member having an electro-mechanical energy conversion element such as a piezo-electric element secured to an elastic member, and a movable member brought into pressure contact with the elastic member, and is such that an AC voltage is applied to the two driving phases of the piezo-electric element to excite a travelling wave in the elastic member and the elastic member and the movable member are moved relative to each other by the vibration energy by the travelling wave through the frictional force with the movable member and said relative movement is used as the output of the motor. From this fact, the elastic member is formed of a material of small vibration loss (internal loss) for the purpose of improving the efficiency of the motor, and as the material of the elastic member, use is made of a material of very high Q, e.g. Q=100-300 so that vibration may be readily generated by small energy. Now, in such a vibration wave driven motor, the movable member is in a state in which it is pressed against the elastic member to take out the output of the motor and therefore, the elastic member is subjected to a vertical force (a force in the direction of pressure contact) and a frictional force (a moment by a frictional force) during the driving of the motor, and in some cases, other vibrations than the driving wave are also excited due to such forces. These vibrations are chiefly the natural vibrations of the vibration member (though the vibration member is weakly compounded with the movable member through a frictional force), and provide noise when the frequencies of these vibrations are within an audible range. Also, even if the frequencies of these vibrations themselves are not within the audible range, there will be created the difference thereof from the vibration frequency of the driving mode and a component harmonic wave by the non-linearity of the vibration of the vibration member in a state in which it is combined with the movable member, and if these are within the audible range, they will pose a problem as noise. Motors of various types have been made for trial purposes and a study made of the vibration mode when the problem of noise arises. As a result, it has been found that there are chiefly two types of noise, one of which is a component harmonic wave of the driving mode created by forced vibration and the other is self-excited vibration created by a frictional force. It has further been found that the cause of creation of the latter self-excited vibration is divided chiefly into two cases, i.e., a case where it is determined by the dimensions of the movable member and the vibration member, and the dynamic rigidity, friction constant, etc. of the contact portion, and a case where it is caused in a mode one order lower than the driving wave (the out-of-plane mode), irrespective of the dimensions. Further examination of the situation in which the self-excited vibration occurs in the vibration mode one order lower than the driving wave (the out-of-plane mode) has found that the self-excited vibration occurs when the contact between the movable member and the elastic member is not kept uniform. Figure 2 of the accompanying drawings shows a typical example of the vibration spectrum at such time. The vibration member used is a circular ring-shaped one. The ordinate represents the output from a sensor layer provided on the vibration member (a sensor layer which produces a voltage conforming to the vibration of the vibration member by the piezo-electric effect, and the abscissa represents frequency. "f" represents the characteristic in the driving vibration mode (the out-of-plane flexure 7th-order mode of the circular ring), and "g" represents the characteristic in the vibration mode which has occurred as the self-excited vibration by a frictional force, i.e., the characteristic of the vibration in the mode one order lower than the characteristic "f", i.e., the out-of-plane flexure 6th-order mode. A characteristic "h" is the difference between the characteristic "f" and the characteristic "g", and vibration of about 8 kHz of this characteristic causes noise. Thus, it has been confirmed empirically that if there is irregularity of contact (irregularity of pressure) between the elastic member and the movable member, the vibration mode one order lower than the driving wave (i.e., vibration having a number of waves less by one than the number of waves of the driving wave) occurs and any other unwanted vibration mode than this vibration mode, for example, the vibration mode two orders lower than the vibration mode of the driving wave, does not occur. That is, it has been found that when there is irregularity of contact (irregularity of pressure), the vibration which causes noise is limited to the vibration of the mode one order lower than the driving mode. Also, the examination of the noise when the irregularity of contact (the irregularity of pressure) is small has found that the noise vibration mode changes depending on the structure, materials, friction constants, driving order numbers, etc. of the movable member and elastic member, but in the case of the driving of seven waves, the driving wave is limited to one of three, four, five and six waves or a combination thereof. Figure 9 of the accompanying drawings shows a typical example of the noise when the irregularity of pressure is null. "f" represents the characteristic of the driving vibration mode, "k" represents the characteristic of the 3rd-order vibration mode, and "j" represents the characteristic of the 4th-order vibration mode. It has been found from what has been described that where there is adopted structure in which no irregularity of pressure occurs, for a case where the driving wave comprises seven waves, a mode free of noise can be realized if a countermeasure for noise is applied to the 3rd-order, 4th-order, 5th-order and 6th-order modes. On the other hand, it has already been proposed in U.S. Application Serial No. 480,201 filed on February 14, 1990 to provide a portion of non-uniform rigidity in the elastic member or the like as a countermeasure for noise. The principle of driving of the vibration wave driven motor is that by an AC electric field being applied to the piezo-electric element, two standing waves positionally deviating from each other by π/2, i.e., a standing wave of sin mode and a standing wave of cos mode, are excited in the elastic member and a travelling wave is formed by the combination of the two standing waves, and if a difference occurs between the natural frequencies of the two standing waves, a travelling wave will no longer be formed. From this, it follows that to prevent the generation of a travelling wave of an order number which causes noise, a difference in natural frequency may be provided between two standing waves in that order number. As a method of providing a difference between the natural frequencies of standing waves, for example in a case where the elastic member is of an annular shape and a plurality of slits are formed at equal pitches in the upper surface thereof along the circumferential direction thereof, the depth of the slit at a location corresponding, for example, to the node of one standing wave but to the antinode in the other standing wave is made greater than the depth of the other slits, whereby it becomes possible to provide a difference between the natural frequencies. A concern of the present invention is to provide a vibration wave driven motor which suffers little from the occurrence of noise. It is another concern of the present invention to provide a vibration wave driven motor which is inexpensive and suffers little from the occurrence of noise. It is still another concern of the present invention to forcibly create a mode of an order number of one order lower than the order number of the driving mode, and suppress the creation of that mode for such an order number by the action of the above-described portion of non-uniform dynamic rigidity and as a result, prevent the occurrence of noise. It is yet still another concern of the present invention to provide a vibration wave driven motor including a member for forcibly creating a mode of an order number one order lower than the order number of the driving mode. According to the present invention, there is provided a vibration wave driven motor having features as recited in claim 1. In the accompanying drawings: Figure 1 is a partly cut-away perspective view showing Embodiment 1 of a vibration wave driven motor according to the present invention. Figure 2 is a graph showing a vibration spectrum. Figure 3 is a perspective view showing a modification of Embodiment 1. Figure 4 is a partly cut-away perspective view of Embodiment 2. Figure 5 is a perspective view of Embodiment 3. Figure 6 is a perspective view of Embodiment 4. Figure 7 is a perspective view of Embodiment 5. Figure 8 is a partly cut-away perspective view of Embodiment 6. Figure 9 is a graph showing a vibration spectrum. Embodiment 1 Figure 1 is a partly cut-away perspective view showing Embodiment 1 of a vibration wave driven motor according to the present embodiment. In this embodiment, the driving is the driving when the driving wave comprises seven waves, that is, the driving in the 7th-order driving mode. In Figure 1, the reference character a designates an elastic member formed into a circular ring-like shape and having a piezo-electric element P as an electro-mechanical energy conversion element adhesively secured to the back thereof. A number of slits S are formed at equal pitches in the upper surface of the elastic member a , and among these slits S, several (in the present embodiment, six) slits S-1 are formed more deeply than the other slits, and a portion of non-uniform dynamic rigidity is provided by these slits S-1 as previously described, whereby the generation of a travelling wave of six waves (6th-order) smaller by one than the number of waves for driving may be suppressed. That is, even in a situation wherein there is generated a travelling wave of six waves which is the cause of noise which is the only unwanted vibration caused by the pressure between a vibration member and a movable member being made non-uniform, the generation of such travelling wave of six waves is suppressed by these slits S-1. The reference character b denotes an annular movable member, and the reference character c designates rubber. A plurality of rollers d are disposed on the upper surface of the rubber c , and a pressing structure e is disposed on these rollers d . When such structure is adopted and an electrical signal is supplied to the piezo-electric element P, a travelling wave is formed in a conventional manner. The movable member b frictionally driven by this travelling wave is rotated and it is possible to accelerate and decelerate the motor through the intermediary of the rollers d . Also, by the rollers d , three portions in which surface pressure is high are forcibly created on the contact driving surface between the elastic member a and the movable member b . Thus, due to the non-uniformity of this surface pressure forcibly created, there is generated the 6th-order mode one order lower than the driving mode (the 7th-order driving mode), that is, there is generated a travelling wave of six waves, but the generation of the travelling wave of six waves is suppressed by the action of the portion of non-uniform rigidity provided by the six slits S-1 which is associated with the 6th-order vibration mode, with a result that the occurrence of noise is suppressed. As shown in Figure 3, balls d 2 may be used instead of the rollers d to obtain a similar effect. By threading a shaft through each ball d 2 , the output can be taken out. Also, the output of the motor may be directly transmitted from the movable member b to a load, for example, the photo-taking lens driving mechanism of a camera. Embodiment 2 Figure 4 shows Embodiment 2. In this embodiment, as in Embodiment 1, the creation of the unnecessary vibration mode of six waves is hampered by the action of six slits S-1 formed in the elastic member a . Also, the non-uniformity of the surface pressure is created by divisionally disposing rubber c 2 . Embodiment 3 Figure 5 shows Embodiment 3. In this embodiment, the elastic member a designed to hamper the creation of the unnecessary vibration mode by the action of slits S-1 formed in the elastic member a is held by coil springs i disposed at three locations, whereby irregularity of pressure is created. Embodiment 4 Figure 6 shows Embodiment 4. In this embodiment, the elastic member a shown in Figure 1 is deformed into a twofold state about the axis ℓ thereof to thereby create irregularity of pressure. If the amount of this fold is of the order of several µm (the order of the vibration amplitude of the driving mode), there may be caused noise by irregularity of pressure. The elastic member a may be deformed into a threefold or fourfold state to thereby create irregularity of pressure likewise. Embodiment 5 Figure 7 shows Embodiment 5. In this embodiment, as shown, two of the slits S formed in the elastic member a are partly thinned out in the circumferential direction thereof (see D) and the pitches of the slits S are made unequal to thereby create irregularity of pressure, and as in the above-described embodiments, slits S-1 for suppressing the occurrence of the unnecessary vibration mode (the vibration mode one order lower than the driving mode) by the portion of non-uniform dynamic rigidity are formed in the elastic member a . Embodiment 6 Figure 8 shows Embodiment 6. In this embodiment, irregularity of pressure is created by the surface deformation of a vibration member caused by a plurality of support member r disposed on a fixing member q to which the vibration member is fixed, and portions of non-uniform dynamic rigidity are provided by cut-away portions 1-q formed at equal pitches at six locations on the circumference of the fixing member q, thereby providing a countermeasure for preventing noise. The mechanism or structure for creating irregularity of pressure in each of the above-described embodiments may often depend upon such factors as manufacturing cost, etc. in the actual mounting of the motor. The structures of the respective embodiments can also be combined together. Also, only the method of making the grooves (slits) deep has been shown as means for providing the portions of non-uniform dynamic rigidity at a pitch integer times as great as the 1/2 wavelength of the vibration mode one order lower than the driving vibration mode, but conversely, the above-described various kinds of pressure irregularity creating means can also be constructed by making the grooves (slits) shallow or by adding a mass, whereby an effect similar to that described above can be obtained. As has hitherto been described, according to the present invention, a vibration mode which is one order lower than the driving vibration mode and in which noise can occur is forcibly created by the means for making the contact pressure between the vibration member and the movable member non-uniform, whereby the occurrence of any other unnecessary vibration mode than that vibration mode, i.e., a vibration mode still lower than the aforementioned one-order lower vibration mode, is eliminated. The occurrence of the afore-described forcibly created unnecessary vibration mode can be prevented by other means, i.e., the means for making the dynamic rigidity non-uniform, with a result that the occurrence of noise can be prevented. The present invention is also applicable to a motor in which, conversely to the above-described embodiments, a vibration member comprising an elastic member and a piezo-electric element is movable and a movable member side element which is other constituent is fixed.

Claims: A vibration wave driven motor comprising: a vibration member (a, P) for generating a travelling vibration wave therein in response to an applied electrical signal; a contact member (b) having a contact portion which is in contact with a contact portion of said vibration member and arranged to receive the travelling vibration wave from the contact portion of said vibration member, whereby the travelling vibration wave creates relative movement between the vibration member and the contact member; and means (S, S-1) for making the dynamic rigidity of the vibration member non-uniform; characterised in that pressure means (d, d2, i) are provided for making the contact pressure between the contact portion of said vibration member and the contact portion of said contact member (b) non-uniform, whereby said pressure means in combination with said means (S, S-1) for making the dynamic rigidity non-uniform suppress any unwanted vibration mode created in the vibration member when the electrical signal is applied to the vibration member. A vibration wave driven motor as claimed in claim 1, characterised in that said unwanted vibration mode is a vibration mode one order lower than a mode of predetermined travelling vibration wave. A vibration wave driven motor as claimed in claim 1 or 2, characterised in that said means for making the dynamic rigidity non-uniform is provided on the vibration member at a pitch about n times as great as the half wavelength of said unwanted vibration mode where n is an integer. A vibration wave driven motor as claimed in claim 1, 2 or 3, characterised in that a member (e) is provided to apply force to said pressure means (d, d2) for applying pressure between the contact portion of said vibration member (a, P) and the contact portion of said contact member (b). A vibration wave driven motor as claimed in claim 4, characterised in that said pressure means comprise rollers (d). A vibration wave driven motor as claimed in any one of claims 1-4, characterised in that said pressure means comprise a plurality of balls (d2). A vibration wave driven motor as claimed in claim 4, characterised in that said pressure means comprise support members provided only on a portion of said contact member. A vibration wave driven motor as claimed in claim 7, characterised in that said support members comprise a plurality of divided pieces (c2). A vibration wave driven motor as claimed in claim 8, characterised in that said pieces are rubber pieces (c2). A vibration wave driven motor as claimed in claim 1 or 2, characterised in that said pressure means includes springs (i) provided at a plurality of locations on said vibration member. A vibration wave driven motor as claimed in claim 1 or 2, characterised in that said pressure means includes a member for keeping said vibration member curved.

Inventors: ATSUTA AKIO, CHIBA ICHIRO, KANAZAWA HAJIME, KOREEDA SHINICHI, MAENO TAKASHI, MUKOHJIMA HITOSHI, TSUKIMOTO TAKAYUKI, ATSUTA, AKIO, CHIBA, ICHIRO, KANAZAWA, HAJIME, KOREEDA, SHINICHI, MAENO, TAKASHI, MUKOHJIMA, HITOSHI, TSUKIMOTO, TAKAYUKI, ATSUTA, AKIO, C/O CANON KABUSHIKI KAISHA, CHIBA, ICHIRO, C/O CANON KABUSHIKI KAISHA, KANAZAWA, HAJIME, C/O CANON KABUSHIKI KAISHA, KOREEDA, SHINICHI, C/O CANON KABUSHIKI KAISHA, MAENO, TAKASHI, C/O CANON KABUSHIKI KAISHA, MUKOHJIMA, HITOSHI, 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