JPH063232B2 - Magnetic particle type electromagnetic coupling device - Google Patents

Magnetic particle type electromagnetic coupling device

Info

Publication number
JPH063232B2
JPH063232B2 JP27703886A JP27703886A JPH063232B2 JP H063232 B2 JPH063232 B2 JP H063232B2 JP 27703886 A JP27703886 A JP 27703886A JP 27703886 A JP27703886 A JP 27703886A JP H063232 B2 JPH063232 B2 JP H063232B2
Authority
JP
Japan
Prior art keywords
inner end
coupling device
electromagnetic coupling
inclined surface
magnetic
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
JP27703886A
Other languages
Japanese (ja)
Other versions
JPS63130931A (en
Inventor
文雄 小野
一雄 ▲吉▼野
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP27703886A priority Critical patent/JPH063232B2/en
Publication of JPS63130931A publication Critical patent/JPS63130931A/en
Publication of JPH063232B2 publication Critical patent/JPH063232B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、駆動体から磁性粒子を介し被駆動体に駆動
力を伝達する磁性粒子式電磁連結装置に関し、特に無励
磁時における連結力発生及び励磁時における連結力低下
を防止する改良にかかわる。
Description: TECHNICAL FIELD The present invention relates to a magnetic particle type electromagnetic coupling device for transmitting a driving force from a driving body to a driven body via magnetic particles, and particularly to generating a coupling force during non-excitation. Also, it is concerned with improvement for preventing a decrease in coupling force during excitation.

〔従来の技術〕[Conventional technology]

従来のこの種の電磁連結装置は、第9図に断面図で示す
ようになっていた。図において、1は磁性材からなる固
定枠で、内部に励磁コイル2を収容しており、固定部
(図示は略す)に取付けるためのフラジ1aが設けられて
いる。3はこの固定枠の内周部に一対の軸受7を介し支
持された駆動体で、軸方向に間隔をあけて配置された磁
性材からなる両側一対の円筒状の駆動部材4,5と、こ
れら両駆動部材を一体的に結合した非磁性の結合環6と
から構成されており、外円周面が固定子1の内円周面に
エアギャップgを介し対向している。8は駆動体3の内
周部に一対の軸受11を介しし支持された被動軸、9はこ
の被動軸に固着された被駆動体で、磁性材の円板体から
なっており、両側面9a,9bが、駆動部材4,5の内端面
4a,5aと軸方向にそれぞれ小さいエアギャップg,g
を介し対向している。エアギャップg,g部には
磁性粒子10が充てんされている。12は駆動体3の内周部
に固着され被動軸8の外周面に接触し、磁性粒子10の散
出を防止するシール部材、13は被動軸8にはめられ各軸
受11を軸方向に止める一対の止め輪、14は駆動部材5に
はめられ一方の軸受7を軸方向に止める止め輪である。
A conventional electromagnetic coupling device of this type has a sectional view shown in FIG. In the figure, 1 is a fixed frame made of a magnetic material, which houses an exciting coil 2 therein, and is provided with a flange 1a for attaching to a fixed portion (not shown). Reference numeral 3 denotes a driving body supported on the inner peripheral portion of this fixed frame via a pair of bearings 7, and a pair of cylindrical driving members 4 and 5 on both sides made of a magnetic material and spaced apart in the axial direction. It is composed of a non-magnetic coupling ring 6 in which these two driving members are integrally coupled, and the outer circumferential surface faces the inner circumferential surface of the stator 1 via an air gap g. Reference numeral 8 denotes a driven shaft supported on the inner peripheral portion of the driving body 3 through a pair of bearings 11. Reference numeral 9 denotes a driven body fixed to the driven shaft, which is made of a disc body of a magnetic material. 9a and 9b are inner end surfaces of the drive members 4 and 5.
4a and 5a and air gaps g 1 and g that are small in the axial direction, respectively
They are facing each other through 2 . Magnetic particles 10 are filled in the air gaps g 1 and g 2 . Reference numeral 12 is a seal member fixed to the inner peripheral portion of the driving body 3 and in contact with the outer peripheral surface of the driven shaft 8 to prevent the magnetic particles 10 from scattering. 13 is fitted on the driven shaft 8 and stops each bearing 11 in the axial direction. A pair of retaining rings, 14 are retaining rings fitted on the driving member 5 and axially stopping the one bearing 7.

上記従来の装置の動作は、次のようになる。駆動源(図
示は略す)に結合された駆動体3が回転しているとき、
励磁コイル2に励磁電流を流すと、第9図に点線で示す
ように、磁束Φが発生し、エアギャップg,g部の
磁性粒子10が磁化し軸方向に鎖状に結合し、被駆動体9
は駆動体3に一体に又は滑りながら回転され、被動軸8
を共に回転させる。
The operation of the above conventional device is as follows. When the driving body 3 coupled to the driving source (not shown) is rotating,
When an exciting current is passed through the exciting coil 2, a magnetic flux Φ is generated as shown by the dotted line in FIG. 9, and the magnetic particles 10 in the air gaps g 1 and g 2 are magnetized and coupled in a chain shape in the axial direction, Driven body 9
Is rotated integrally with the driving body 3 or while sliding, and the driven shaft 8
Rotate together.

こうして、励磁電流を制御することにより、トルク制御
ができ、許容温度上昇内において、連続滑り状態で使用
することができるという、すぐれた長所をもっている。
Thus, by controlling the exciting current, the torque can be controlled, and there is an advantage that it can be used in a continuous sliding state within the allowable temperature rise.

第10図は無励磁で駆動体3を高速回転させている状態
を示す。高速回転による遠心力で磁性粒子10は両端面4
a,5a間の空所部の外周部へ片寄ってしまう。
FIG. 10 shows a state in which the driving body 3 is rotated at high speed without excitation. Due to the centrifugal force generated by the high speed rotation, the magnetic particles 10 have both end surfaces 4
It will be offset toward the outer periphery of the void between a and 5a.

この高速回転のとき、励磁を始めると、第11図に示す
ように、磁束Φにより磁性粒子10の一部はエアギャップ
,g部で軸方向に結合するが、空所部の外周部の
磁性粒子10は、ここを通る磁束により軸方向に結合し、
被駆動体9へのトルク伝達に寄与しない。
When excitation is started at this high speed rotation, as shown in FIG. 11, a part of the magnetic particles 10 is axially coupled at the air gaps g 1 and g 2 due to the magnetic flux Φ, but the outer periphery of the void portion is The magnetic particles 10 in the part are axially coupled by the magnetic flux passing therethrough,
It does not contribute to torque transmission to the driven body 9.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

上記のような従来の電磁連結装置では、高速回転で無励
磁状態が長く続くと、両端面4a,5a間の空所部の外周部
へ片寄ってしまった磁性粒子10群が固化状態となり、無
励磁にもかかわらず、被駆動体9と駆動体3間に連結力
が生じ、トルク伝達がなされてしまうという問題点があ
った。
In the conventional electromagnetic coupling device as described above, when a non-excited state continues for a long time at a high speed, the magnetic particles 10 group which are biased to the outer peripheral portion of the space between both end surfaces 4a and 5a are solidified, and Despite the excitation, there is a problem that a connecting force is generated between the driven body 9 and the driving body 3 and torque is transmitted.

また、駆動体3の高速回転を続けているとき、励磁を開
始すると、両端面4a,5a間の空所部の外周部の磁性粒子
10が直接連結し、トルク伝達に寄与しない府分が生じ、
エアギャップg,g部を連結する磁性粒子10が減少
し、伝達トルクが低下するという問題点があった。
Further, when excitation is started while the driving body 3 continues to rotate at high speed, the magnetic particles on the outer peripheral portion of the space between both end surfaces 4a and 5a are started.
10 is directly connected, and there is a part that does not contribute to torque transmission,
There has been a problem that the magnetic particles 10 connecting the air gaps g 1 and g 2 are reduced and the transmission torque is reduced.

これに対処し、磁性粒子10の量を増加すると、連結力を
増すことができるが、無励磁における連結力の発生が、
比較的低速回転から生じる不具合ができ、また、増加し
た磁性粒子10がシール部材12に接触することが多くな
り,シール部材の寿命が短くなるという問題点が生じ
る。
By coping with this and increasing the amount of the magnetic particles 10, the coupling force can be increased, but the generation of the coupling force in non-excitation is
There is a problem that the problems caused by the relatively low speed rotation occur, and the increased magnetic particles 10 often come into contact with the seal member 12, which shortens the life of the seal member.

この発明は、このような問題点を解決するためになされ
たもので、高速回転における無励磁時の連結力の発生を
防止し、かつ、励磁時の連結力の低下をきたすことをな
くし、また、励磁遮断時の連結力の切れをよくした磁性
粒子式電磁連結装置を得ることを目的としている。
The present invention has been made to solve such a problem, prevents the generation of a coupling force during non-excitation in high-speed rotation, and prevents a reduction in coupling force during excitation. An object of the present invention is to obtain a magnetic particle type electromagnetic coupling device in which disconnection of the coupling force when the excitation is cut off is improved.

〔問題点を解決するための手段〕[Means for solving problems]

この発明にかかる電磁連結装置は、駆動体の両駆動部材
の軸方向に対向する両内端面の外周部に、それぞれ環状
切欠き部を設け、磁性粒子の逃し込み部を形成し、か
つ、環状切欠き部の底面部を内端面側が小径になる傾斜
状面に形成したものである。
The electromagnetic coupling device according to the present invention is provided with annular notches at the outer peripheral portions of both inner end surfaces of the drive member, which face each other in the axial direction of the drive members, to form escape portions for magnetic particles, and The bottom surface of the notch is formed as an inclined surface having a smaller diameter on the inner end surface side.

〔作用〕[Action]

この発明においては、無励磁時の駆動体の高速回転にお
いて遠心力が生じた磁性粒子は、駆動体の両駆動部材の
両環状切欠き部間により形成れさた逃し込み部に収容さ
れ、連結力を生じることなく被駆動体の停止が維持され
る。また、駆動体が高速回転状態で励磁を始めると、駆
動体の逃し込み部に収容されている磁性粒子は、被駆動
体の両側のエアギャップ部に磁気吸引により円滑に引込
まれ、連結力の立上りが早くなる。
In the present invention, the magnetic particles generated by the centrifugal force in the high speed rotation of the drive body during non-excitation are accommodated in the escape portion formed between the annular cutout portions of both drive members of the drive body, and are connected. The driven body remains stopped without producing force. When the driving body starts to be excited in a high-speed rotation state, the magnetic particles contained in the escape portion of the driving body are smoothly drawn into the air gaps on both sides of the driven body by magnetic attraction, and the coupling force Starts up faster.

〔実施例〕〔Example〕

第1図はこの発明による磁性粒子式電磁連結装置の断面
図であり、1,2,6〜14,1a,9a,9bは上記従来装置
と同一のものである。20は駆動体で、軸方向に間隔をあ
けて配置され、磁性材からなる両側一対の円筒状の駆動
部材21,22と、これら両駆動部材を一体的に結合した非
磁性の結合環6とから構成されている。両駆動部材21,
22の対向する内端面21a,22a間に被駆動体9が小さいエ
アギャップg,gを介し配置されている。駆動部材
21,22の内端面21a,22aの外周部には、軸方向及び半径
方向に広げられた環状切込み部21b,22bが形成されてい
る。
FIG. 1 is a sectional view of a magnetic particle type electromagnetic coupling device according to the present invention, in which 1, 2, 6 to 14, 1a, 9a and 9b are the same as those of the conventional device. Reference numeral 20 denotes a driving body, which is arranged at a distance in the axial direction and has a pair of cylindrical driving members 21 and 22 made of a magnetic material, and a non-magnetic coupling ring 6 integrally coupling these driving members. It consists of Both drive members 21,
The driven body 9 is arranged between the inner end surfaces 21a, 22a facing each other of 22 via small air gaps g 1 , g 2 . Drive member
On the outer peripheral portions of the inner end surfaces 21a and 22a of the reference numerals 21 and 22, annular cut portions 21b and 22b that are widened in the axial direction and the radial direction are formed.

上記駆動部材21,22の環状切込み部21b,22b部を第2図
に拡大図で示す。この第2図は、駆動体20が高速回転で
無励磁状態を示している。切込み部21b,22bの底面部
は、内端面21a,22a側を小径(外径A)にした傾斜面21
c,22cに形成されている。両切欠き部21b,22bと結合環
6内円周部とによる空所により幅cの広い逃し込み部23
をなしており、駆動体20の高速回転無励時の遠心作用に
よる磁性粒子10を収容する。駆動部材21,22の内端面の
外円周部(外径A)と傾斜面21c,22cとの角部は円弧面
による面とり部21d,22dにより丸められてあり、逃し込
み部23に収容状態の磁性粒子の、励磁によるエアギャッ
プg,gへの磁気吸引移動を円滑にしている。この
面とり部21d,22dは、円弧面の外、角部を落とす傾斜面
によってもよい。
The annular cutouts 21b and 22b of the drive members 21 and 22 are shown in an enlarged view in FIG. FIG. 2 shows a state in which the driving body 20 rotates at a high speed and is not excited. The bottom surfaces of the cutouts 21b and 22b are inclined surfaces 21 whose inner end surfaces 21a and 22a have a small diameter (outer diameter A).
It is formed on c and 22c. A relief portion 23 having a wide width c due to a space formed by the notches 21b and 22b and the inner circumferential portion of the coupling ring 6.
The magnetic particles 10 are accommodated by the centrifugal action when the driving body 20 is not excited by high-speed rotation. Corners between the outer circumferential portion (outer diameter A) of the inner end surfaces of the drive members 21 and 22 and the inclined surfaces 21c and 22c are rounded by chamfered portions 21d and 22d formed by arcuate surfaces, and accommodated in the escape portion 23. This facilitates the magnetic attraction movement of the magnetic particles in the state to the air gaps g 1 and g 2 by the excitation. The chamfered portions 21d and 22d may be sloped surfaces that drop the corners in addition to the arcuate surfaces.

内端面21a,22aの外径Aは、被駆動体9の外径Bより小
さくし、磁性粒子10の逃し込み部23からエアギャップg
,gへの移動が容易になるようにしている。
The outer diameter A of the inner end surfaces 21a and 22a is made smaller than the outer diameter B of the driven body 9 so that the air gap g from the escape portion 23 of the magnetic particles 10 is reduced.
It is made easy to move to 1 and g 2 .

次に、上記一実施例の装置の動作を説明する。なお、励
磁による連結作用は上記従来装置と同様であり、従来の
問題点となっていた高速回転時の作用を説明する。
Next, the operation of the apparatus of the above-described embodiment will be described. The coupling action by excitation is similar to that of the above-mentioned conventional device, and the action at the time of high-speed rotation, which has been a problem of the conventional device, will be described.

駆動源により駆動体20が高速回転され無励磁であると、
第2図の状態になる。磁性粒子10は遠心力により放射状
に移動し、十分大きい空所の逃し込み部23に分布し収容
される。高速回転が長時間続いても、逃し込み部23の大
きい収容容積により、磁性粒子10群は固化状態になるこ
とがない。こうして、従来のような、機械的損失を超え
た連結力が生じることがない。この逃し込み部23には、
エアギャップg,g部に全面分布するに十分な量の
磁性粒子10が収容される。
When the drive body 20 is rotated at high speed by the drive source and is not excited,
The state shown in FIG. 2 is obtained. The magnetic particles 10 move radially due to centrifugal force, and are distributed and accommodated in the escape portion 23 in a sufficiently large space. Even if the high-speed rotation continues for a long time, the magnetic particles 10 group will not be solidified due to the large accommodation volume of the escape portion 23. In this way, a coupling force that exceeds mechanical loss as in the conventional case does not occur. In this escape section 23,
A sufficient amount of magnetic particles 10 are housed in the air gaps g 1 and g 2 to be distributed over the entire surface.

このような高速回転の状態で、励磁すると、逃し込み部
23は軸方向の幅Cが十分広く、磁気抵抗が大きくてここ
を通る磁束が少いので、この空所での磁性粒子10は連結
しなく、十分な量の磁性粒子10を収容していていても支
障はない。
When excited in such a high-speed rotation state, the escape part
In No. 23, the width C in the axial direction is sufficiently wide, the magnetic resistance is large, and the magnetic flux passing therethrough is small, so that the magnetic particles 10 in this void are not connected and contain a sufficient amount of magnetic particles 10. But there is no problem.

こうして、第3図に示すように、励磁により磁束が多く
通っているエアギャップg,gに、磁性粒子10が磁
気吸引で移動されるが、切込み部21b,22bは内端面21
a,22aへ向けて傾斜面21c,22cが形成され、さらに、角
部が面とり部21d,22dで円滑にされており、かつ、被駆
動体9の外径より、内端面21a,22aの外周部(面とり
部)外径が小さいので、逃し込み部23からの磁性粒子10
が整流作用を受けることになって、エアギャップg
へ極めて円滑に吸引流入される。
Thus, as shown in FIG. 3, the magnetic particles 10 are moved by magnetic attraction into the air gaps g 1 and g 2 through which a large amount of magnetic flux passes by excitation, but the cut portions 21b and 22b have inner end surfaces 21a and 21b.
The inclined surfaces 21c and 22c are formed toward a and 22a, and the corners are smoothed by the chamfered portions 21d and 22d, and the inner diameters of the inner end surfaces 21a and 22a are larger than the outer diameter of the driven body 9. Since the outer diameter of the outer peripheral portion (chamfered portion) is small, the magnetic particles 10 from the escape portion 23
Is to be rectified, and the air gap g 1 ,
It is sucked into the g 2 very smoothly.

こうして、第4図に示すように、磁性粒子10は被駆動体
9の両側のエアギャップg,gに全面的に分布され
完全な連結状態になり、トルク伝達をする。これによ
り、高速回転状態においても伝達トルクが低下すること
がない。
Thus, as shown in FIG. 4, the magnetic particles 10 are entirely distributed in the air gaps g 1 and g 2 on both sides of the driven body 9 and are in a completely connected state to transmit torque. As a result, the transmission torque does not decrease even in the high speed rotation state.

なお、駆動部材21,22の環状切欠き部21b,22bが単に矩
形状に形成され、傾斜面21c,22cや面とり部21d,22dが
設けられてない場合、あるいは、傾斜面や面とり部が設
けられているが、被駆動体9の外径より、内端面21a,2
2aの外周部(面とり部)外径が大きい場合は、幅の広い
逃し込み部23により磁性粒子10群は遠心力による固化状
態になることはないが、非常な高速回転の場合、励磁さ
れても磁性粒子10が大きい流入抵抗のためエアギャップ
,g部へ入りきらず、所定の連結力が得られない
不具合がある。
In addition, when the annular notches 21b and 22b of the drive members 21 and 22 are simply formed in a rectangular shape and the inclined surfaces 21c and 22c and the chamfered portions 21d and 22d are not provided, or the inclined surfaces and the chamfered portions are formed. Is provided, but the inner end surfaces 21a, 2a are larger than the outer diameter of the driven body 9.
When the outer diameter of the outer peripheral portion (chamfered portion) of 2a is large, the wide escape portion 23 does not cause the magnetic particles 10 group to be solidified by centrifugal force, but it is excited when rotating at an extremely high speed. However, due to the large inflow resistance of the magnetic particles 10, there is a problem that a predetermined connecting force cannot be obtained because the magnetic particles 10 do not enter the air gaps g 1 and g 2 .

上記第9図に示す従来装置の場合と、環状切欠き部とし
て、単なる矩形状切欠き部で傾斜面を設けない場合と、
この発明の一実施例の装置との伝達トルク測定結果を、
次表に示す。なお、駆動体が200rpmの場合の伝達トルク
を100とした割合を示す。
In the case of the conventional device shown in FIG. 9 and in the case where the annular notch is simply a rectangular notch and the inclined surface is not provided,
The transmission torque measurement result with the device of one embodiment of the present invention,
It is shown in the following table. It should be noted that the ratio of the transmission torque when the driving body is 200 rpm is 100 is shown.

第5図はこの考案の第2の実施例による駆動体の駆動部
材の逃し込み部の拡大断面図で、高速回転無励磁状態を
示す。駆動体20の双方の駆動部材31,32の内端面31a,3
2aの外周部には軸方向及び半径方向に切込んだ環状切欠
き部31b,32bが設けられ、奥面から内端面31a,32aにか
けた底面部を、傾斜状面として円弧面31c,32cに形成し
てなだらかに連結させている。両切欠き部31b,32b間に
形成された逃し込み部23に、磁性粒子10が遠心力により
移動し収容されている。
FIG. 5 is an enlarged sectional view of a relief portion of a driving member of a driving body according to a second embodiment of the present invention, showing a high speed rotation non-excitation state. Inner end surfaces 31a, 3 of both drive members 31, 32 of the drive body 20
The outer peripheral portion of 2a is provided with annular notch portions 31b and 32b which are cut in the axial direction and the radial direction, and the bottom surface portion extending from the inner surface to the inner end surfaces 31a and 32a is formed as an inclined surface on the circular arc surfaces 31c and 32c. It is formed and connected smoothly. The magnetic particles 10 are moved and accommodated in the escape portion 23 formed between the notches 31b and 32b by centrifugal force.

この状態から励磁すると、第6図に示すように、磁性粒
子10は円滑にエアギャップg,g部に磁気吸引流入
され連結状態となる。
When excited from this state, as shown in FIG. 6, the magnetic particles 10 are smoothly magnetically attracted and flowed into the air gaps g 1 and g 2 to be in a connected state.

第7図(a),(b)はこの発明の第3の実施例を示し、駆動
体20の一方に駆動部材41には、内端面41aの外周部に、
円周方向に複数箇所に断続した環状切欠き部41bが設
けられ、底面部には内端面41a側を小径にした傾斜面41c
が形成され、角部には円弧面の面とり部41dが設けられ
ている。なお、対向する他方の駆動部材(図示は略す)
にも、同様の切欠き部を設ける。
FIGS. 7 (a) and 7 (b) show a third embodiment of the present invention. One of the driving bodies 20 has a driving member 41 on the outer peripheral portion of the inner end surface 41a.
An annular cutout portion 41b is provided intermittently at a plurality of positions in the circumferential direction, and a bottom surface portion has an inclined surface 41c having a smaller diameter on the inner end surface 41a side.
Is formed, and a chamfered portion 41d having an arc surface is provided at the corner. The other drive member (not shown) that faces the other drive member
Also, a similar notch is provided.

第8図はこの発明の第4の実施例を示す。駆動体20の駆
動部材51,52には、内端面51a,52aの外周部に、内端面
51a,52a側を小径とした急な傾斜面51c,52cを形成した
環状切欠き部51b,52bが設けられ、双方間で逃し込み部
23をなしている。傾斜面51c,52cは傾斜が急であり、内
端面51a,52aとの角部は大きい鈍角であるので、面とり
を要しない。しかし、この角部を、さらに面とりしても
よい。
FIG. 8 shows a fourth embodiment of the present invention. The drive members 51, 52 of the drive body 20 include the inner end faces 51a, 52a on the outer periphery thereof.
Annular cutouts 51b and 52b, which are formed with steep slopes 51c and 52c with a small diameter on the 51a and 52a side, are provided, and a relief portion is provided between them.
I am 23. Since the inclined surfaces 51c and 52c are steeply inclined and the corners with the inner end surfaces 51a and 52a are large obtuse angles, chamfering is not required. However, this corner may be further chamfered.

なお、上記実施例では固定枠1を設け励磁コイル2を内
蔵したが、被駆動体を厚肉とし励磁コイルを内蔵するよ
うにしてもよい。この場合は、被駆動軸側にスリップリ
ングを設けて給電するようにする。また、この場合は、
駆動体の双方の駆動部材を外周部で双方を結合して外周
側の磁路とし、固定枠を省くこともできる。
Although the fixed frame 1 is provided and the exciting coil 2 is incorporated in the above-described embodiment, the driven body may be made thick and the exciting coil may be incorporated. In this case, a slip ring is provided on the driven shaft side to supply power. Also, in this case,
It is also possible to omit the fixing frame by connecting both driving members of the driving body at the outer peripheral portion to form a magnetic path on the outer peripheral side.

また,双方の駆動部材を半径方向に厚くし、双方間に励
磁コイルを収容し、固定枠を省いてもよい。この場合は
駆動部材にスリップリングを設ける。
Further, both drive members may be thickened in the radial direction, the exciting coil may be housed between them, and the fixing frame may be omitted. In this case, the drive member is provided with a slip ring.

さらに、被駆動体9は伝達軸8と別個のものにしたが、
一体のものにして被駆動体としてもよく、被駆動体の構
成形状は上記実施例の外、必要により変形したものであ
ってもよい。
Furthermore, although the driven body 9 is separate from the transmission shaft 8,
The driven body may be integrally formed, and the driven body may have a constitutional shape other than that of the above embodiment, which may be modified if necessary.

なおまた、上記実施例では、駆動体20は一対の駆動部材
21、22により構成した場合を示したが、複数対の駆動部
材により構成した場合にも適用できるものである。
Furthermore, in the above embodiment, the driving body 20 is a pair of driving members.
Although the case where it is configured by 21 and 22 is shown, it is also applicable to the case where it is configured by a plurality of pairs of driving members.

〔発明の効果〕〔The invention's effect〕

以上のように、この発明によれば、駆動体の両駆動部材
の軸方向に対向する両内端面の外周部に、それぞれ軸方
向及び半径方向に切欠いだ環状切欠き部を設け、これら
双方間に磁性粒子の逃し込み部を形成し、かつ、切欠き
部底面部を内端面側を小径にした傾斜状面に形成し、さ
らに、被駆動体の外径より上記内端面の外周部の外径を
小さくしたので、高速回転で無励磁時の場合、連結力を
生じることがなく、高速回転で励磁時には低速回転時と
同様に所定の連結力が得られる。
As described above, according to the present invention, annular notch portions that are notched in the axial direction and the radial direction are provided on the outer peripheral portions of both inner end surfaces of the drive member that face each other in the axial direction. A magnetic particle escape portion is formed in between, and the bottom surface portion of the cutout portion is formed into an inclined surface having a smaller diameter on the inner end surface side, and further, the outer peripheral portion of the inner end surface from the outer diameter of the driven body. Since the outer diameter is made small, no coupling force is generated in the case of non-excitation at high speed rotation, and a predetermined coupling force is obtained in the case of excitation at high speed rotation as in the case of low speed rotation.

また、高速回転で励磁状態から励磁を遮断すると、磁性
粒子は逃し込み部へ急速に収容され連結力の切れが良好
になる。
Further, when the excitation is shut off from the excited state at a high speed, the magnetic particles are rapidly accommodated in the escape portion, and the disconnection of the coupling force becomes good.

さらに、磁性流子が逃し込み部からエアギャップ部へ磁
気吸引流入する際、抵抗が少なく円滑に移動され、磁性
粒子が圧迫により破損することが極めて少なくなり、寿
命が延長されるなどの効果がある。
Further, when the magnetic flux flows into the air gap portion from the escape portion by magnetic attraction, it moves smoothly with less resistance, magnetic particles are less likely to be damaged by pressure, and the life is extended. is there.

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

第1図はこの発明による磁性粒子式電磁連結装置の縦断
面図、第2図ないし第4図は第1図の両駆動部材の対向
内端面部環状切欠き部の高速回転での無励磁から励磁状
態を動作順に示す拡大断面図、第5図及び第6図はこの
発明の第2実施例を動作順に示す両駆動部材の対向内端
面部環状切欠き部の拡大断面図、第7図及び第8図はこ
の発明の第3の実施例を示す一方の駆動部材の内端面部
環状切欠き部の断面図及び正面図、第8図はこの発明の
第4の実施例を示す両駆動部材の対向内端面部の環状切
欠き部の拡大断面図、第9図は従来の電磁連結装置の縦
断面図、第10図及び第11図は第9図の両駆動部材の
対向内端面部の高速回転での無励磁及び励磁状態を示す
拡大断面図である。 2…励磁コイル、9…被駆動体、9a,9b…側面、10…磁
性粒子、20…駆動体、21,22,31,32,41,51,52…駆
動部材、21a,22a,31a,32a,41a,51a,52a…内端
面、21b,22b,31b,32b,41b,51b,52b…環状切欠き
部、21c,22c,41c,51c,52c…傾斜面、21d,22d,41d
…面とり部、23…逃し込み部、31c,32c…円弧状傾斜
面、g,g…エアギャップ なお、図中同一符号は同一又は相当部分を示す。
FIG. 1 is a vertical cross-sectional view of a magnetic particle type electromagnetic coupling device according to the present invention, and FIGS. 2 to 4 are views from non-excitation at a high speed rotation of opposing inner end face annular notches of both drive members of FIG. FIG. 5 and FIG. 6 are enlarged cross-sectional views showing the excitation state in the order of operation, FIG. 5 and FIG. FIG. 8 is a sectional view and a front view of an inner end face annular cutout portion of one drive member showing a third embodiment of the present invention, and FIG. 8 is a drive member showing a fourth embodiment of the present invention. FIG. 9 is an enlarged sectional view of an annular cutout portion of the opposing inner end surface portion, FIG. 9 is a longitudinal sectional view of a conventional electromagnetic coupling device, and FIGS. 10 and 11 are opposing inner end surface portions of both drive members of FIG. It is an expanded sectional view which shows a non-excitation and an excitation state in high speed rotation. 2 ... Excitation coil, 9 ... Driven body, 9a, 9b ... Side surface, 10 ... Magnetic particle, 20 ... Drive body, 21, 22, 31, 32, 41, 51, 52 ... Drive member, 21a, 22a, 31a, 32a, 41a, 51a, 52a ... Inner end surface, 21b, 22b, 31b, 32b, 41b, 51b, 52b ... Annular notch, 21c, 22c, 41c, 51c, 52c ... Inclined surface, 21d, 22d, 41d
... chamfered portion, 23 ... relief addition unit, 31c, 32c ... arcuate inclined surfaces, g 1, g 2 ... air gap should be noted that the same reference characters denote the same or corresponding parts.

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】双方の内端面を軸方向に間隔をあけ対向さ
せて結合した少なくとも一対の駆動部材により構成され
た駆動体と、円板体を有し、上記駆動体の双方の駆動部
材の内端面間にそれぞれ軸方向のエアギャップをあけ、
かつ、外円周側に空所をあけ配置された被駆動体と、上
記双方のエアギャップ部に充てんされる磁性粒子と、通
電されて磁束を発生し、上記駆動部材から上記両エアギ
ャップを介し上記駆動体を経る磁路に通し、上記磁性粒
子を磁化するための励磁コイルとを備えた電磁連結装置
において、上記双方の駆動部材の対向する各内端面の外
周部にそれぞれ環状切欠き部を形成し、この環状切欠き
部の底面部を内端面側が小形になる傾斜状面に形成し、
かつ、この傾斜状面と上記内端面との角部の外径を上記
被駆動体の外径より小さくしたことを特徴とする磁性粒
子式電磁連結装置。
1. A drive body composed of at least a pair of drive members in which both inner end faces are opposed to each other with an interval in the axial direction and are joined together, and a disk body, and both drive members of the drive bodies are provided. Open an air gap in the axial direction between the inner end faces,
And, a driven body which is arranged with an open space on the outer circumferential side, magnetic particles filled in the air gap portions of both of the above, and a magnetic flux is generated by being energized, and the both air gaps from the driving member are generated. In an electromagnetic coupling device including an exciting coil for magnetizing the magnetic particles, which is passed through a magnetic path passing through the driving body via an annular cutout portion on the outer peripheral portion of each inner end surface of the both driving members facing each other. To form a bottom surface portion of the annular notch portion into an inclined surface where the inner end surface side is small,
The magnetic particle type electromagnetic coupling device is characterized in that an outer diameter of a corner portion between the inclined surface and the inner end surface is smaller than an outer diameter of the driven body.
【請求項2】環状切欠き部の傾斜状面は、傾斜面に形成
され、この傾斜面と内端面との角部を面とりした特許請
求の範囲第1項記載の磁性粒子式電磁連結装置。
2. The magnetic particle type electromagnetic coupling device according to claim 1, wherein the inclined surface of the annular notch portion is formed as an inclined surface, and a corner between the inclined surface and the inner end surface is chamfered. .
【請求項3】環状切欠き部の傾斜状面は、円弧面により
形成された特許請求の範囲第1項記載の磁性粒子式電磁
連結装置。
3. The magnetic particle type electromagnetic coupling device according to claim 1, wherein the inclined surface of the annular notch is formed by an arc surface.
【請求項4】環状切欠き部の傾斜状面は、内端面への急
な傾斜面により形成された特許請求の範囲第1項記載の
磁性粒子式電磁連結装置。
4. The magnetic particle type electromagnetic coupling device according to claim 1, wherein the inclined surface of the annular notch is formed by a steep inclined surface toward the inner end surface.
【請求項5】環状切欠き部は、円周方向に断続して形成
された特許請求の範囲第1項ないし第4項のいずれかに
記載の磁性粒子式電磁連結装置。
5. The magnetic particle type electromagnetic coupling device according to any one of claims 1 to 4, wherein the annular notch is formed so as to be interrupted in a circumferential direction.
JP27703886A 1986-11-19 1986-11-19 Magnetic particle type electromagnetic coupling device Expired - Lifetime JPH063232B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP27703886A JPH063232B2 (en) 1986-11-19 1986-11-19 Magnetic particle type electromagnetic coupling device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP27703886A JPH063232B2 (en) 1986-11-19 1986-11-19 Magnetic particle type electromagnetic coupling device

Publications (2)

Publication Number Publication Date
JPS63130931A JPS63130931A (en) 1988-06-03
JPH063232B2 true JPH063232B2 (en) 1994-01-12

Family

ID=17577913

Family Applications (1)

Application Number Title Priority Date Filing Date
JP27703886A Expired - Lifetime JPH063232B2 (en) 1986-11-19 1986-11-19 Magnetic particle type electromagnetic coupling device

Country Status (1)

Country Link
JP (1) JPH063232B2 (en)

Also Published As

Publication number Publication date
JPS63130931A (en) 1988-06-03

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