ROTATIONAL RESISTANCE APPARATUS AND OPERATION APPARATUS
A rotational resistance apparatus includes a shaft member that includes a first shaft and a second shaft having a diameter larger than a diameter of the first shaft and that has magnetism, a bobbin that is arranged on an outer periphery of the first shaft and that does not have magnetism, a coil that is wound around the bobbin, a case member having magnetism that covers the bobbin, the coil, and the second shaft, a slide bearing that rotatably receives the first shaft through a first gap and that does not have magnetism, and a magnetic viscous fluid that is arranged between the second shaft and the case member. The first gap is smaller than a second gap between the case member and the first shaft.
The present invention relates to a rotational resistance apparatus and an operation apparatus.
Description of the Related ArtA rotational resistance apparatus that generates resistance to a rotation operation using a magnetic viscous fluid can present, for example, resistance to rotation of an operation member capable of a rotation operation to an operator as an operational feeling (touch sensation). Japanese Patent Laid-Japanese Open No. (“JP”) 2017-89732 and Japanese Patent Laid-Open No. (“JP”) 2017-110756 disclose a rotational resistance apparatus adjusting a magnetic field that is applied to a rotatable rotor and a magnetic viscous fluid arranged around a shaft member to adjust resistance (resistance torque) for shearing the magnetic viscous fluid.
However, the rotational resistance apparatus disclosed in JP 2017-89732 and JP 2017-110756 maintains a gap where the magnetic viscous fluid is arranged by supporting the rotor and the shaft member using a ball bearing, and thus increases in a radial direction. Additionally, since components for use the rotor as part of a magnetic circuit, the coil, and the magnetic viscous fluid are accumulated in the radial direction, the rotational resistance apparatus of JP 2017-89732 is not suitable for reducing a diameter. Further, since the magnetic viscous fluid is arranged on an inner diameter side of the apparatus, the rotational resistance apparatus of JP 2017-110756 cannot generate the resistance torque efficiently.
SUMMARY OF THE INVENTIONThe present invention provides a rotational resistance apparatus advantageous in, for example, generation efficiency of rotation resistance and small size.
A rotational resistance apparatus according to one aspect of the present invention includes a shaft member that includes a first shaft and a second shaft having a diameter larger than a diameter of the first shaft and that has magnetism, a bobbin that is arranged on an outer periphery of the first shaft and that does not have magnetism, a coil that is wound around the bobbin, a case member having magnetism that covers the bobbin, the coil, and the second shaft, a slide bearing that rotatably receives the first shaft through a first gap and that does not have magnetism, and a magnetic viscous fluid that is arranged between the second shaft and the case member. The first gap is smaller than a second gap between the case member and the first shaft.
An operation apparatus as another aspect of the present invention includes an operation member that is rotatable, and a rotational resistance apparatus that applies resistance force to the operation member. The rotational resistance apparatus includes a shaft member that includes a first shaft and a second shaft having a diameter larger than a diameter of the first shaft and that has magnetism, a bobbin that is arranged on an outer periphery of the first shaft and that does not have magnetism, a coil that is wound around the bobbin, a case member having magnetism that covers the bobbin, the coil, and the second shaft, a slide bearing that rotatably receives the first shaft through a first gap and that does not have magnetism, and a magnetic viscous fluid that is arranged between the second shaft and the case member. The first gap is smaller than a second gap between the case member and the first shaft.
Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
Referring now to the accompanying drawings, a detailed description will be given of examples according to the present invention.
Example 1The cylindrical member 102 is formed as a magnetic material, and has cutout parts 102a, 102b and through hole parts 102c, 102d. The first and second circular plate 103, 104 are formed as a magnetic material and have through hole parts 103a, 104a, respectively.
The shaft member 101 is formed as a magnetic material, and has first shafts 101a, 101b that are provided at both ends of the shaft member 101 in a shaft direction and a second shaft 101c that is provided between the first shafts 101a, 101b and that has a diameter larger than a diameter of the first shafts 101a, 101b. In the following description, the shaft direction of the shaft member 101 is used as a shaft direction of the rotational resistance apparatus 100, and a direction perpendicular to the shaft direction is referred to as a radial direction.
The first shaft 101a has a transmission shaft part 101d, in which a diameter is reduced by forming a step 101f, on a tip side (a side opposite to the second shaft 101c) in the shaft direction. On the other hand, the first shaft 101b has a detection shaft part 101e, in which a diameter is reduced by forming a step 101g, on a tip side in the shaft direction.
On an outer periphery of the first shafts 101a, 101b provided inside the cylindrical member 102, coils 105, 106 that are respectively wound around bobbins 107, 108 are arranged. The cylindrical member 102 is arranged to cover an outer periphery of the coils 105, 106 and an outer periphery of the second shaft 101c. The first and second circular plates 103, 104 are arranged to cover ends of outside (a side far from the second shaft 101c) of the bobbins 107, 108 in the shaft direction.
The transmission shaft part 101d and the detection shaft part 101e of the shaft member 101 project to an outside of the case member through the through hole parts 103a, 104a of the first and second circular plates 103, 104, respectively. As illustrated in
A gear 115 is fixed to the tip of the first shaft 101a to rotate integrally with the shaft member 101, and a detected member 116 for rotation (angle) detection is fixed to the tip of the first shaft 101b to rotate integrally with the shaft member 101. A detector 117 is arranged to face a side surface of the detected member 116.
The gear 115 can transmit rotation resistance torque generated by the rotational resistance apparatus 100 on the basis of a principle described later to a rotation operation member (not illustrated). The detector 117 optically or magnetically detects a pattern (not illustrated) provided on the detected member 116 and outputs a signal. The rotation angle of the rotation operation member can be detected using the signal.
Both bobbins 107, 108 are formed as non-magnetic materials. Each of the bobbins 107, 108 has, on both sides in the shaft direction, annular end surface parts 107a, 108a that abut on an inner circumferential surface of the cylindrical member 102. Additionally, the bobbins 107, 108 are respectively provided with wiring parts 107b, 108b for connecting the windings of the coils 105, 106 to an external magnetic field control apparatus (not illustrated).
Further, slide bearings 107c, 108c that rotatably receives the first shaft 101a (transmission shaft part 101d) and the first shaft 101b (detection shaft part 101e) are formed on an inner periphery of the end surface parts 107a, 108a provided outside of the bobbins 107, 108 in the shaft direction, respectively. As illustrated in
A magnetic viscous fluid (hereinafter referred to as MR fluid) F is arranged in a gap area that is surrounded by an outer circumferential surface and both side surfaces of the second shaft 101c, the inner circumferential surface of the cylindrical member 102, and the end surface parts 107a, 107b inside (a side near the second shaft 101c) of the bobbins 107a, 108a. As illustrated in
In annular concave parts provided on outer circumferential surfaces of the end surface parts 107a, 108a inside of the bobbins 107, 108 in the shaft direction, first seal rings 109, 110 to seal a gap between the outer circumferential surfaces of the end surface parts 107a, 108a and the inner circumferential surface of the cylindrical member 102 are fitted and retained. Further, in annular concave parts provided on inner circumferential surfaces of the end surface parts 107a, 108a inside of the bobbins 107, 108 in the shaft direction, second seal rings 111, 112 to seal a gap between the inner circumferential surfaces of the end surface parts 107a, 108a and the inner circumferential surfaces of the first shafts 101a, 101b are fitted and retained.
The rotational resistance apparatus 100 is assembled as follows. As illustrated in
In the rotational resistance apparatus 100 configured as above, a size in the radial direction of the gap Gb1 between the inner circumferential surface of the slide bearing 107c and the outer circumferential surface of the transmission shaft part 101d is smaller (that is, narrower) than that of the gap Ga1 between the inner circumferential surface of the through hole part 103a and the outer circumferential surface of the transmission shaft part 101d. Additionally, the gap Gb2 between the inner circumferential surface of the slide bearing 108c and the outer circumferential surface of the detection shaft part 101e is narrower than the gap Ga2 between the inner circumferential surface of the through hole part 104a and the outer circumferential surface of the detection shaft part 101e. Further, the gaps Gb1, Gb2 is narrower than the gap (third gap) GM between the outer circumferential surface of the second shaft 101c and the outer circumferential surface of the cylindrical member 102 in a space where the MR fluid F is arranged.
Referring now to
As illustrated in
The magnetic fluxes that flow from each of the first shafts 101a, 101b of the shaft member 101 to the second shaft 101c repels in the second shaft 101c and flow toward the outer circumferential surface of the second shaft 101c. The magnetic fluxes flowing through from the outer circumferential surface of the second shaft 101c pass through the MR fluid F and flow in the cylindrical member 102. The magnetic fluxes generated by energizing the coil 105 of the magnetic fluxes which flow in the cylindrical member 102 flow in part facing the coil 105 of the cylindrical member 102 and flow toward the first circular plate 103. Then, the magnetic fluxes flowing out the first circular plate 103 returns to the first shaft 101a through the transmission shaft part 101d, which faces the through hole part 103a in a non-contact manner. On the other hand, the magnetic fluxes generated by energizing the coil 106 of the magnetic fluxes which flow in the cylindrical member 102 flow in part facing the coil 106 of the cylindrical member 102 and flow toward the second circular plate 104. Then, the magnetic fluxes flowing through the second circular plate 104 returns to the first shaft 101b through the detection shaft part 101e, which faces the through hole part 104a in a non-contact manner.
In this example, since almost all of the magnetic fluxes generated by energizing the coils 105, 106 flow in the MR fluid F through the first and second magnetic circuits M1, M2 to form numberless clusters C in the MR fluid F, the resistance force (rotation resistance torque) against the rotation of the shaft member 101 can be efficiently generated. Then, changing the amount of current flowing in the coils 105, 106 can control the strength of the magnetic fluxes flowing in the MR fluid F to adjust the magnitude of the rotation resistance torque.
Further, as described above, since the gaps Gb1, Gb2 are narrower than the gaps Ga1, Ga2, Gm, the shaft member 101 is rotatably supported in a non-contact state with the case member (the cylindrical member 102, the first and second circular plates 103, 104). As a result, the gaps Ga1, Ga2, Gm are always kept constant, and stable rotation resistance torque can be generated by contacting the shaft member 101 with the case member without making the magnetic resistance of the first and second magnetic circuits M1, M2 unstable and changing the magnetic fluxes flowing in the MR fluid F.
In this example, since the slide bearings 107c, 108c are formed integrally with the bobbins 107, 108, the number of parts of the rotational resistance apparatus 100 is smaller than that in the case where these are separate parts, so that the configuration and the assembly can be simplified. Further, since the number of parts is reduced, the tolerances are less accumulated, and the gap (Ga1, Ga2, Gm) in each magnetic circuit can be reduced. As a result, the magnetic resistance of each magnetic circuit can be reduced, and larger rotation resistance torque can be obtained.
Further, since the slide bearings 107c, 108c function as a thrust bearing that sandwiches the steps 101f, 101g of the shaft member 101, it is possible to further simplify the configuration and the assembly.
Example 2The rotational resistance apparatus 200 according to this example includes a coil spring 215 that is arranged between a step 201f on an outer periphery of a first shaft 201a of a shaft member 201 and an internal surface of an end surface part 207a of a bobbin 207 and that biases the shaft member 201 on one side (a side of a first shaft 201b) in a shaft direction as a biasing member. A second circular plate 204 does not have a through hole part corresponding to the through hole part 104a of the second circular plate 104 according to Example 1, and a hemispherical convex part 201e at a tip of the first shaft 201b is pressed against the second circular plate 204 by the biasing force E1 of the coil spring 215. The second circular plate 204 is fixed to a cylindrical member 202 to withstand the biasing force E1. The first shaft 201b is not provided with a detection shaft part corresponding to the detection shaft part 101e according to Example 1.
Further, reaction force E2 against the biasing force E1 acts on the bobbin 207 on which the coil spring 215 abuts. A first circular plate 203 that abuts on the bobbin 207 is fixed to the cylindrical member 202 to withstand the reaction force E2.
As illustrated in
The magnetic fluxes that flow from each of the first shafts 201a, 201b of the shaft member 201 to the second shaft 201c repels in the second shaft 201c and flow toward an outer circumferential surface of the second shaft 201c. The magnetic fluxes flowing out from the outer circumferential surface of the second shaft 201c pass through the MR fluid F and flow in the cylindrical member 202. The magnetic fluxes generated by energizing the coil 205 of the magnetic fluxes which flow in the cylindrical member 202 flow in part facing the coil 205 of the cylindrical member 202 and flow toward the first circular plate 203. Then, the magnetic fluxes flowing through the first circular plate 203 returns to the first shaft 201a through the transmission shaft part 201d, which faces the through hole part 203 a in a non-contact manner. On the other hand, the magnetic fluxes generated by energizing the coil 206 of the magnetic fluxes which flow in the cylindrical member 202 flow in part facing the coil 206 of the cylindrical member 202 and flow toward the second circular plate 204. Then, the magnetic fluxes flowing through the second circular plate 204 returns to the first shaft 201b.
As described above, in this example, since almost all of the magnetic fluxes generated by energizing the coils 205, 206 flow in the MR fluid F through the first and second magnetic circuits M3, M4, rotation resistance torque against the shaft member 201 can be efficiently generated. Then, changing the amount of current flowing in the coils 205, 206 can control the strength of the magnetic fluxes flowing in the MR fluid F to adjust the magnitude of the rotation resistance torque.
In this example, since the gaps Gb3, Gb4 are narrower than the gaps Ga3, Gm, the first shaft 201a and the second shaft 201c of the shaft member 201 are respectively rotatably supported in a non-contact state with the circular plate 203 and the cylindrical member 202, and the gaps Ga3, Gm are kept constant. On the other hand, the first shaft 201b contacts the second circular plate 203 at the convex part 201e, but the gap Ga4 is kept constant by the convex part 201e and the biasing force of the coil spring 215. Keeping the gaps Ga3, Ga4, Gm constant can generate stable rotation resistance torque without making the magnetic resistance of the first and second magnetic circuits M3, M4 unstable and changing the magnetic fluxes flowing in the MR fluid F.
In this example, since the slide bearings 207c, 208c are formed integrally with the bobbins 207, 208, the configuration and the assembly can be simplified. Further, the gap (Ga3, Ga4, Gm) in each magnetic circuit can be reduced, and larger rotation resistance torque can be obtained by reducing the magnetic resistance of each magnetic circuit.
In addition, the shaft member 201 is biased by the coil spring 215 in this example but may be biased by another biasing member.
Example 3The slide bearings 107c, 108c are integrally provided to the bobbins 107, 108 in Example 1 but, in this example, slide bearings 315, 316, which are made of a non-magnetic material and are formed as a separate part from bobbins 307, 308, are fixed to inner circumferential surfaces of end surface parts 307a, 308a of the bobbins 307, 308. As the slide bearings 315, 316, a resin bearing made of a low friction material, and a metal bearing impregnated with lubricating oil can be used.
In this example, as illustrated in
As illustrated in
Slide bearings receiving bearing members, which are corresponding to the slide bearings 315, 316 and are fixed to a shaft member, may be integrally provided on bobbins. In this case, the bearing members fixed to the shaft member 301 may be regarded as one body with the shaft member, and a gap between each bearing member and each slide bearing of the bobbin may be a first gap.
The rotation resistance apparatuses 100, 200, 300 according to Examples 1 to 3 described above are small in size and can efficiently generate rotation resistance torque.
Example 4An imaging optical system 401 is arranged in the interchangeable lens 400. An outer periphery of the interchangeable lens 400 is provided with an operation ring 402 as an operation member that allows a user to perform a rotational operation. When the operation ring 402 rotates, a variable power lens and a focus lens in the imaging optical system 401 move to an optical axis direction to perform zooming and focusing.
The rotation of the operation ring 402 is transmitted through the gear 115 to the shaft member 101 of the rotational resistance apparatus 100 according to Example 1 arranged in the interchangeable lens 400. As a result, the rotation resistance torque generated in the rotational resistance apparatus 100 by the rotational operation of the operation ring 402 is applied as an operational feeling. The rotational resistance apparatuses 200, 300 described in Examples 2, 3 may be used instead of the rotational resistance apparatus 100. Further, the rotation resistance apparatus described in Examples 1 to 3 may be used in operation apparatuses other than the interchangeable lens.
According to the above-mentioned example, for example, it is possible to provide to a rotational resistance apparatus advantageous in generation efficiency of rotation resistance and small size.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2019-176362, filed on Sep. 27, 2019 which is hereby incorporated by reference herein in its entirety.
Claims
1. A rotational resistance apparatus comprising:
- a shaft member that includes a first shaft and a second shaft having a diameter larger than a diameter of the first shaft and that has magnetism;
- a bobbin that is arranged on an outer periphery of the first shaft and that does not have magnetism;
- a coil that is wound around the bobbin;
- a case member having magnetism that covers the bobbin, the coil, and the second shaft;
- a slide bearing that rotatably receives the first shaft through a first gap and that does not have magnetism; and
- a magnetic viscous fluid that is arranged between the second shaft and the case member,
- wherein the first gap is smaller than a second gap between the case member and the first shaft.
2. The rotational resistance apparatus according to claim 1, wherein the first gap is smaller than a third gap between the second shaft and the case member in a space where the magnetic viscous fluid is arranged.
3. The rotational resistance apparatus according to claim 1,
- wherein the case member has a through hole through which the first shaft passes, and
- wherein the second gap is provided between an inner circumferential surface of the through hole and an outer circumferential surface of the first shaft.
4. The rotational resistance apparatus according to claim 1,
- wherein a convex part is provided on one of an end surface of the first shaft in a shaft direction of the first shaft and the case member so as to abut on the other of the end surface and the case member, and
- wherein the second gap is provided between the end surface and the case member and around the convex part.
5. The rotational resistance apparatus according to claim 1, wherein the slide bearing is formed integrally with the bobbin.
6. The rotational resistance apparatus according to claim 1, wherein the first shafts and the coils are provided on both sides of the second shaft in a shaft direction of the shaft member.
7. The rotational resistance apparatus according to claim 6, wherein, by energizing the coils provided on the both sides so that magnetic fluxes in opposite directions to each other are generated in the first shafts provided on the both sides, a first magnetic circuit is formed through one first shaft, the second shaft, and the case member, and a second magnetic circuit is formed through the other first shaft, the second shaft, and the case member.
8. The rotational resistance apparatus according to claim 1, further comprising:
- a first sealing member that seals a gap between an outer circumferential surface of the bobbin and an inner circumferential surface of the case member; and
- a second sealing member that seals a gap between an inner circumferential surface of the bobbin and an outer circumferential surface of the first shaft.
9. An operation apparatus comprising:
- an operation member that is rotatable; and
- a rotational resistance apparatus that applies resistance force to the operation member,
- wherein the rotational resistance apparatus includes: a shaft member that includes a first shaft and a second shaft having a diameter larger than a diameter of the first shaft and that has magnetism; a bobbin that is arranged on an outer periphery of the first shaft and that does not have magnetism; a coil that is wound around the bobbin; a case member having magnetism that covers the bobbin, the coil, and the second shaft; a slide bearing that rotatably receives the first shaft through a first gap and that does not have magnetism; and a magnetic viscous fluid that is arranged between the second shaft and the case member,
- wherein the first gap is smaller than a second gap between the case member and the first shaft.
Type: Application
Filed: Sep 15, 2020
Publication Date: Apr 1, 2021
Inventor: Junya Hirano (Utsunomiya-shi)
Application Number: 17/021,151