JPH0460221A - Thrust bearing setting structure in magnetic clutch - Google Patents
Thrust bearing setting structure in magnetic clutchInfo
- Publication number
- JPH0460221A JPH0460221A JP2172485A JP17248590A JPH0460221A JP H0460221 A JPH0460221 A JP H0460221A JP 2172485 A JP2172485 A JP 2172485A JP 17248590 A JP17248590 A JP 17248590A JP H0460221 A JPH0460221 A JP H0460221A
- Authority
- JP
- Japan
- Prior art keywords
- thrust bearing
- small diameter
- inner tube
- cylindrical part
- cylindrical
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000004907 flux Effects 0.000 claims abstract description 15
- 230000002093 peripheral effect Effects 0.000 abstract description 8
- 239000000696 magnetic material Substances 0.000 description 6
- 239000004809 Teflon Substances 0.000 description 5
- 229920006362 Teflon® Polymers 0.000 description 5
- 230000000149 penetrating effect Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 2
- 238000004904 shortening Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は、ロータのインナーチューブとステータの中
心軸部との間にスラスト軸受けとして円形シートを配置
した電磁クラッチにおけるスラスト軸受は取り付け構造
に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a thrust bearing mounting structure in an electromagnetic clutch in which a circular seat is disposed as a thrust bearing between an inner tube of a rotor and a central shaft portion of a stator.
[従来の技術]
第3図に従来の電磁クラッチを示す。固定部1に固定さ
れる磁性材のステータ2は、筒状部3と中心軸部4とを
持ち、前記筒状部3の内面側に電磁コイル5を設けてい
る。ロータ6は、外周に入力ギヤ7を固定した磁性体の
アウターチューブ8と、クラッチ軸心を貫通する非磁性
材の固定の中心貫通軸9に回転自在に嵌合する磁性材の
インナーチューブ10と、このインナーチューブ10と
前記アウターチューブ8とを結合させる非磁性材の結合
部11とからなっている。ステータ2の筒状部3の外周
面とロータ6のアウターチューブ8の内周面との間には
微小な一定のクリアランスが形成されている。また、前
記中心貫通軸9にはロータ6に接触・離間可能に設けら
れてロータ6の回転を伝達されるアマチュア12が回転
自在に取り付けられ、このアマチュア12と回転方向に
係合する出力ギヤ13が中心貫通軸9に回転可能に取り
付けられている。また、インナーチューブ10の下端面
とステータ中心軸部4の上端面との間に第4図にも拡大
して示すように、スラスト軸受けとして例えばテフロン
シートによる円形シート14が配置されている。テフロ
ンシートは強度が強く摩擦抵抗が小さいことからスラス
ト軸受けとして好適であるため用いられる。電磁コイル
5に通電した時、矢印で示すごとき磁気回路が形成され
るが、この磁気回路の磁気抵抗を小さくするために、前
記円形シート14は極力1いものが望ましく、例えば厚
さt=0.1mm程度のものが用いられる。[Prior Art] Fig. 3 shows a conventional electromagnetic clutch. A stator 2 made of a magnetic material and fixed to a fixed part 1 has a cylindrical part 3 and a central shaft part 4, and an electromagnetic coil 5 is provided on the inner surface of the cylindrical part 3. The rotor 6 includes an outer tube 8 made of a magnetic material to which an input gear 7 is fixed on the outer periphery, and an inner tube 10 made of a magnetic material rotatably fitted to a fixed center penetrating shaft 9 made of a non-magnetic material passing through the clutch axis. , and a connecting portion 11 made of a non-magnetic material that connects the inner tube 10 and the outer tube 8. A small constant clearance is formed between the outer peripheral surface of the cylindrical portion 3 of the stator 2 and the inner peripheral surface of the outer tube 8 of the rotor 6. Further, an armature 12 is rotatably attached to the central penetrating shaft 9 so as to be able to come into contact with and separate from the rotor 6, and to which the rotation of the rotor 6 is transmitted, and an output gear 13 that engages with this armature 12 in the rotational direction. is rotatably attached to the central penetrating shaft 9. Further, as shown in an enlarged view in FIG. 4, a circular sheet 14 made of, for example, a Teflon sheet is disposed between the lower end surface of the inner tube 10 and the upper end surface of the stator central shaft portion 4 as a thrust bearing. Teflon sheets are used because they are suitable for thrust bearings because they have high strength and low frictional resistance. When the electromagnetic coil 5 is energized, a magnetic circuit as shown by the arrow is formed. In order to reduce the magnetic resistance of this magnetic circuit, it is desirable that the circular sheet 14 be as thin as possible; for example, the thickness t = 0. A material with a diameter of about .1 mm is used.
[発明が解決しようとする課題]
テフロンシートは延性があるため、これにスラスト荷重
が加わると円形シート14が半径方向に伸びてしまい、
その周縁部が第5図に示すように軸受は面から外にはみ
出してしまう。そうすると。[Problems to be Solved by the Invention] Since the Teflon sheet is ductile, when a thrust load is applied to it, the circular sheet 14 stretches in the radial direction.
The peripheral edge of the bearing protrudes out of the surface as shown in FIG. Then.
厚みtが一層薄くなるとともに、はみ出した部分が円滑
な回転を妨げ、スラスト軸受けとして使用不可となる1
例えば、使用開始時に厚み0.1mmのテフロンの円形
シートが300時間使用後に厚み0.08mm 〜0.
05mm程度まで薄くなる。As the thickness t becomes thinner, the protruding portion impedes smooth rotation and becomes unusable as a thrust bearing1.
For example, a Teflon circular sheet that is 0.1 mm thick at the beginning of use becomes 0.08 mm to 0.0 mm thick after 300 hours of use.
It becomes thinner to about 0.05mm.
本発明は上記従来の欠点を解消するためになされたもの
で、円形シート状のスラスト軸受けの寿命を長くするこ
とのできるスラスト軸受は取り付け構造を提供すること
を目的とする。The present invention has been made to solve the above-mentioned conventional drawbacks, and an object of the present invention is to provide a thrust bearing mounting structure that can extend the life of a circular sheet-shaped thrust bearing.
[課題を解決するための手段]
上記課題を解決する請求項1の発明は、ロータのインナ
ーチューブの端面とこれに対向するステータの中心軸部
の端面との間にスラスト軸受けとして円形シートを配置
した電磁クラッチにおけるスラスト軸受は取り付け構造
であって、前記インナーチューブの端部またはステータ
中心軸部の端部の一方に薄肉の円筒部、他方に前記円筒
部に嵌合する小径部を形成し、前記円筒部の内面と前記
小径部の外面とのギャップXをスラスト軸受けである前
記円形シートの厚みtより小さく形成したことを特徴と
する
請求IR2の発明は、インナーチューブの端部またはス
テータ中心軸部の端部の一方に厚肉かつ深い円筒部、他
方に前記円筒部に嵌合する小径部を形成するとともに、
前記円筒部と小径部との嵌合面の面積がインナーチュー
ブの断面積とほぼ同等かそれより大きく、かつ、前記小
径部の断面積および円筒部の断面積がいずれも、電磁コ
イルが発生する磁束を通すために十分な面積を持つこと
を特徴とする電磁クラッチにおけるスラスト軸受は取り
付け構造、前記円筒部と小径部との嵌合面の面積がイン
ナーチューブの断面積とほぼ同等かそれより大きく、か
つ、前記小径部の断面積および円筒部の断面積がいずれ
も、電磁コイルが発生する磁束を通すために十分な面積
を持つことを特徴とする電磁クラッチにおけるスラスト
軸受は取り付け構造である。[Means for Solving the Problems] The invention according to claim 1 which solves the above problems includes disposing a circular seat as a thrust bearing between the end face of the inner tube of the rotor and the end face of the central shaft portion of the stator facing thereto. The thrust bearing in the electromagnetic clutch has a mounting structure, and has a thin cylindrical part formed at one end of the inner tube or the end of the stator central shaft part, and a small diameter part that fits into the cylindrical part at the other end, The invention of claim IR2 is characterized in that the gap X between the inner surface of the cylindrical portion and the outer surface of the small diameter portion is formed to be smaller than the thickness t of the circular sheet that is a thrust bearing. A thick and deep cylindrical part is formed at one end of the part, and a small diameter part that fits into the cylindrical part is formed at the other end,
The area of the fitting surface between the cylindrical part and the small diameter part is approximately equal to or larger than the cross-sectional area of the inner tube, and the cross-sectional area of the small diameter part and the cross-sectional area of the cylindrical part are both such that an electromagnetic coil is generated. A thrust bearing in an electromagnetic clutch characterized by having a sufficient area for passing magnetic flux has a mounting structure, and the area of the fitting surface between the cylindrical part and the small diameter part is approximately equal to or larger than the cross-sectional area of the inner tube. , and the thrust bearing in the electromagnetic clutch is a mounting structure, wherein both the cross-sectional area of the small diameter portion and the cross-sectional area of the cylindrical portion have a sufficient area to pass the magnetic flux generated by the electromagnetic coil.
[作用]
請求項1のスラスト軸受は取り付け構造において、円形
シートにスラスト荷重が加わった時、円形シートは半径
方向に延びようとするが、円筒部の内面と小径部の外面
とのギャップXが円形シートの厚みtより小さいので、
円形シートの周縁部がこのギャップ内に入り込むことは
なく、したがって、円形シートの周縁部は円筒部の内面
により確実に拘束され、半径方向に延びてしまうことが
防止される。このように、円形シートは一定の体積内に
封じ込められ、厚みが薄くなることがなく、寿命が短く
なることは防止される。[Function] In the thrust bearing of claim 1, in the mounting structure, when a thrust load is applied to the circular seat, the circular seat tends to extend in the radial direction, but the gap X between the inner surface of the cylindrical portion and the outer surface of the small diameter portion is Since it is smaller than the thickness t of the circular sheet,
The peripheral edge of the circular sheet does not enter into this gap, so that the peripheral edge of the circular sheet is reliably restrained by the inner surface of the cylindrical part and is prevented from extending in the radial direction. In this way, the circular sheet is confined within a constant volume, does not become thinner, and is prevented from shortening its lifespan.
請求項2のスラスト軸受は取り付け構造において、電磁
コイルにより発生した磁束は、小径部を軸心方向に通り
、小径部と円筒部との嵌合面を略半径方向に通り、円筒
部を軸心方向に通る。そして、小径部の断面積、円筒部
の断面積、および小径部と円筒部との嵌合面の面積が、
いずれも電磁コイルが発生する磁束を通すために十分な
面積を持つので、円形シートのある軸受は面を磁気通路
としなくても、必要な磁束を通すことができる。In the thrust bearing of claim 2, in the mounting structure, the magnetic flux generated by the electromagnetic coil passes through the small diameter part in the axial direction, passes through the fitting surface between the small diameter part and the cylindrical part in the approximately radial direction, and passes through the cylindrical part in the axial direction. Pass in the direction. Then, the cross-sectional area of the small diameter part, the cross-sectional area of the cylindrical part, and the area of the fitting surface between the small diameter part and the cylindrical part are:
Since both have a sufficient area to pass the magnetic flux generated by the electromagnetic coil, bearings with circular seats can pass the necessary magnetic flux without using the surface as a magnetic path.
したがって、円形シートは、磁気抵抗を小さくするとい
う要求がなくなり、厚みを厚くして、寿命を長くするこ
とができる。Therefore, the circular sheet does not need to have low magnetic resistance and can be thickened and have a long life.
[実施例コ 第1図に請求項1の発明の一実施例を示す。[Example code] FIG. 1 shows an embodiment of the invention according to claim 1.
以下の実施例において電磁クラッチ自体の構造としては
、スラスト軸受は部分を除き第3図で説明した構造と同
じであり、再度の説明は省略する。In the following embodiments, the structure of the electromagnetic clutch itself is the same as the structure explained in FIG. 3 except for the thrust bearing, and a repeated explanation will be omitted.
第1図において、符号10はロータ6のインナーチュー
ブ、符号4はステータ2の中心軸部、符号っけ中心貫通
軸である。In FIG. 1, the reference numeral 10 is an inner tube of the rotor 6, and the reference numeral 4 is a central shaft portion of the stator 2, which is a central penetrating shaft.
この実施例ては、インナーチューブ10の端部に1肉の
円筒部10aを形成し、ステ〜り中心軸部4の端部に前
記円筒部10に嵌合する小径部4aを形成し、前記円筒
部10aの内面と前記小径部4aの外面とのギャップX
をテフロンシートを用いたスラスト軸受けである円形シ
ート14の厚みtより小さく形成している。この場合、
電磁コイル5が発生させた磁束が円形シート14を通過
するため、円形シート14は、磁気回路の磁気抵抗を小
さくするために薄くする必要がある。図示例では、円形
シート14の厚みtを0.1mm程度、ギャッ7xを0
.02rnrn−0,05mm程度としている。In this embodiment, a one-thick cylindrical portion 10a is formed at the end of the inner tube 10, a small diameter portion 4a that fits into the cylindrical portion 10 is formed at the end of the stay center shaft portion 4, and the Gap X between the inner surface of the cylindrical portion 10a and the outer surface of the small diameter portion 4a
is formed to be smaller than the thickness t of the circular sheet 14 which is a thrust bearing using a Teflon sheet. in this case,
Since the magnetic flux generated by the electromagnetic coil 5 passes through the circular sheet 14, the circular sheet 14 needs to be thin in order to reduce the magnetic resistance of the magnetic circuit. In the illustrated example, the thickness t of the circular sheet 14 is approximately 0.1 mm, and the gap 7x is 0.
.. It is approximately 0.02rnrn-0.05mm.
上記のスラスト軸受は取り付け構造において、円形シー
ト14にスラスト荷重が加わった時、円形シート14は
半径方向に延びようとするが、円筒部10aの内面と小
径部4aの外面とのギャップXが円形シート14の厚み
tより小さいので、円形シート14の周縁部がこのギャ
ップ内に入り込むことはなく、したがって、円形シート
14の周縁部は円筒部]、 Oaの内面により確実に拘
束され、半径方向に延びてしまうことが防止される。In the above-described thrust bearing, in the mounting structure, when a thrust load is applied to the circular seat 14, the circular seat 14 tends to extend in the radial direction, but the gap X between the inner surface of the cylindrical portion 10a and the outer surface of the small diameter portion 4a is circular. Since the thickness t of the sheet 14 is smaller than the thickness t of the sheet 14, the peripheral edge of the circular sheet 14 does not enter into this gap, and therefore the peripheral edge of the circular sheet 14 is reliably constrained by the inner surface of the cylindrical portion Oa and radially This prevents it from elongating.
このように、円形シート14は一定の体積内に封じ込め
られ、厚みが薄くなることがなく、寿命が短くなること
は防止される。In this way, the circular sheet 14 is confined within a constant volume, does not become thinner, and is prevented from shortening its lifespan.
第2図に請求項2の発明の一実施例を示す。FIG. 2 shows an embodiment of the invention according to claim 2.
インナーチューブ10の端部に円筒部]、 Oaを形成
し、ステータ中心軸部4の端部に前記円筒部10に嵌合
する小径部4aを形成している点は第1図の場合と同様
であるが、この発明では、円筒部]、 Oaの肉厚を厚
くし、がっ、深さ11を深くする。さらに、円筒部10
aと小径部4aとの嵌6面の面積S、がインナーチュー
ブ1oの断面積s2とほぼ同等かそれより大きく、かつ
、前記小径部4aの断面積S3および円筒部]、 Oa
の断面積S。Similar to the case of FIG. 1, a cylindrical portion] and Oa are formed at the end of the inner tube 10, and a small diameter portion 4a that fits into the cylindrical portion 10 is formed at the end of the stator central shaft portion 4. However, in the present invention, the thickness of the cylindrical portion Oa is increased, and the depth 11 is increased. Furthermore, the cylindrical part 10
The area S of the fitting surface between the small diameter portion 4a and the small diameter portion 4a is approximately equal to or larger than the cross sectional area s2 of the inner tube 1o, and the cross sectional area S3 of the small diameter portion 4a and the cylindrical portion], Oa
The cross-sectional area S.
かいずれも、電磁コイル5が発生する磁束を通すために
十分余裕のある面積にする。インナーチューブ10の径
をD、ステータ中心軸部4の小径部4aの径をd、クラ
ッチ軸心の中心貫通軸つとして非磁性材を用いたとして
その径をmとすれば、前記各面積S l、 S 2.
S 3. S−は、次式で表される。In either case, the area should be large enough to pass the magnetic flux generated by the electromagnetic coil 5. If the diameter of the inner tube 10 is D, the diameter of the small diameter portion 4a of the stator central shaft portion 4 is d, and the shaft passing through the center of the clutch axis is made of a non-magnetic material and its diameter is m, each of the above-mentioned areas S l, S2.
S 3. S- is represented by the following formula.
S −π dx
S 2−yr (D 2 m ’ )/ 4S s
= π(d 2m 2) y’4S、−π (D2
d2)z′4
なお、この実施例では第1図のものと同様に、円筒部1
0aの内面と小径部4aの外面とのギャップXを0 、
02 m m 〜0 、05 m m程度と、円形シー
ト14の厚みt = 0 、1 m rnより小さく形
成している。S −π dx S 2-yr (D 2 m')/4S s
= π(d 2m 2) y'4S, -π (D2
d2)z'4 Note that in this embodiment, the cylindrical portion 1 is
The gap X between the inner surface of 0a and the outer surface of small diameter portion 4a is 0,
The thickness of the circular sheet 14 is about 0.02 mm to 0.05 mm, which is smaller than the thickness t=0.1 mrn.
また、インナーチューブ10の円筒部1.0 a (7
1先端面とステータ中)C・軸部4とのギヤツブnは、
n = 0 、5 m m程度としている。実施例では
このギャップnの部分は磁束が通る磁気回路の一部とは
見ていない。このギャップnを狭くすれば、磁束を通す
ことができるが、この場合、円形シートの摩耗時に接触
するおそれが生じるため、十分余裕をとって大きなギャ
ップとしている。In addition, the cylindrical portion 1.0 a (7
1) The gear lug n between the tip surface and the shaft part 4 (inside the stator) is:
n = 0, about 5 mm. In the embodiment, this gap n is not considered to be part of the magnetic circuit through which magnetic flux passes. If this gap n is made narrower, the magnetic flux can pass through, but in this case, there is a risk that the circular sheets will come into contact with each other when they are worn out, so the gap is made large enough to allow for a sufficient margin.
上記のスラスト軸受は取り付け構造において、電磁コイ
ル5により発生した磁束は、矢印で示すように小径部4
aを軸心方向に通り、小径部4aど円筒部10aとのギ
ャップX=0.02mm〜0.05mmなる嵌き面Aを
通り、円筒部10aを軸心方向に通る。この場合、小径
部4aと円筒部10aとの嵌合面Aの面積S1がインナ
ーチューブ10の断面積S2と同等以上であり、かつ、
小径部4aの断面MS、および円筒部10aの断面積S
、かいずれも電磁コイル5が発生する磁束を通すために
十分な面積を持つので、円形シート14のある軸受は面
を磁気通路としなくても、必要な磁束を通すことができ
る。したがって、円形シート14は、磁気抵抗を小さく
するという要求がなくなり、例えば厚みtを0.1mm
以上に厚くして、寿命を長くすることができる。In the mounting structure of the above thrust bearing, the magnetic flux generated by the electromagnetic coil 5 is transferred to the small diameter portion 4 as shown by the arrow.
a in the axial direction, passes through the fitting surface A where the small diameter portion 4a and the cylindrical portion 10a have a gap X of 0.02 mm to 0.05 mm, and passes through the cylindrical portion 10a in the axial direction. In this case, the area S1 of the fitting surface A between the small diameter portion 4a and the cylindrical portion 10a is equal to or larger than the cross-sectional area S2 of the inner tube 10, and
Cross section MS of small diameter portion 4a and cross section S of cylindrical portion 10a
, have a sufficient area to pass the magnetic flux generated by the electromagnetic coil 5, so the bearing with the circular seat 14 can pass the necessary magnetic flux without using the surface as a magnetic path. Therefore, the circular sheet 14 is no longer required to have low magnetic resistance, and for example, the thickness t can be reduced to 0.1 mm.
By increasing the thickness, the lifespan can be extended.
また、インナーチューブ10とステータ中心軸部4との
間の磁気吸引力は、円筒部10aの先端面のギャップn
を大きくしているので、小径部4aの端面(すなわち円
形シートのある軸受は面)に働くが、この端面の面積(
−小径部4aの面積)は、単に同径のインナーチューブ
とステータ中心軸部とを対向させた従来構造の場合の面
積(−π(D2−d2))と比較して狭くなるのて、電
磁コイル5で発生させた磁束によりインナーチューブ1
0とステータ中心軸部4との間に働く磁気吸引力が小さ
くなり、したがってスラスト軸受けに働くスラスト荷重
が小さくなり、円形シート14の寿命が長くなる。Furthermore, the magnetic attraction force between the inner tube 10 and the stator central shaft portion 4 is caused by the gap n between the distal end surface of the cylindrical portion 10a.
is made large, so it acts on the end face of the small diameter portion 4a (i.e., the surface of a bearing with a circular seat), but the area of this end face (
-The area of the small diameter portion 4a) is narrower than the area (-π(D2-d2)) in the case of the conventional structure in which the inner tube of the same diameter and the stator center shaft are simply opposed, so the electromagnetic The magnetic flux generated by the coil 5 causes the inner tube 1 to
0 and the stator center shaft portion 4 becomes smaller, the thrust load acting on the thrust bearing becomes smaller, and the life of the circular seat 14 becomes longer.
なお、上記の各実施例とは逆に、インナーチューブ10
側に円筒部でなく小径部を形成し、ステータ中心軸部側
4に小径部でなく円筒部を形成してもよい。Note that, contrary to each of the above embodiments, the inner tube 10
A small diameter portion instead of a cylindrical portion may be formed on the side, and a cylindrical portion instead of a small diameter portion may be formed on the stator central shaft side 4.
[発明の効果]
本発明は上記の通り構成されているので、次のような効
果を奏する。[Effects of the Invention] Since the present invention is configured as described above, it has the following effects.
請求項1のスラスト軸受は取り付け構造によれば、円筒
部の内面と小径部の外面とのギャップがスラスト軸受け
である円形シートの厚みtより小さくされているので、
円形シートが半径方向に延びて厚みが薄くなることが防
止され、スラスト軸受けとしての寿命が長くなる。According to the mounting structure of the thrust bearing according to claim 1, the gap between the inner surface of the cylindrical portion and the outer surface of the small diameter portion is smaller than the thickness t of the circular sheet that is the thrust bearing.
This prevents the circular sheet from extending in the radial direction and becoming thinner, extending the life of the thrust bearing.
請求項2のスラスト軸受は取り付け構造によれば、円形
シートのある軸受は面を磁気回路としない構造であるか
ら、円形シートの厚みを厚くすることができ、これによ
りスラスト軸受けとしての寿命を長くすることができる
。According to the mounting structure of the thrust bearing of claim 2, since the bearing with the circular sheet has a structure in which the surface does not have a magnetic circuit, the thickness of the circular sheet can be increased, thereby extending the life of the thrust bearing. can do.
また、インナーチューブとステータ中心軸部との間に働
く磁気吸引力が小さくなり、スラスト軸受けに働くスラ
スト荷重が小さくなるので、この点でもスラスト軸受け
としての寿命が長くなる。Furthermore, the magnetic attraction force acting between the inner tube and the stator central shaft portion is reduced, and the thrust load acting on the thrust bearing is reduced, so the life of the thrust bearing is extended in this respect as well.
第1図は請求項1の発明の一実施例を示すスラスト軸受
は取り付け構造の断面図、第2図は請求項2の発明の一
実施例を示すスラスト軸受は取り付け構造の断面図、第
3図は従来のスラスト軸受は取り付け構造を持つ電磁ク
ラッチの断面図、第4図および第5図は従来のスラスト
軸受は取り付け構造の問題を説明する図である。
2・・・ステータ、4・・・ステータ中心軸部、4a・
・小径部、5・・・電磁コイル、6・・・ローラ、9・
・中心貫通軸、10・・・インナーチューブ、10a・
・・筒状部、14・・・円形シート(スラスト軸受け)
。FIG. 1 is a sectional view of the mounting structure of a thrust bearing showing an embodiment of the invention of claim 1, FIG. 2 is a sectional view of the mounting structure of a thrust bearing showing an embodiment of the invention of claim 2, and FIG. The figure is a sectional view of an electromagnetic clutch having a conventional thrust bearing mounting structure, and FIGS. 4 and 5 are diagrams illustrating problems with the conventional thrust bearing mounting structure. 2... Stator, 4... Stator center shaft portion, 4a.
・Small diameter part, 5... Electromagnetic coil, 6... Roller, 9.
・Center penetrating shaft, 10... Inner tube, 10a・
...Cylindrical part, 14...Circular seat (thrust bearing)
.
Claims (2)
るステータの中心軸部の端面との間にスラスト軸受けと
して円形シートを配置した電磁クラッチにおけるスラス
ト軸受け取り付け構造であって、 前記インナーチューブの端部またはステータ中心軸部の
端部の一方に薄肉の円筒部、他方に前記円筒部に嵌合す
る小径部を形成し、前記円筒部の内面と前記小径部の外
面とのギャップxをスラスト軸受けである前記円形シー
トの厚みtより小さく形成したことを特徴とする電磁ク
ラッチにおけるスラスト軸受け取り付け構造。(1) A thrust shaft mounting structure in an electromagnetic clutch in which a circular seat is disposed as a thrust bearing between an end face of an inner tube of a rotor and an end face of a central shaft portion of a stator opposing thereto, wherein the end face of the inner tube Alternatively, a thin cylindrical part is formed at one end of the stator central shaft part, and a small diameter part that fits into the cylindrical part is formed at the other end, and the gap x between the inner surface of the cylindrical part and the outer surface of the small diameter part is filled with a thrust bearing. A thrust shaft mounting structure for an electromagnetic clutch, characterized in that the structure is formed to be smaller than the thickness t of a certain circular sheet.
るステータの中心軸部の端面との間にスラスト軸受けと
して円形シートを配置した電磁クラッチにおけるスラス
ト軸受け取り付け構造であって、 前記インナーチューブの端部またはステータ中心軸部の
端部の一方に厚肉かつ深い円筒部、他方に前記円筒部に
嵌合する小径部を形成するとともに、前記円筒部と小径
部との嵌合面の面積がインナーチューブの断面積とほぼ
同等かそれより大きく、かつ、前記小径部の断面積およ
び円筒部の断面積がいずれも、電磁コイルが発生する磁
束を通すために十分な面積を持つことを特徴とする電磁
クラッチにおけるスラスト軸受け取り付け構造。(2) A thrust shaft mounting structure in an electromagnetic clutch in which a circular seat is arranged as a thrust bearing between an end face of an inner tube of a rotor and an end face of a center shaft portion of a stator opposing thereto, the end face of the inner tube Alternatively, a thick and deep cylindrical portion is formed at one end of the stator center shaft portion, and a small diameter portion that fits into the cylindrical portion is formed at the other end, and the area of the fitting surface between the cylindrical portion and the small diameter portion is the inner tube. The electromagnetic coil is substantially equal to or larger than the cross-sectional area of the electromagnetic coil, and the cross-sectional area of the small diameter portion and the cross-sectional area of the cylindrical portion are both sufficient to pass the magnetic flux generated by the electromagnetic coil. Thrust shaft mounting structure in clutch.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2172485A JP2779545B2 (en) | 1990-06-29 | 1990-06-29 | Thrust bearing mounting structure for electromagnetic clutch |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2172485A JP2779545B2 (en) | 1990-06-29 | 1990-06-29 | Thrust bearing mounting structure for electromagnetic clutch |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0460221A true JPH0460221A (en) | 1992-02-26 |
JP2779545B2 JP2779545B2 (en) | 1998-07-23 |
Family
ID=15942863
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2172485A Expired - Lifetime JP2779545B2 (en) | 1990-06-29 | 1990-06-29 | Thrust bearing mounting structure for electromagnetic clutch |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2779545B2 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2004031601A1 (en) * | 2002-10-03 | 2004-04-15 | Oiles Corporation | Sliding bearing |
CN100436850C (en) * | 2002-10-03 | 2008-11-26 | 奥依列斯工业株式会社 | Sliding bearing |
US7993061B2 (en) | 2002-10-03 | 2011-08-09 | Oiles Corporation | Sliding bearing |
JP2013011288A (en) * | 2011-06-28 | 2013-01-17 | Toyota Motor Corp | Electromagnetic engagement device |
-
1990
- 1990-06-29 JP JP2172485A patent/JP2779545B2/en not_active Expired - Lifetime
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2004031601A1 (en) * | 2002-10-03 | 2004-04-15 | Oiles Corporation | Sliding bearing |
JP2004176728A (en) * | 2002-10-03 | 2004-06-24 | Oiles Ind Co Ltd | Sliding bearing |
US7293918B2 (en) | 2002-10-03 | 2007-11-13 | Oiles Corporation | Sliding bearing |
US7407329B2 (en) | 2002-10-03 | 2008-08-05 | Oiles Corporation | Sliding bearing |
CN100436850C (en) * | 2002-10-03 | 2008-11-26 | 奥依列斯工业株式会社 | Sliding bearing |
KR100976867B1 (en) * | 2002-10-03 | 2010-08-24 | 오일레스고교 가부시키가이샤 | Sliding Bearing |
US7993061B2 (en) | 2002-10-03 | 2011-08-09 | Oiles Corporation | Sliding bearing |
JP2013011288A (en) * | 2011-06-28 | 2013-01-17 | Toyota Motor Corp | Electromagnetic engagement device |
Also Published As
Publication number | Publication date |
---|---|
JP2779545B2 (en) | 1998-07-23 |
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