JPH045855B2 - - Google Patents

Info

Publication number
JPH045855B2
JPH045855B2 JP57127127A JP12712782A JPH045855B2 JP H045855 B2 JPH045855 B2 JP H045855B2 JP 57127127 A JP57127127 A JP 57127127A JP 12712782 A JP12712782 A JP 12712782A JP H045855 B2 JPH045855 B2 JP H045855B2
Authority
JP
Japan
Prior art keywords
magnetic particles
drive member
working space
driven member
driven
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.)
Expired - Lifetime
Application number
JP57127127A
Other languages
Japanese (ja)
Other versions
JPS5919725A (en
Inventor
Toshihiro Takei
Takahiro Goshima
Yoshuki Hatsutori
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Denso Corp
Original Assignee
NipponDenso Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by NipponDenso Co Ltd filed Critical NipponDenso Co Ltd
Priority to JP12712782A priority Critical patent/JPS5919725A/en
Publication of JPS5919725A publication Critical patent/JPS5919725A/en
Publication of JPH045855B2 publication Critical patent/JPH045855B2/ja
Granted legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16DCOUPLINGS FOR TRANSMITTING ROTATION; CLUTCHES; BRAKES
    • F16D37/00Clutches in which the drive is transmitted through a medium consisting of small particles, e.g. centrifugally speed-responsive
    • F16D37/02Clutches in which the drive is transmitted through a medium consisting of small particles, e.g. centrifugally speed-responsive the particles being magnetisable
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16DCOUPLINGS FOR TRANSMITTING ROTATION; CLUTCHES; BRAKES
    • F16D37/00Clutches in which the drive is transmitted through a medium consisting of small particles, e.g. centrifugally speed-responsive
    • F16D2037/002Clutches in which the drive is transmitted through a medium consisting of small particles, e.g. centrifugally speed-responsive characterised by a single substantially axial gap in which the fluid or medium consisting of small particles is arranged

Landscapes

  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • One-Way And Automatic Clutches, And Combinations Of Different Clutches (AREA)
  • Braking Arrangements (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は自動車や各種産業機械に使用され、磁
粉を媒体としてトルク伝達の通断を行う電磁パウ
ダー式クラツチに関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to an electromagnetic powder clutch used in automobiles and various industrial machines, which uses magnetic powder as a medium to transmit torque.

〔従来の技術〕 この種の電磁パウダー式クラツチは、駆動側回
転体であるドライブメンバと被駆動側回転体であ
るドリブンメンバとの間に動作空〓を形成し、こ
の動作空〓に磁粉を充填するとともに、この磁粉
を電磁力により上記動作空〓内に集結させ、磁粉
相互間の磁気吸引力および磁粉と動作面との摩擦
によつてドライブメンバのトルクをドリブンメン
バに伝達するようになつている。
[Prior Art] This type of electromagnetic powder clutch forms a working space between a drive member, which is a rotating body on the driving side, and a driven member, which is a rotating body on the driven side, and injects magnetic powder into this working space. At the same time, the magnetic particles are concentrated in the operating space by electromagnetic force, and the torque of the drive member is transmitted to the driven member by the magnetic attraction between the magnetic particles and the friction between the magnetic particles and the operating surface. ing.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかしながら、従来の電磁パウダー式クラツチ
においては、無励磁時に磁粉が動作空〓から離脱
してドライブメンバやドリブンメンバの側面等に
付着し、再度の励磁時に磁粉が動作空〓内に有効
に集結せず、トルク伝達が十分に行えない不具合
があつた。特に、クラツチ連結時の立上がり特性
に劣り、励磁を数回繰り返さないと最初から大き
な動力伝達が行えない場合があつた。
However, in conventional electromagnetic powder type clutches, when the clutch is not energized, the magnetic particles separate from the working air and adhere to the drive member or the side surfaces of the driven member, and when the clutch is energized again, the magnetic particles cannot effectively collect in the working air. First, there was a problem in which the torque could not be transmitted sufficiently. In particular, the start-up characteristics when the clutch is engaged are poor, and large power transmission may not be possible from the beginning unless excitation is repeated several times.

本発明はこのような事情にもとづきなされたも
ので、その目的とするのは、動作空〓から脱落離
脱した磁粉を効果的に動作空〓へ集結させ、最初
から大きな力でトルク伝達が行える電磁パウダー
式クラツチを提供しようとするものである。
The present invention was made based on the above circumstances, and its purpose is to effectively collect the magnetic particles that have fallen off from the working space into the working space, and to create an electromagnetic system that can transmit torque with a large force from the beginning. It is an attempt to provide a powder type clutch.

〔課題を解決するための手段〕[Means to solve the problem]

すなわち本発明は、動作空〓における径方向の
間隔を軸方向に沿うどこの箇所も同等寸法とし、
この動作空〓の軸方向両端部に軸方向中央部に近
づくに応じて径が大きくなる傾斜または屈曲され
た端部空〓を形成し、これら端部空〓におけるド
ライブメンバ側に形成した傾斜または屈曲された
内面と上記動作空〓との境界部を、上記ドリブン
メンバの軸方向両端よりも中央部寄りに位置させ
たことを特徴とする。
In other words, in the present invention, the radial spacing in the working space is made the same size everywhere along the axial direction,
An inclined or bent end cavity is formed at both axial ends of this operating cavity, the diameter of which increases as it approaches the center in the axial direction, and an inclined or bent end cavity is formed on the drive member side of these end cavities. It is characterized in that the boundary between the bent inner surface and the operating space is located closer to the center of the driven member than both ends in the axial direction.

〔作用〕[Effect]

このような構成によると、消磁時に動作面から
離脱して動作空〓の端部やドライブメンバやドリ
ブンメンバの側面等に分散された磁粉は、回転に
よる遠心力を受けて上記傾斜または屈曲された端
部空〓の案内作用により動作空〓に集結されるよ
うになる。このため、動作空〓には動力伝達に有
効な量の磁粉を集めることができ、励磁時に磁化
される磁粉の量が多くなるので励磁の当初から大
きなトルクの伝達を可能にする。この場合、端部
空〓は傾斜または屈曲した形状であるから遠心力
による磁粉の移動を円滑に案内し、しかもこれら
端部空〓におけるドライブメンバ側に形成した傾
斜または屈曲形状の内面と上記動作空〓との境界
部を、ドリブンメンバの軸方向両端よりも中央部
寄りに位置させたので、遠心力により動作空〓に
集結しようとする磁粉のこどれが少なく、磁粉は
動力伝達に有効な動作空〓に確実に集まるように
なり、トルク伝達の効率を高めることができる。
According to such a configuration, the magnetic particles separated from the operating surface during demagnetization and dispersed at the end of the operating space, the side surface of the drive member, and the driven member are tilted or bent by the centrifugal force caused by rotation. Due to the guiding effect of the end air, the particles are concentrated into the operating air. Therefore, an amount of magnetic particles effective for power transmission can be collected in the operating space, and the amount of magnetic particles magnetized during excitation increases, making it possible to transmit a large torque from the beginning of excitation. In this case, since the end cavities have an inclined or bent shape, they can smoothly guide the movement of magnetic particles due to centrifugal force, and the above-mentioned operation can be achieved with the inclined or bent inner surface formed on the drive member side of these end cavities. Since the boundary with the air is located closer to the center than both ends of the driven member in the axial direction, there are fewer magnetic particles that tend to gather in the operating air due to centrifugal force, and the magnetic particles are effective for power transmission. It will surely gather in the working space and improve the efficiency of torque transmission.

〔実施例〕〔Example〕

以下本発明の一実施例を、第1図および第2図
にもとづき説明する。
An embodiment of the present invention will be described below with reference to FIGS. 1 and 2.

図において1は、駆動側回転体であるところの
ドライブメンバであり、このドライブメンバ1
は、左右2つ割りの磁性体からなるヨーク2a,
2b内に励磁コイル3を収容し、一方のヨーク2
aにフランジ4およびフロントカバー5を取着す
るとともに、他方のヨーク2bにドリブンホルダ
6、このドリブンホルダ6に固着されたリヤラビ
リンス7およ同じくドリブンホルダ6に取付けら
れた電流供給部であるスリツプリング8…を一体
的に取着して構成されている。
In the figure, 1 is a drive member which is a rotating body on the drive side, and this drive member 1
is a yoke 2a made of a magnetic material divided into left and right halves,
The excitation coil 3 is housed in 2b, and one yoke 2
A flange 4 and a front cover 5 are attached to the other yoke 2b, a driven holder 6 is attached to the other yoke 2b, a rear labyrinth 7 fixed to the driven holder 6, and a slip which is a current supply part also attached to the driven holder 6. It is constructed by integrally attaching rings 8...

本発明の電磁パウダー式クラツチを車輛用クラ
ツチとして適用する場合は、上記フランジ4に、
ボルト9…を介して、エンジンのクランク軸10
に取り付けられたリングギア11を連結する。
When the electromagnetic powder clutch of the present invention is applied as a vehicle clutch, the flange 4 includes:
Engine crankshaft 10 via bolts 9...
The ring gear 11 attached to is connected.

前記フローカバー5およびリヤラビリンス7は
いづれも非磁性体からなり、これらフロントカバ
ー5およびリヤラビリンス7のドリブンメンバ2
0に対向する先端部には、全周に亘つて環状のゴ
ム磁石12が接着されている。上記スリツプリン
グ8…にはブラシ13…が摺接されており、これ
らブラシ13はブラシホルダ14に取着されてい
る。なおブラシホルダ14は図示しないクラツチ
カバーに固定されている。
The flow cover 5 and the rear labyrinth 7 are both made of non-magnetic material, and the driven member 2 of the front cover 5 and the rear labyrinth 7 is
An annular rubber magnet 12 is adhered to the tip portion facing 0 over the entire circumference. Brushes 13 are in sliding contact with the slip rings 8, and these brushes 13 are attached to a brush holder 14. The brush holder 14 is fixed to a clutch cover (not shown).

被駆動側回転体としてのドリブンメンバ20は
磁性体からなり、中心部にハブ21をねじ止めに
より備えている。ハブ21にはトランスミツシヨ
ンのインプツトシヤフト22がスプライン23を
介して係合されており、ドリブンメンバ20とイ
ンプツトシヤフト22は一体に回転する。ハブ2
1は、サークリツプ24,25により固定された
軸受26により、ドリブンホルダ6に軸方向には
固定でかつ回転自在に支持されている。
The driven member 20, which serves as a driven rotating body, is made of a magnetic material and has a hub 21 screwed in its center. An input shaft 22 of the transmission is engaged with the hub 21 via a spline 23, and the driven member 20 and input shaft 22 rotate together. hub 2
1 is fixed in the axial direction and rotatably supported by the driven holder 6 by a bearing 26 fixed by circlips 24 and 25.

ドライブメンバ1の内周面とドリブンメンバ2
0の外周面との間には動作空〓27が形成されて
おり、この動作空〓27内には磁粉28が充填さ
れている。この磁粉28は励磁コイル3によつて
励磁されると、磁粉28相互の磁気吸引力および
磁粉28とドライブメンバ1およびドリブンメン
バの動作面との摩擦力により、ドライブメンバ1
の回転トルクをドリブンメンバ20に伝達し、両
者を一体的に回転させる。
Inner peripheral surface of drive member 1 and driven member 2
A working space 27 is formed between the outer circumferential surface of the magnet and the working space 27, and this working space 27 is filled with magnetic particles 28. When the magnetic particles 28 are excited by the excitation coil 3, the magnetic attraction force between the magnetic particles 28 and the frictional force between the magnetic particles 28 and the drive member 1 and the operating surface of the driven member cause the drive member 1 to move.
is transmitted to the driven member 20, causing both to rotate integrally.

動作空〓27の軸方向に沿う両端部位には、第
2図に示されるように端部空〓29a,29bが
形成されている。これら端部空〓29a,29b
に臨む位置のドライブメンバ1側には、具体的に
はフロントカバー5およびドリブンホルダ6に
は、動作空〓27の軸方向に沿う中央部に向つて
内径が増大される傾斜面30a,30bが形成さ
れている。このような傾斜面30a,30bに対
向してドリブンメンバ20の角部には、上記傾斜
面30a,30bと平行な傾斜面31a,31b
が形成されている。上記一方の傾斜面30aの動
作空〓27の中央部に向かう終端30aaと傾斜
面31aの同じく終端31aaは軸方向に沿つて
同じ位置に対向されているとともに、上記他方の
傾斜面30bの終端30bbと傾斜面31bの終
端31bbも軸方向に沿つて同じ位置に対向され
ている。このため各傾斜面30aと31aとの間
隔、および30bと31bとの間隔は、それぞれ
軸方向に沿つて一定となつており、かつこれらの
間隔部は動作空〓27に対して大きく折曲するこ
となく滑らかに連続している。したがつて、動作
空〓27は軸方向全体に亘り空〓幅の寸法が一定
となつている。
As shown in FIG. 2, end cavities 29a and 29b are formed at both end portions of the operating cavity 27 along the axial direction. These ends are empty 〓 29a, 29b
On the side of the drive member 1 facing the front cover 5 and the driven holder 6, there are inclined surfaces 30a and 30b whose inner diameters increase toward the center along the axial direction of the operating space 27. It is formed. At the corners of the driven member 20 facing the inclined surfaces 30a, 30b, there are inclined surfaces 31a, 31b parallel to the inclined surfaces 30a, 30b.
is formed. The terminal end 30aa of the one inclined surface 30a toward the center of the operating space 27 and the terminal end 31aa of the inclined surface 31a are opposed to each other at the same position along the axial direction, and the terminal end 30bb of the other inclined surface 30b and the terminal end 31bb of the inclined surface 31b are also opposed to each other at the same position along the axial direction. Therefore, the distance between the inclined surfaces 30a and 31a and the distance between 30b and 31b are constant along the axial direction, and these distances are largely bent with respect to the operating space 27. Continuously and smoothly. Therefore, the width of the working space 27 is constant throughout the axial direction.

そして、この場合、ドライブメンバ1側の内面
に形成された傾斜面30a,30bにおける動作
空〓27の中央部に向かう終端30aaおよび3
0bb、すなわち傾斜面30a,30bと動作空
〓27との境界部は、当然ながら、ドリブンメン
バ20の軸方向両端よりも上記中央側に位置して
いる。
In this case, the terminal ends 30aa and 3 toward the center of the operating space 27 on the inclined surfaces 30a and 30b formed on the inner surface on the drive member 1 side.
0bb, that is, the boundary between the inclined surfaces 30a, 30b and the working space 27, is naturally located closer to the center than both ends of the driven member 20 in the axial direction.

このような構成による実施例の作用について説
明する。
The operation of the embodiment with such a configuration will be explained.

第1図において、エンジンからの動力はクラン
ク軸10を通じてリングギア11からドライブメ
ンバ1に伝達され、したがつてドライブメンバ1
はエンジンの回転とともに一体的に回転する。
In FIG. 1, power from the engine is transmitted from the ring gear 11 to the drive member 1 through the crankshaft 10, and therefore the drive member 1
rotates as the engine rotates.

電磁コイル3に通電して磁粉28が存在してい
る動作空〓27に磁束を生じさせると、磁粉28
が磁化され、磁粉相互の磁気的な結合力、および
磁粉28と動作面との摩擦力によつて上記エンジ
ンの動力がドライブメンバ1からドリブンメンバ
20に伝達される。したがつて、ハブ21からス
プライン23を介してトランスミツシヨンのイン
プツトシヤフト22に上記エンジンの動力が伝達
される。上記動作空〓27に磁束を生じさせるコ
イル3にはブラシ13からスリツプリング8を介
して給電され、このコイル3に電流が流れること
により、ヨーク2a,2b、動作空〓27、ドリ
ブンメンバ20を通る磁気回路が形成され、これ
により磁束が発生する。よつてコイル3への励磁
電流の有無により回転トルクの伝達の可、不可が
決定される。
When the electromagnetic coil 3 is energized to generate magnetic flux in the operating space 27 where the magnetic particles 28 are present, the magnetic particles 28
is magnetized, and the power of the engine is transmitted from the drive member 1 to the driven member 20 by the magnetic coupling force between the magnetic particles and the frictional force between the magnetic particles 28 and the operating surface. Therefore, the power of the engine is transmitted from the hub 21 via the spline 23 to the input shaft 22 of the transmission. Power is supplied from the brush 13 to the coil 3 that generates a magnetic flux in the working space 27 via the slip ring 8, and as a result of current flowing through the coil 3, the yokes 2a, 2b, the working space 27, and the driven member 20 are A magnetic circuit is formed through which a magnetic flux is generated. Therefore, whether or not rotational torque can be transmitted is determined by the presence or absence of excitation current to the coil 3.

コイル3に通電された状態では磁粉28が動作
空〓27内で最つとも強く磁化されるが、通電を
断つた場合は磁化が開放状態となり、磁粉28は
遠心力によりドライブメンバ1の内面に押しつけ
られて完全に連結が断たれる。
When the coil 3 is energized, the magnetic particles 28 are most strongly magnetized in the operating space 27, but when the energization is cut off, the magnetization becomes open, and the magnetic particles 28 are attracted to the inner surface of the drive member 1 by centrifugal force. It is pushed and the connection is completely severed.

この場合、磁粉28…は動作空〓27のみなら
ず、動作空〓27両端の空〓29a,29bにも
離散分布する。また、エンジンを停止した場合
は、フロントカバー5およびドリブンホルダ6の
側面、ドリブンメンバ20の端面などに分散して
付着する。このように分散した磁粉28…は再度
の励磁により動作空〓27内に円滑に移動集結せ
ず、このため動力伝達に寄与しないことがある。
In this case, the magnetic particles 28 are discretely distributed not only in the working space 27 but also in the spaces 29a and 29b at both ends of the working space 27. Furthermore, when the engine is stopped, the particles are dispersed and adhere to the side surfaces of the front cover 5 and driven holder 6, the end surface of the driven member 20, and the like. The magnetic particles 28 dispersed in this manner may not smoothly move and condense within the working space 27 due to re-excitation, and therefore may not contribute to power transmission.

しかるに、本発明においては、端部空〓29
a,29bやその外に分散された磁粉28を、遠
心力によつて動作空〓27内に強制的に送り込む
ことができる。すなわち、エンジンを回転させる
と、無励磁状態であつてもドライブメンバ1はエ
ンジンとともに回転しているのに対し、ドリブン
メンバ20は停止している。この場合、端部空〓
29a,29b内の磁粉28はドライブメンバ1
の回転に伴つてつれ回り回転させられ、よつて遠
心力によりドライブメンバ1側の内面の傾斜面3
0a,30bに押し付けられる。傾斜面30a,
30bは動作空〓27に向つて拡径されているの
で、これら傾斜面30a,30bは磁粉29を動
作空〓27に案内移動させる。したがつて端部空
〓29a,29b内の磁粉29は遠心力および傾
斜面30a,30bのガイド作用により効果的に
動作空〓27内に集結させられ、再度の励磁時に
は速やかに動力連結に寄与し、最初から大きなト
ルク伝達を行うことができ、立上がり特性も向上
する。
However, in the present invention, the end space 29
The magnetic particles 28 dispersed in a, 29b and outside can be forcibly fed into the working space 27 by centrifugal force. That is, when the engine is rotated, the drive member 1 rotates together with the engine even in a non-excited state, whereas the driven member 20 is stopped. In this case, the end is empty
The magnetic particles 28 in 29a and 29b are part of the drive member 1
The inclined surface 3 on the inner surface of the drive member 1 side is rotated by the centrifugal force.
It is pressed against 0a and 30b. Slanted surface 30a,
Since the diameter of magnetic powder 30b is increased toward the working space 27, these inclined surfaces 30a and 30b guide the magnetic particles 29 toward the working space 27. Therefore, the magnetic particles 29 in the end spaces 29a and 29b are effectively concentrated in the operating space 27 by the centrifugal force and the guiding action of the inclined surfaces 30a and 30b, and quickly contribute to power connection when excitation is re-energized. However, large torque transmission can be performed from the beginning, and the start-up characteristics are also improved.

この場合、傾斜面の終端30aaと31aa、す
なわち傾斜面30aおよび30bと動作空〓27
の境界部は、ドリブンメンバ20の軸方向幅より
内側(中央部側)に設置されているので、遠心力
により傾斜面30a,30bに沿つて動作空〓2
7内に移動しようとする磁粉28がこぼれること
はなく、効果的に動作空〓27に集まる。
In this case, the terminal ends 30aa and 31aa of the inclined surfaces, that is, the inclined surfaces 30a and 30b and the operating space 27
Since the boundary portion of the driven member 20 is located inside (on the center side) of the axial width of the driven member 20, the operating space 〓2
The magnetic particles 28 that try to move into the space 7 do not spill out and are effectively collected in the working space 27.

また、本実施例の場合、傾斜面30aと31
a、および30bと31bが互に平行であるの
で、これらの対向間隔が軸方向に向つて一定とな
つており、磁粉28が動作空〓27に向つて移動
するのを阻害しない。
In addition, in the case of this embodiment, the inclined surfaces 30a and 31
Since a, 30b and 31b are parallel to each other, the distance between them is constant in the axial direction, and movement of the magnetic particles 28 toward the working space 27 is not inhibited.

さらに、傾斜面の終端30aaと31aa、およ
び30bbと31bbが互に軸方向に沿う同じ位置
に対向されているので、端部空〓29a,29b
から動作空〓27に向つて移動しようとする磁粉
28の通路抵抗が小さくなり、よつて磁粉28を
円滑に案内移動させることができる。
Furthermore, since the terminal ends 30aa and 31aa and 30bb and 31bb of the inclined surface are opposed to each other at the same position along the axial direction, the end portions 29a and 29b are
The passage resistance of the magnetic particles 28 trying to move toward the working space 27 is reduced, so that the magnetic particles 28 can be guided and moved smoothly.

一方、動作空〓27は、空〓寸法が軸方向に沿
つて一定となつているので軸方向のどこの場所で
も間〓を小さく保つことができ、よつてトルク伝
達率を高くすることができ、トルク伝達に消費す
る電磁コイルへの通電量を低減することができ
る。
On the other hand, since the working space 27 has a constant space size along the axial direction, the space can be kept small at any location in the axial direction, and thus the torque transmission rate can be increased. , it is possible to reduce the amount of current to the electromagnetic coil consumed for torque transmission.

なお、本発明は、第3図に示すような他の実施
例であつても実施可能である。すなわち、第3図
の場合、動作空〓27の動作面を、中央部に近づ
くに応じて拡径される傾斜面40a,40bおよ
び41a,41bとしたものである。
It should be noted that the present invention can be practiced even with other embodiments as shown in FIG. That is, in the case of FIG. 3, the operating surfaces of the operating space 27 are sloped surfaces 40a, 40b and 41a, 41b whose diameter increases as they approach the center.

また、端部空〓29a,29bは各傾斜面40
a,40b,41a,41bに滑らかに連続する
曲面42a,42b,43a,43bとしてあ
る。
In addition, the end spaces 29a and 29b are each sloped surface 40.
The curved surfaces 42a, 42b, 43a, 43b are smoothly continuous with the curved surfaces 42a, 40b, 41a, 41b.

そして、端部空〓29a,29bに臨むドライ
ブメンバ1の内面側の曲面42a,42bの終端
42aaと42bb、すなわち動作空〓27の境界
部は、ドリブンメンバ20の軸方向幅より内側
(中央部側)に設置されており、このため、遠心
力により曲面42a,42bに沿つて動作空〓2
7内に移動しようとする磁粉28は効果的に動作
空〓27に集まる。
The terminal ends 42aa and 42bb of the inner curved surfaces 42a and 42b of the drive member 1 facing the end spaces 29a and 29b, that is, the boundary between the operating space 27, are located inside the axial width of the driven member 20 (the central part Therefore, centrifugal force causes movement along the curved surfaces 42a and 42b.
The magnetic particles 28 trying to move into the space 7 effectively gather in the working space 27.

なお、本発明は、各実施例から理解できるよう
に、動作空〓27の形状と端部空〓29a,29
bの形状の組合わせは任意に選択することがで
き、かつ動作空〓27は中央部に近づくに応じて
拡径される曲面に形成してもよい。
In addition, as can be understood from each embodiment, the present invention is characterized by the shape of the operating space 27 and the end spaces 29a, 29.
The combination of shapes b can be arbitrarily selected, and the working space 27 may be formed into a curved surface whose diameter increases as it approaches the center.

なお、各実施例では、第2図および第3図に示
す通り、ドリブンメンバ20の動作面の中央部に
周方向に沿う溝35を形成してあるが、この溝3
5は励磁コイル3の磁束をドリブンメンバ20側
に迂回させるためのものであり、トルク伝達には
寄与しない。
In each embodiment, as shown in FIGS. 2 and 3, a groove 35 is formed along the circumferential direction in the center of the operating surface of the driven member 20.
5 is for detouring the magnetic flux of the exciting coil 3 to the driven member 20 side, and does not contribute to torque transmission.

また、第2図におけるドリブンメンバ20の動
作面に形成した凹部36…は、磁粉の分布を均一
にするもので、トルク伝達には影響しない。
Further, the recesses 36 formed on the operating surface of the driven member 20 in FIG. 2 are for making the distribution of magnetic particles uniform, and do not affect torque transmission.

さらに本発明は、ドライブメンバ1の回転に伴
う遠心力と、傾斜面もしくは曲面のガイド作用に
よつて端部空〓29a,29bの磁粉を動作空〓
27に集結させるものであるから、少なくともド
ライブメンバ1の内周面に形成した傾斜面または
曲面30a,30b,42a,42bと、動作空
〓27との境界部が、ドリブンメンバ20の軸方
向両端位置よりも中央部側に位置しておればよ
い。よつて、ドリブンメンバ20の角部に形成さ
れた傾斜面または曲面31a,31b,43a,
43bと、動作空〓27との境界部は、必ずしも
上記ドライブメンバ1の内面30a,30b,4
2a,42bと動作空〓27との境界部に一致さ
せる必要はない。
Furthermore, the present invention uses the centrifugal force accompanying the rotation of the drive member 1 and the guiding action of the inclined or curved surface to move the magnetic particles in the end spaces 29a and 29b into the operating space.
27, the boundary between at least the inclined surfaces or curved surfaces 30a, 30b, 42a, 42b formed on the inner circumferential surface of the drive member 1 and the operating space 27 is at both axial ends of the driven member 20. It suffices if it is located closer to the center than the position. Therefore, the inclined surfaces or curved surfaces 31a, 31b, 43a,
43b and the operating space 27 are not necessarily the inner surfaces 30a, 30b, 4 of the drive member 1.
It is not necessary to match the boundary between 2a, 42b and the operating space 27.

〔発明の効果〕〔Effect of the invention〕

以上詳述した通り本発明によれば、消磁時に動
作面から離脱して動作空〓の端部やその外部の近
傍に分散された磁粉は、回転による遠心力を受け
て傾斜または屈曲形状をなしている端部空〓のガ
イド作用により、動力伝達に有効な中央側の動作
空〓に集結されるようになる。このため励磁時に
有効に磁化される磁粉の量が多くなり、励磁の最
初から大きなトルク伝達を可能となり、立上り特
性が向上する。この場合、端部空〓は傾斜または
屈曲した形状であるから遠心力による磁粉の移動
を円滑に案内し、しかもこれら端部空〓における
ドライブメンバ側に形成した傾斜または屈曲形状
の内面と上記動作空〓との境界部を、ドリブンメ
ンバの軸方向両端よりも中央部寄りに位置させた
ので、遠心力により動作空〓に集結しようとする
磁粉のこぼれが少なく、磁粉は動力伝達に有効な
動作空〓に確実に集まるようになり、トルク伝達
の効率を高めることができる。このようなことか
ら、トルク伝達に要する電磁コイルへの通電量を
低減することができる等の利点がある。
As detailed above, according to the present invention, the magnetic particles separated from the operating surface during demagnetization and dispersed near the end of the operating space or the outside thereof form an inclined or bent shape due to the centrifugal force caused by rotation. Due to the guiding effect of the end spaces, the working spaces are concentrated in the center, which is effective for power transmission. Therefore, the amount of magnetic particles that are effectively magnetized during excitation increases, making it possible to transmit a large torque from the beginning of excitation, and improving the rise characteristics. In this case, since the end cavities have an inclined or bent shape, they can smoothly guide the movement of the magnetic particles due to centrifugal force, and the above-mentioned operation can be achieved with the inclined or bent inner surface formed on the drive member side of these end cavities. Since the boundary with the air is located closer to the center than both ends of the driven member in the axial direction, there is less spillage of magnetic particles that tend to collect in the operating air due to centrifugal force, and the magnetic particles are effective for power transmission. The air will surely gather in the air, increasing the efficiency of torque transmission. For this reason, there are advantages such as being able to reduce the amount of current applied to the electromagnetic coil required for torque transmission.

【図面の簡単な説明】[Brief explanation of drawings]

第1図および第2図は本発明の一実施例を示
し、第1図は縦断面図、第2図は要部の拡大した
断面図、第3図は本発明の他の実施例を示す要部
の拡大した断面図である。 1…ドライブメンバ、3…励磁コイル、20…
ドリブンメンバ、27…動作空〓、28…磁粉、
29a,29b…端部空〓、30a,30b,4
0a,40b…ドライブメンバ側傾斜面、31
a,31b,41a,41b…ドリブンメンバ側
傾斜面、30aa,30bb…境界部、42a,4
2b…曲面、42aa,42bb…境界部。
1 and 2 show one embodiment of the present invention, FIG. 1 is a longitudinal sectional view, FIG. 2 is an enlarged sectional view of the main part, and FIG. 3 is another embodiment of the present invention. FIG. 3 is an enlarged cross-sectional view of main parts. 1... Drive member, 3... Excitation coil, 20...
Driven member, 27...Operation space, 28...Magnetic powder,
29a, 29b... end empty, 30a, 30b, 4
0a, 40b... Drive member side inclined surface, 31
a, 31b, 41a, 41b...Driven member side inclined surface, 30aa, 30bb...Boundary part, 42a, 4
2b...Curved surface, 42aa, 42bb...Boundary part.

Claims (1)

【特許請求の範囲】 1 駆動側回転体であるドライブメンバと被駆動
側回転体であるドリブンメンバとを径方向に間隔
を存して同心状に対向させ、上記間隔は軸方向に
所定の幅を有しかつ周方向に連続する動作空〓と
し、この動作空〓に磁粉を充填し、この磁粉を電
磁力により上記動作空〓に集結させて上記ドライ
ブメンバとドリブンメンバとの間で動力伝達を行
う電磁パウダー式クラツチにおいて、 上記動作空〓は径方向の間隔が軸方向に沿うど
この箇所も同等寸法とし、この動作空〓の軸方向
両端部に軸方向中央部に近づくに応じて径が大き
くなる傾斜または屈曲された端部空〓を形成し、
これら端部空〓におけるドライブメンバ側に形成
した傾斜または屈曲された内面と上記動作空〓と
の境界部を、上記ドリブメンバの軸方向両端より
も中央部寄りに位置させたことを特徴とする電磁
パウダー式クラツチ。
[Claims] 1. A drive member, which is a driving side rotating body, and a driven member, which is a driven side rotating body, are concentrically opposed to each other with an interval in the radial direction, and the interval is a predetermined width in the axial direction. The working space is continuous in the circumferential direction and is filled with magnetic particles, and the magnetic particles are concentrated in the working space by electromagnetic force to transmit power between the drive member and the driven member. In an electromagnetic powder type clutch that performs Forms a sloped or bent end cavity where the
The electromagnetic device is characterized in that the boundary between the inclined or bent inner surface formed on the drive member side of the end cavities and the operating cavity is located closer to the center than both axial ends of the drive member. Powder clutch.
JP12712782A 1982-07-21 1982-07-21 Electromagnetic powder type clutch Granted JPS5919725A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12712782A JPS5919725A (en) 1982-07-21 1982-07-21 Electromagnetic powder type clutch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12712782A JPS5919725A (en) 1982-07-21 1982-07-21 Electromagnetic powder type clutch

Publications (2)

Publication Number Publication Date
JPS5919725A JPS5919725A (en) 1984-02-01
JPH045855B2 true JPH045855B2 (en) 1992-02-03

Family

ID=14952273

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12712782A Granted JPS5919725A (en) 1982-07-21 1982-07-21 Electromagnetic powder type clutch

Country Status (1)

Country Link
JP (1) JPS5919725A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0325446Y2 (en) * 1985-01-10 1991-06-03

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2886151A (en) * 1949-01-07 1959-05-12 Wefco Inc Field responsive fluid couplings
JPS5023701U (en) * 1973-06-28 1975-03-17
JPS568898Y2 (en) * 1973-06-29 1981-02-26
JPS6114661Y2 (en) * 1980-12-12 1986-05-08

Also Published As

Publication number Publication date
JPS5919725A (en) 1984-02-01

Similar Documents

Publication Publication Date Title
EP0909901B1 (en) Magneto rheological fluid coupling
US4160498A (en) Electromagnetic coupling
US5971121A (en) Mag stop clutch with center pole
US2739683A (en) Magnetic drive
US4973870A (en) Electromagnetic clutch with flux-equalized rotating member
US5059842A (en) Electromagnetic clutch with grooved friction surface
JPH045855B2 (en)
JPH0323769B2 (en)
JPS5919724A (en) Electromagnetic powder type clutch
JPH043133Y2 (en)
JPH0325446Y2 (en)
JPS61201938A (en) Electromagnetic powder type clutch
JPS6135788Y2 (en)
JPS6322339Y2 (en)
GB2156013A (en) Electromagnetic clutch
JPH0432503Y2 (en)
JP2002340036A (en) Electromagnetic clutch
JPH0220497Y2 (en)
JPH036376B2 (en)
JPH10220492A (en) Vehicular coupling fan device
JPS61206831A (en) Electromagnetic powder type clutch
JPH0642556A (en) Electromagnetic clutch
JPS641542Y2 (en)
JPH11153158A (en) Driving force transmission device
CN118382552A (en) Power take-off with bell housing cooling system