1. Field of the Invention
The present invention relates to a nonparallel-axes transmission mechanism and a robot.
2. Discussion of the Background
Nonparallel-axes transmission mechanisms transmit power between nonparallel axes and are employed in many kinds of machines such as at joints of robots. Intersecting-axes transmission mechanisms are among the most frequently used nonparallel-axes belt transmission mechanisms. Some intersecting-axes transmission mechanisms are used in differential forms.
Bevel gears are among the most popular nonparallel-axes transmission mechanisms. Generally, bevel gears involve large backlashes due to the need for ensuring some degree of clearance for minimized friction. Bevel gears also need highly rigid materials to avoid chipping on teeth, resulting in heaviness in weight. In an attempt to address these technical circumstances, Japanese Unexamined Patent Application Publication No. 3-505067 discloses a nonparallel-axes transmission mechanism that uses wires.
Wires transmit power only in their directions of pull. In view of this, Japanese Unexamined Patent Application Publication No. 3-505067 discloses a pair of stepped pulleys of intersecting rotation axes, with wires wound on the pulleys in opposite directions so as to provide bi-directional rotary transmission. Some other nonparallel-axes transmission mechanisms use belts (see, for example, Ito, Shigeru. Dictionary of Mechanisms, Rikogakusha Publishing Co., Ltd., May 10, 1983, pp. 108-112).
According to one aspect of the present invention, a nonparallel-axes transmission mechanism includes a plurality of pulleys, support shafts, and a transmission medium. The plurality of pulleys include a first pulley and a second pulley. The first pulley includes a first rotation axis and a first conical pulley. The first conical pulley forms a first imaginary conical surface. The first imaginary conical surface forms a cone including a first center line identical to the first rotation axis. The first imaginary conical surface includes a first apex. The second pulley includes a second rotation axis and a second conical pulley. The second rotation axis is not parallel to the first rotation axis. The second conical pulley forms a second imaginary conical surface. The second imaginary conical surface forms a cone including a second center line identical to the second rotation axis. The second imaginary conical surface includes a second apex that matches the first apex. The support shafts include a first support shaft and a second support shaft. The first support shaft rotatably supports the first pulley. The second support shaft rotatably supports the second pulley. The transmission medium is configured to, when power is input to the first pulley, transmit the power from the first pulley to the second pulley. The transmission medium includes a fan belt including a fan shape in a developed plan view. The fan belt is in contact with the first imaginary conical surface and with the second imaginary conical surface. The first conical pulley includes a shape of the first imaginary conical surface removing a shape of the fan belt in contact with the first imaginary conical surface. The second conical pulley includes a shape of the second imaginary conical surface removing a shape of the fan belt in contact with the second imaginary conical surface.
According to another aspect of the present invention, a robot includes a plurality of arms and a joint. The joint pivotably or rotatably couples the plurality of arms to each other. The joint includes the above-described nonparallel-axes transmission mechanism.
A more complete appreciation of the invention and many of the attendant advantages thereof will be readily obtained as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings, wherein:
The embodiments will now be described with reference to the accompanying drawings, wherein like reference numerals designate corresponding or identical elements throughout the various drawings.
While the term “cone” is used for convenience sake, the imaginary conical surface of each of the conical pulleys 1 and 2 may not necessarily form an apexed cone. In operation, it suffices that each imaginary conical surface be conical at the portions of contact with the fan belts. The conical pulleys 1 and 2 abut on one another such that the apexes of the respective imaginary conical surfaces match. That is, the rotation axis 5 and the rotation axis 6 intersect at the apexes of the respective imaginary conical surfaces. As used herein, the term “fan belt” is defined as a belt having a fan shape in a developed plan view. While the term “fan shape” is used, the fan belt may not necessarily have an apexed fan shape. In operation, the term “fan shape” encompasses a band shape drawing an arc as shown in
Hence, the conical shape of each of the conical pulleys 1 and 2 has a radius smaller than the radius of the corresponding imaginary conical surface 7 by half the belt thickness. The conical pulleys 1 and 2 are disposed with the respective imaginary conical surfaces 7 in contact with one another, and this leaves a gap between the conical pulleys 1 and 2 corresponding to the thickness of the fan belts 3 and 4. The outer radius of each fan belt in a developed view, as shown in
The contact surface between the imaginary conical surface of the conical pulley and the fan belt can be regarded as a part of the side surface of a truncated cone. In view of this, the conical pulley at its surface of contact with the fan belt can also be seen in a developed plan view, with a development radius and a development center angle of the conical pulley itself. The portion of contact between the conical pulley 1 and the fan belt 3 has the same development radius as the development radius at the portion of contact between the conical pulley 2 and the fan belt 3. Likewise, the portion of contact between the conical pulley 1 and the fan belt 4 has the same development radius as the development radius at the portion of contact between the conical pulley 2 and the fan belt 4. The radius of the bottom surface of each truncated cone will be hereinafter referred to as a “truncated cone bottom radius”. The angle defined between the generatrix and the rotation axis of the cone will be hereinafter referred to as a “cone angle”. The geometry of the belt transmission mechanism of this embodiment is designed by first determining: a truncated cone bottom radius r1 formed by the conical pulley 1 and the fan belt 3, a truncated cone bottom radius r2 formed by the conical pulley 2 and the fan belt 3, and an angle ψ formed by the rotation axis 5 and the rotation axis 6. These values are used to determine the development radius R of the fan belt 3, the cone angle θ1 of the conical pulley 1, and the cone angle θ2 of the conical pulley 2, while ensuring that the following relationships are satisfied.
These equations are solved to determine R, θ1, and θ2 in the following manner.
The development radius R′ of the fan belt 4 may be determined similarly to the fan belt 3, using a truncated cone bottom radius r1′ formed by the conical pulley 1 and the fan belt 4 and a truncated cone bottom radius r2′ formed by the conical pulley 2 and the fan belt 4. In this regard, the ratio between the truncated cone bottom radii r1′ and r2′ is made equal to the ratio between r1 and r2. Alternatively, the development radius r of the fan belt 4 may be first determined while avoiding overlapping with the fan belt 3, and then the truncated cone bottom radii r1′ and r2′ may be determined using the following equations.
r′
1
=R′ sin θ1
r′
2
=R′ sin θ2 Equations 3
In this embodiment, the pulleys are conical pulleys and the belts are fan belts, and the conical pulleys are disposed such that the respective apexes match. This ensures that power is transmitted between non-intersecting axes without twisting the belts.
Description will be made with regard to how the mechanism according to this embodiment operates. When the conical pulley 1 rotates about the rotation axis 5 in the clockwise direction as viewed from top, the fan belt 3 is wound up, causing the conical pulley 2 to rotate about the rotation axis 6 in the counterclockwise direction as viewed from top. Meanwhile, the fan belt 4 is wound up around the conical pulley 2, and thus kept from going slack or meeting with like occurrences. When the conical pulley 1 rotates about the rotation axis 5 in the counterclockwise direction as viewed from top, the fan belt 4 is wound up, causing the conical pulley 2 to rotate about the rotation axis 6 in the clockwise direction as viewed from top. Thus, the rotation of the rotation axis 5 is transmitted to the rotation axis 6, which is not parallel to the rotation axis 5. The transmission is accelerated or decelerated depending on the ratio between r1 and r2. In this embodiment, the fan belts 3 and 4 each are secured at both ends. In this case, the largest possible number of rotations to be transmitted is one. In view of this, at r1≦r2, the development center angle α of each of the fan belts 3 and 4 may be set as shown below. This makes the range of transmission of rotation as extensive as approximately one full rotation of the smaller pulley, which is the conical pulley 1.
At r1=r2, θ1 is π/4, and the development center angle α is as follows.
α=√2π Equation 5
If the thickness of each of the fan belts 3 and 4 is small enough to enlarge the respective development center angles and to wind each belt a plurality of turns, approximately a plurality of rotations can be transmitted. In practice, however, a belt superimposed on itself has a changing radius due to the thickness of the superimposition, which makes accurate transmission difficult.
In the second embodiment, a V ribbed belt is used as an exemplary fan belt.
That is, the rotation axes of the main conical pulleys 11 and 12 and the guide conical pulleys 17 and 18 intersect at the apexes of the respective imaginary conical surfaces. This arrangement of the conical pulleys turns the fan belt into loops of the same radii as the radii of the respective corresponding conical pulleys. This, in turn, ensures continuous transmission of a plurality of rotations. When the main conical pulleys 11 and 12 have large cone angles, the development center angle of the fan loop belt 13 might exceed 2π. Even in this case, a fan loop belt is realized by preparing a plurality of fan belts and joining them to each other into a loop.
Also in this embodiment, a determination is first made as to a truncated cone bottom radius r1 formed by the main conical pulley 11 and the fan loop belt 13, a truncated cone bottom radius r2 formed by the main conical pulley 12 and the fan loop belt 13, and an angle ψ formed by a rotation axis 15 and a rotation axis 16. These values are used to determine the development radius R of the fan loop belt 13, the cone angle θ1 of the main conical pulley 11, and the cone angle θ2 of the main conical pulley 12, using equations similar to the equations in the first embodiment. Additionally, the truncated cone bottom radius formed by the guide conical pulley 17 and the fan loop belt 13 is determined, and the truncated cone bottom radius formed by the guide conical pulley 18 and the fan loop belt 13 is determined. The truncated cone bottom radius of the guide conical pulley 17 may be different from the truncated cone bottom radius of the guide conical pulley 18. In this embodiment, however, both truncated cone bottom radii are denoted r3 for simplicity. The cone angle θ3 of each of the guide conical pulleys 17 and 18 is obtained using the following equation.
Description will be now made with regard to determination of the angle of the rotation axis of each of the guide conical pulleys 17 and 18, and determination of the development center angle of the fan loop belt 13 in this embodiment. When the guide conical pulleys 17 and 18 are the same in shape, the rotation axes of the guide conical pulleys 17 and 18 are symmetrical with the same angles. In view of this, the following calculations will be concerning the guide conical pulley 17 alone. The intersection point between the truncated cone bottom surface and the rotation axis of the main conical pulley 11 will be denoted N1. The intersection point between the truncated cone bottom surface and the rotation axis of the main conical pulley 12 will be denoted N2. The intersection point between the truncated cone bottom surface and the rotation axis of the guide conical pulley 17 will be denoted N3. Further in this embodiment, the contact point between the truncated cone bottom surface of the main conical pulley 11 and the truncated cone bottom surface of the main conical pulley 12 will be denoted R1. The truncated cone bottom surface of the main conical pulley 11 is in contact with the truncated cone bottom surface of the guide conical pulley 17, and the contact point will be denoted R2. The contact point between the truncated cone bottom surface of the main conical pulley 12 and the truncated cone bottom surface of the guide conical pulley 17 will be denoted R3. The vector in the direction from point A to point B will be denoted “vector A→B”. The apexes of the conical pulleys will be assumed an origin O, with a Z-axis assumed in the direction of the vector O→N1.
A Y-axis, which is perpendicular to the Z-axis, is assumed on the plane formed by the vector O→N1 and the vector O→N2. An X-vector is assumed in the direction of the cross product of the vector O→N2 and the vector O→N1. The angle defined between the vector N1→R1 and the vector N1→R2 will be denoted φ1. The angle defined between the vector N2→R1 and the vector N2→R3 will be denoted φ2. The angle defined between the vector N3→R3 and the vector N3→R2 will be denoted φ3. The point N3 is located on the O—N1—R2 plane and on the O—N2—R3 plane. Hence, determining the angles φ1 and φ2 ensures determination of the rotation axis direction of the guide conical pulley 17. Also, once the angles φ1, φ2, and φ3 are determined, the development center angle α of the fan loop belt 13 is determined using the following equation.
n
3z
=R cos θ3 cos(θ1+θ3) Equation 8
L
1
=R cos θ3 sin(θ1+θ3) Equation 9
h
2
=R cos θ3 cos(θ2+θ3)
L
2
=R cos θ3 sin(θ2+θ3) Equations 10
n
3y
=h
2 sin ψ−L2 cos φ2 cos ψ Equation 11
n
3z
=h
2 cos ψ+L2 cos φ2 sin ψ Equation 12
Referring to Equations 8 and 12, n3z is canceled, and then hs and L2 in the resulting equation are substituted by Equations 10. Then, φ2 is obtained in the following manner.
As shown in
As shown in
n
3x
=L
1 sin φ1 Equation 15
Thus, the coordinates of the point N3 are obtained. As shown in
{right arrow over (OR2)}=(r1 sin φ1,r1 cos φ1,R cos θ1)
{right arrow over (OR3)}=(r2 sin φ2,R cos φ2 sin ψ−r2 cos ψ,R cos θ2 cos ψ+r2 sin ψ) Equations 16
Now that the coordinates of the points N3, R2, and R3 are obtained, φ3 is determined in the following manner.
Thus, the rotation axis direction of each guide conical pulley and the development center angle of the fan loop belt 13 are obtained, resulting in a nonparallel-axes belt transmission mechanism. Such nonparallel-axes belt transmission mechanism ensures a nonparallel-axes that reduces weight and backlashes as compared with bevel gears, and that ensures high rigidity and high durability as compared with wire transmission mechanisms.
In the fourth embodiment, a timing belt is used as an exemplary fan loop belt.
In the third embodiment, the truncated cone bottom radius r3 of each guide conical pulley is first determined, followed by obtaining the development center angle α of the fan loop belt 13 corresponding to the truncated cone bottom radius r3. In many cases, however, the radius r3 may be at any value insofar as the radius r3 is large enough to ensure the durability of the fan loop belt and small enough to eliminate mechanistical interference with other components. Meanwhile, when a timing belt is used as the fan loop belt, it is necessary to determine the development center angle α such that the number of teeth is an integer. Therefore, it is preferred to first determine the angle α and then to obtain the radius r3 corresponding to the angle α. It is difficult, however, to obtain associated equations analytically. In this case, a calculator may be used to repeat the calculation using r3 to obtain the angle α until the calculation result converges to a sufficient accuracy.
The rotation axis of the main conical pulley 23 is orthogonal to the rotation axes of the input conical pulleys 21 and 22. The fan loop belt 28 is wound around the input conical pulleys 21 and 22, the main conical pulley 23, and the guide conical pulleys 24, 25, 26, and 27 in the manner shown in
The input conical pulleys 21 and 22 may be symmetrical, and therefore, the cone bottom radii of the input conical pulleys 21 and 22 may be denoted collectively, r1. The truncated cone bottom radius of the main conical pulley 23 will be denoted r2, and the truncated cone bottom radius of each of the guide conical pulleys 24, 25, 26, and 27 will be denoted r3. These may be used to calculate angles φ1, φ2, and φ3, similarly to the second embodiment. In this embodiment, however, the rotation axes of the input conical pulley 21 and the main conical pulley 23 intersect at right angles, and the rotation axes of the input conical pulley 22 and the main conical pulley 23 intersect at right angles. Accordingly, assuming that ψ=π/2, the equations to obtain φ1, φ2, φy, the vector O→R2, and the vector O→R3 are simplified as follows.
n
ay
=R cos θ3 cos(θ2+θ3)
{right arrow over (OR2)}=(r1 sin φ1,r1 cos φ1,r2)
{right arrow over (OR3)}=(r2 sin φ2,r1,r2 cos φ2)
The development center angle α of the fan loop belt 28 is determined using the following equation with φ1, φ2, and φ3.
The main conical pulley 23 is in contact with the fan loop belt 28 at two portions, and it is necessary to keep the engagement at one portion consistent with the engagement at the other portion. For example, when the input conical pulleys 21 and the main conical pulley 23 have the same shapes each with an odd number of tooth grooves, then it is necessary that the teeth of the fan loop belt 28 be an odd number. When the input conical pulleys 21 and the main conical pulley 23 have the same shapes each with an even number of tooth grooves, then it is necessary that the teeth of the fan loop belt 28 be an even number.
This intersecting-axes differential belt transmission mechanism serves as an intersecting-axes differential transmission mechanism that reduces weight and backlashes as compared with bevel gears, and that ensures high rigidity and high durability as compared with wire transmission mechanisms. Such transmission mechanism is used with power individually input to each of the input conical pulley 21 and the input conical pulley 22, and with the main conical pulley 23 secured to the output shaft.
In this embodiment, a harmonic gear 67 including two circular splines is considered as a reducer. It is also possible to use harmonic gears of other types or to use other reducers. On the hollow securing support shaft 63, an outer rotor motor stator 66 is secured. An outer rotor motor rotator 64 is supported rotatably about the pitch axis via a bearing. A wave generator, which serves as an input of the harmonic gear 67, is secured to the outer rotor motor rotator 64. The other circular spline of the harmonic gear 67 serves as its output, and the input conical pulley 21 is secured to the other circular spline. The input conical pulley 21 is rotatably supported about the pitch axis via a main pulley support disk 65 and a cross roller bearing 68. In this embodiment, the input conical pulley 21 is supported by the outer circumference of the outer rotor motor rotator 64, in order to reduce the dimensions of the mechanism as a whole. It is, of course, possible to support the input conical pulley 21 at a stationary member such as the hollow securing support shaft 63.
Reference numeral symbol 61 denotes a guide pulley support shaft that supports the guide conical pulley 24 rotatably about the center axis of the guide pulley support shaft 61 via a bearing 69. The guide pulley support shaft 61 is secured to a sub-support frame 56. A total of four sub-support frames 56 are disposed at four, anteroposteriorly and laterally symmetrical positions. The sub-support frames 56 are secured integrally with side support frames 53 and 54 and a top support frame 55. The sub-support frames 56, the side support frames 53 and 54, and the top support frame 55 are rotatably supported about the pitch axis via bearings disposed on the side support frames 53 and 54. Reference numeral 60 denotes an output shaft that is supported on the top support frame 55 via a bearing 70 rotatably about the roll axis. To the output shaft 60, the main conical pulley 23 is secured, so as to output power on the roll axis transmitted by the fan loop belt 28.
Description will be made with regard to how the mechanism according to this embodiment operates. When the input conical pulley 21 and the input conical pulley 22 are rotated in the same direction, the sum of the two kinds of torque involved is transmitted as the power to rotate the output shaft 60 about the pitch axis. For example, when the input conical pulley 21 and the input conical pulley 22 are rotated counterclockwise as viewed from the right side of
Japanese Unexamined Patent Application Publication No. 3-505067 necessitates the pulleys to be stepped in four levels in order to obtain a differential mechanism. Contrarily, in this embodiment, only a single step is necessary on the pulleys, resulting in reductions in size and weight. Additionally, using a belt ensures high durability as compared with the use of a wire. Additionally, the JP3-505067 publication ensures only one rotation, at most, of transmission. Contrarily, this embodiment ensures continuous transmission of a plurality of rotations. Applying this mechanism to interference-driven joint mechanisms of robots realizes robots reduced in size and weight.
Similarly to the second and third embodiments, the input conical pulleys 33 and 34, the main conical pulleys 35 and 36, and the guide conical pulleys 37, 38, 40, 41, 42, and 44 are each rotatable about the center line of the corresponding imaginary conical surface. The input conical pulleys 33 and 34, the main conical pulleys 35 and 36, and the guide conical pulleys 37, 38, 40, 41, 42, and 44 abut on each other such that the apexes of the respective imaginary conical surfaces match. That is, the rotation axes of the input conical pulleys 33 and 34, the main conical pulleys 35 and 36, and the guide conical pulleys 37, 38, 40, 41, 42, and 44 intersect at the apexes of the respective imaginary conical surfaces. In this embodiment, the input conical pulleys 33 and 34 have the same truncated cone bottom radii, and are opposed to one another with the respective rotation axes aligned on a common line. Likewise, the main conical pulleys 35 and 36 have the same truncated cone bottom radii, and are opposed to one another with the respective rotation axes aligned on a common line. The rotation axes of the main conical pulleys 35 and 36 are orthogonal to the rotation axes of the input conical pulleys 33 and 34. The fan loop belt 31 is wound around the input conical pulleys 33 and 34, the main conical pulleys 35 and 36, and the guide conical pulleys 37, 38, 41, and 42 in the manner shown in
The fan loop belt 31 is held taut by four guide conical pulleys to effect a tension in the fan loop belt 31. The fan loop belt 32 is held taut by four guide conical pulleys at a position anteroposteriorly symmetrical with respect to the fan loop belt 31. This arrangement of the conical pulleys turns the fan belts into loops of the same radii as the radii of the respective corresponding conical pulleys. This, in turn, ensures continuous transmission of a plurality of rotations. The fan loop belts 31 and 32 each may be, for example, a timing belt similarly to the second and third embodiments.
The input conical pulleys 33 and 34 may be symmetrical, and the main conical pulleys 35 and 36 may be symmetrical. Therefore, the truncated cone bottom radii of the input conical pulleys 33 and 34 may be denoted collectively, r1, and the truncated cone bottom radii of the main conical pulleys 35 and 36 may be denoted collectively, r2. The truncated cone bottom radius of each of the eight guide conical pulleys will be denoted r3. These may be used to calculate angles φ1, φ2, and φ3, similarly to the second and third embodiments. The development center angle α of each of the fan loop belts 31 and 32 is determined from φ1, φ2, and φ3 using the following equation.
This intersecting-axes differential belt transmission mechanism serves as an intersecting-axes differential transmission mechanism that reduces weight and backlashes as compared with bevel gears, and that ensures high rigidity and high durability as compared with wire transmission mechanisms. Such transmission mechanism is used with power individually input to each of the input conical pulley 33 and the input conical pulley 34, and with the main conical pulley 35 (or the main conical pulley 36) secured to an output shaft. This structure ensures that the fan loop belt on one side can be detached by the simple operation of removing the four guide conical pulleys on the one side, thus facilitating maintenance.
It is necessary that the length of each fan belt be an integral multiple of p. At a teeth number T of 50, p is 5.09. The length of each fan belt is equivalent to 463.3 degrees at a teeth number T of 91; equivalent to 468.4 degrees at a teeth number T of 92; and equivalent to 473.5 degrees at a teeth number T of 93. The length of each fan belt is appropriate at no other teeth numbers T. Hence, the length of each fan loop belt (equivalent to the development center angle α) is determined on any one of the above values, and then the ratio between r1 and r3 corresponding to the determined length is obtained from
In the sixth embodiment, the rotation axes of the main conical pulleys 35 and 36 are aligned on a common line. Instead of aligning the rotation axes on a common line, it is also possible to provide three or more conical pulleys with their respective rotation axes orthogonal to the rotation axes of the input conical pulleys 33 and 34. This reduces load per fan loop belt, with the result, however, that the weight of the mechanism as a whole increases. In view of this, it is preferred in many applications that the number of the conical pulleys be not significantly large. Providing three or more conical pulleys makes each fan loop belt a simple circle depending on the dimensional conditions of the conical pulleys. This facilitates the belt production.
While in other embodiments description is made with regard to a belt, it is also possible to use a chain, in which case a similar transmission mechanism is realized.
Sliding support members as compared with guide conical pulleys have less desirable aspects such as being less efficient in transmission due to friction of the sliding contact portions, more likely causing wear of the fan loop belt 28, and generating heat. Still, the sliding support members do not involve rotation themselves, and therefore, all that is necessary is a contact surface on a single side. This ensures use of metal plates or plastics as the sliding support members, providing advantages including reductions in size, weight, and cost.
Description will now be made with regard to an exemplary robot arm that uses the intersecting-axes differential belt transmission mechanism according to any of the fifth to ninth embodiments.
Reference numeral 109 denotes an output unit, which is secured to the output shaft 60 shown in
The covered support structure 110 rotates about the horizontal axis with the support disk 101 as the center of rotation, while the output unit 109 rotates about the vertical axis. With this structure, a differential joint unit is able to horizontally and vertically rotate a conveyed object attached to the distal end of the output unit 109. The two, horizontal and vertical output axes are configured to form an interference-driven joint mechanism, and this ensures that each axis provides a maximum output of twice the output of a single motor.
As shown in
ψ=θ1+θ2+Δψ Equation 22
Similarly to the above-described embodiments of transmitting power through the engagement between the fan belt and the conical pulley, it is necessary that the development center angle of the fan belt be an integral multiple of the pitch of the engagement between the fan belt and the conical pulley. In the sixth embodiment, the truncated cone bottom radius of the guide conical pulley is determined such that the development center angle of the fan loop belt is an integral multiple of the pitch p of the teeth of the main conical pulley. In the eleventh embodiment, the imaginary conical surface of the main conical pulley is separated from the imaginary conical surface of the input conical pulley by the angle Δψ. In this case, it is possible to determine in advance the truncated cone bottom radius of the guide conical pulley in a convenient manner. Then, the angle Δψ may be determined such that the development center angle of the fan loop belt is an integral multiple of the pitch p of the engagement.
With the use of a belt for power transmission between intersecting axes, the differential mechanism according to the embodiments minimizes backlashes, is highly durable, and is small in size and weight. The differential mechanism finds applications in joint mechanisms of robots such as shoulders, elbows, wrists, hip joints, knees, ankles, necks, waists, and fingers. The differential mechanism also finds applications in power transmission mechanisms each of which use two actuators to implement vehicle steering and rotation of tires, and also in pan/tilt/roll mechanisms of cameras.
Obviously, numerous modifications and variations of the present invention are possible in light of the above teachings. It is therefore to be understood that within the scope of the appended claims, the invention may be practiced otherwise than as specifically described herein.
Number | Date | Country | Kind |
---|---|---|---|
2009-240757 | Oct 2009 | JP | national |
The present application is a continuation application of International Application No. PCT/JP2010/068138, filed Oct. 15, 2010, which claims priority to Japanese Patent Application No. 2009-240757, filed Oct. 19, 2009. The contents of these applications are incorporated herein by reference in their entirety.
Number | Date | Country | |
---|---|---|---|
Parent | PCT/JP2010/068138 | Oct 2010 | US |
Child | 13450425 | US |