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JPS645168B2 - - Google Patents
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JPS645168B2 - - Google Patents

Info

Publication number
JPS645168B2
JPS645168B2 JP21551983A JP21551983A JPS645168B2 JP S645168 B2 JPS645168 B2 JP S645168B2 JP 21551983 A JP21551983 A JP 21551983A JP 21551983 A JP21551983 A JP 21551983A JP S645168 B2 JPS645168 B2 JP S645168B2
Authority
JP
Japan
Prior art keywords
magnetic
rotating body
gap
circumferential surface
yoke
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
Application number
JP21551983A
Other languages
Japanese (ja)
Other versions
JPS60109623A (en
Inventor
Michiru Sakamoto
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.)
Shinko Electric Co Ltd
Original Assignee
Shinko Electric 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 Shinko Electric Co Ltd filed Critical Shinko Electric Co Ltd
Priority to JP21551983A priority Critical patent/JPS60109623A/en
Publication of JPS60109623A publication Critical patent/JPS60109623A/en
Publication of JPS645168B2 publication Critical patent/JPS645168B2/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)
  • Braking Arrangements (AREA)

Description

【発明の詳細な説明】 本発明は一対の回転体、または回転体と固定体
で構成された空隙に磁性粉体を封入し、これを磁
化させることによつて生じる粉体の剪断抵抗を利
用してトルクの伝達、または制動作用を行わせる
形の磁気連結装置に関するものである。
Detailed Description of the Invention The present invention utilizes the shear resistance of the powder generated by enclosing magnetic powder in a gap formed by a pair of rotating bodies or a rotating body and a fixed body and magnetizing the powder. The present invention relates to a magnetic coupling device that transmits torque or performs a braking action.

この種連結装置は摩擦形のデイスククラツチ、
またはブレーキに比し耐スリツプ特性を有する点
で優れているが同一外径寸法におけるトルク容量
は約1/3〜1/4であり、同一トルクに対して寸法的
に大形となる。
This type of coupling device is a friction type disc clutch,
Although it is superior to brakes in that it has anti-slip characteristics, its torque capacity at the same outer diameter is about 1/3 to 1/4, making it dimensionally larger for the same torque.

本発明は小形で高トルクを発生させることので
きるこの種磁気連結装置を提供することを目的と
する。
SUMMARY OF THE INVENTION An object of the present invention is to provide a magnetic coupling device of this type that is compact and capable of generating high torque.

まずこの種装置として一般的に知られているも
のを第1図について説明する。同図において1は
コイル2を収容するヨークで左右のブラケツト
3,4で支持される。5は右方側壁部により回転
軸6に連なる外方回転体で円筒状部7を有し、こ
の部分は中央部に介在せられた非磁性遮断リング
8により左右に磁気的に分割される。回転軸6は
軸受9を介して右方ブラケツト4で支持される。
10は外方回転体5に囲まれた内方回転体で外周
面と上記回転体5の円筒状部7の内周面との間に
空隙が存在し、この空隙内に磁性粉体11が封入
される。図示する装置はブレーキとして使用され
る場合を示すもので上記内方回転体10は制動体
としての機能を発揮させるため左方ブラケツト3
に一体的に結合され、そしてこのブラケツトを当
該ブレーキの使用機械の適所に固定することによ
り、運転中回転しないようになつている。またこ
の場合回転軸6は被制動軸となり、図示しない被
制動体に連結される。
First, a generally known device of this type will be explained with reference to FIG. In the figure, 1 is a yoke that accommodates a coil 2 and is supported by left and right brackets 3 and 4. Reference numeral 5 denotes an outer rotary body connected to the rotating shaft 6 by a right side wall portion, and has a cylindrical portion 7, and this portion is magnetically divided into left and right sides by a non-magnetic blocking ring 8 interposed in the center. The rotating shaft 6 is supported by the right bracket 4 via a bearing 9.
Reference numeral 10 denotes an inner rotating body surrounded by an outer rotating body 5, and there is a gap between the outer peripheral surface and the inner circumferential surface of the cylindrical part 7 of the rotating body 5, and the magnetic powder 11 is inside this gap. Enclosed. The illustrated device is used as a brake, and the inner rotating body 10 is attached to the left bracket 3 in order to function as a braking body.
The bracket is integrally connected to the brake and is secured in place on the machine in which the brake is used so that it does not rotate during operation. Further, in this case, the rotating shaft 6 becomes a braked shaft and is connected to a braked body (not shown).

従来の連結装置はこのように構成され、コイル
2に電流が供給されると、同図に破線で磁路を示
す磁束を生じ、磁性粉体11の粒子間並びにこの
粉体と、これを収容する空隙を構成する周壁間に
磁気吸引力を生じ、これにより磁性粉体粒子間に
剪断抵抗を生じ内方回転体10、従つてこれと一
体の回転軸6に連結された被制動体に制動がかけ
られる。
The conventional coupling device is constructed as described above, and when a current is supplied to the coil 2, a magnetic flux is generated, which is shown by the broken line in the figure, and the magnetic flux flows between the particles of the magnetic powder 11 as well as between the powder and the magnetic powder contained therein. A magnetic attraction force is generated between the circumferential walls constituting the gap, which causes shear resistance between the magnetic powder particles and applies braking to the inner rotating body 10 and, therefore, to the braked body connected to the rotating shaft 6 integral therewith. is applied.

このような従来の連結装置では内方回転体10
の磁性粉体11に対する接触面は、その回転体の
外周面のみであるため磁性粉体11の磁化時にお
ける回転体10に対する拘束力、従つて小さい制
動力しか発揮できない。
In such a conventional coupling device, the inner rotating body 10
Since the contact surface with the magnetic powder 11 is only the outer peripheral surface of the rotating body, only a restraining force on the rotating body 10 when the magnetic powder 11 is magnetized, and hence only a small braking force can be exerted.

これに鑑み本発明は一方の回転体に相当する部
材の内、外両周面に磁気結合力を生ぜしめる構成
とすることによつて制動力、またはクラツチとし
て使用する場合のトルク容量を倍増させるもので
以下本発明をブレーキに実施した場合の実施例を
第2図について説明する。同図において12はコ
イル13を収容するヨークで内周部には、その両
側から夫々中央に向つて延びる磁極部14,1
4′を有することは上記従来のヨークの構成と同
一であるがこの実施例では両磁極部の先端に亘つ
て非磁性の遮断リング15を接合し、このリング
と両磁極部の内周面で後述す磁性粉体を封入する
ための空隙の一方の壁面を構成する。16,17
は夫々非磁性材から成る左右のブラケツトで周縁
部においてヨーク12の両端を支持しており、な
お一方のブラケツトは当該ブレーキの使用機械の
適所に固定され、ヨーク部分と共に運転中回転し
ないようになつている。18は断面T字状の回転
体で円盤状部のボス部において回転軸19と一体
となり、円筒状部の中央部は永久磁石リング20
で形成され、かつ同筒状部の外周面と上記磁極部
14,14′の内周面間には空隙が構成され、こ
の空隙内に磁性粉体21が充填される。回転軸1
9は軸受22,22′を介して各ブラケツト16,
17によつて支持される。なお上記において永久
磁石リング20は回転体18の円筒状部の中央部
のみに介在させるだけでもよいが円盤状部の一部
にかけて設けてもよい。23,23′はブラケツ
ト16,17の内側に固着された環状の磁極体で
各外周面と回転体18の円筒状部の内周面との間
に空隙を構成し、こ空隙内に磁性粉体24が封入
される。25,25′および26,26′はシール
でシール25,25′は磁極体22と22′の内側
面の凹所に挿入され、回転体18の円盤状部に軽
く接触し、またシール26,26′は磁極体22
と22′の内周面の凹部にはめ込まれ、回転軸1
9の突出部に対接し、上記シール25,25′と
ともに磁性粉体24の流出を防止している。
In view of this, the present invention doubles the braking force or torque capacity when used as a clutch by creating a magnetic coupling force on both the inner and outer peripheral surfaces of a member corresponding to one rotating body. An embodiment in which the present invention is applied to a brake will be described below with reference to FIG. In the figure, reference numeral 12 denotes a yoke that accommodates the coil 13, and magnetic pole portions 14, 1 are provided on the inner circumference of the yoke, each extending toward the center from both sides of the yoke.
4' is the same as the structure of the conventional yoke described above, but in this embodiment, a non-magnetic cutoff ring 15 is joined across the tips of both magnetic pole parts, and this ring and the inner peripheral surface of both magnetic pole parts are joined. It constitutes one wall surface of a gap for enclosing magnetic powder, which will be described later. 16,17
The left and right brackets are made of non-magnetic material and support both ends of the yoke 12 at their peripheral edges, and one of the brackets is fixed in place on the machine in which the brake is used, so that it does not rotate together with the yoke portion during operation. ing. Reference numeral 18 denotes a rotating body having a T-shaped cross section, which is integrated with the rotating shaft 19 at the boss portion of the disk-shaped portion, and a permanent magnet ring 20 in the center of the cylindrical portion.
A gap is formed between the outer circumferential surface of the cylindrical portion and the inner circumferential surface of the magnetic pole portions 14, 14', and the magnetic powder 21 is filled in this gap. Rotating axis 1
9 connects each bracket 16, via bearings 22, 22'.
Supported by 17. In the above description, the permanent magnet ring 20 may be interposed only in the center of the cylindrical portion of the rotating body 18, but it may also be provided over a part of the disc-shaped portion. Reference numerals 23 and 23' denote annular magnetic pole bodies fixed to the insides of the brackets 16 and 17, forming a gap between each outer peripheral surface and the inner peripheral surface of the cylindrical part of the rotating body 18, and magnetic powder is placed in this gap. A body 24 is enclosed. 25, 25' and 26, 26' are seals, and the seals 25, 25' are inserted into recesses on the inner surfaces of the magnetic pole bodies 22 and 22', and lightly contact the disc-shaped portion of the rotating body 18. 26' is the magnetic pole body 22
and 22' into the recesses on the inner circumferential surface of the rotary shaft 1.
9 and prevents the magnetic powder 24 from flowing out together with the seals 25 and 25'.

本発明の実施例は以上で構成され、コイル13
に給電が行われると破線で示す磁路に磁束が流
れ、回転体18の円筒状部の内、外面周面上の空
隙内に封入された各磁性粉体24,21が磁化さ
れ、これ等磁性粉体の粒子間に働らく剪断抵抗に
より回転体18の回転は拘束され、従つてこの回
転体に回転軸19を介して連らなる図示しない被
制動体に制動がかけられる。
The embodiment of the present invention is configured as described above, and the coil 13
When power is supplied, a magnetic flux flows in the magnetic path shown by the broken line, and the magnetic powders 24 and 21 sealed in the gap on the inner and outer circumferential surface of the cylindrical part of the rotating body 18 are magnetized. The rotation of the rotating body 18 is restrained by the shear resistance acting between the particles of the magnetic powder, and therefore, a brake is applied to a braked body (not shown) connected to the rotating body via the rotating shaft 19.

この時、永久磁石リング20はその極性が、コ
イルによる磁束の流れる方向に対し、逆対する如
く帯磁させて置けばT字状断面を有する回転体の
円筒部における磁束は円盤状部周辺近くでは永久
磁石リング20により遮断されるため矢印で示す
ように磁性粉体24、磁極体23,23′、およ
び回転体18の円盤状部の中心寄りの部分を通過
するように流れ、所定の拘束力を発生する。
At this time, if the permanent magnet ring 20 is magnetized so that its polarity is opposite to the direction in which the magnetic flux flows from the coil, the magnetic flux in the cylindrical part of the rotating body having a T-shaped cross section will be permanent near the periphery of the disc-shaped part. Because it is blocked by the magnet ring 20, the flow passes through the magnetic powder 24, the magnetic pole bodies 23, 23', and the center portion of the disc-shaped portion of the rotating body 18, as shown by the arrow, and exerts a predetermined restraining force. Occur.

また、コイル13に対する給電を電流の方向を
切換え、コイルによつて発生する磁束の方向を図
示と逆向きにすると、その磁束は図中一点鎖線で
示した永久磁石による磁束と同方向となり、この
とき回転体18の円筒状部の断面が十分大でコイ
ルによつて発生する磁束の殆んど全てがリング2
0の部分を通過しうるよう設計されておればコイ
ルによる磁束は磁性粉体24、磁極体23,2
3′、および回転体18の円盤状部の中心寄りの
部分で構成する磁気回路、つまり空隙が介在する
レラクタンスの大きい磁気回路中を流通する磁束
は殆んどなく微小で磁性粉体24による拘束力は
微弱でこのときの拘束力は磁性粉体21のみが発
生することとなる。
In addition, if the direction of the current is switched to feed the coil 13 and the direction of the magnetic flux generated by the coil is reversed to that shown in the figure, the magnetic flux will be in the same direction as the magnetic flux caused by the permanent magnet shown by the dashed line in the figure. When the cross section of the cylindrical part of the rotating body 18 is sufficiently large, almost all of the magnetic flux generated by the coil is transferred to the ring 2.
If the design is such that it can pass through the 0 part, the magnetic flux from the coil will flow through the magnetic powder 24, the magnetic pole bodies 23, 2
3', and the magnetic circuit formed by the central part of the disc-shaped part of the rotating body 18, that is, the magnetic circuit with a large reluctance with an intervening air gap. The force is weak, and the binding force at this time is generated only by the magnetic powder 21.

而してコイルに対する両通電状態を比較すると
前者では回転体18の円筒状部左右の内、外周に
当る作動空隙の4箇所、後者では同円筒状部左右
の外周に当る作動空隙の2箇所となり発生トルク
は前者に較べ後者は1/2となる。
Comparing the two energization states to the coil, in the former there are four working gaps on the left and right outer peripheries of the cylindrical part of the rotating body 18, and in the latter there are two working gaps on the left and right outer peripheries of the cylindrical part. The generated torque is 1/2 in the latter compared to the former.

実施例はブレーキの場合について説明したがク
ラツチとして使用する場合、ヨーク側を固定する
ことなく、このヨーク側を例えば被動側に連結す
ると同時に他方の回転側である回転軸19を駆動
側に連結することにより、コイル13に対し電流
を供給し、或は給電を断つとき、動力の伝達が行
われ或は遮断されることはいうまでもない。
The embodiment has been described in the case of a brake, but when used as a clutch, the yoke side is not fixed, and the yoke side is connected to the driven side, for example, and at the same time, the rotating shaft 19, which is the other rotating side, is connected to the driving side. Therefore, it goes without saying that when supplying current to the coil 13 or cutting off the power supply, power transmission is performed or interrupted.

本発明は上記のように回転体18を断面T字状
に形成し、その両翼である左右の円筒状を永久磁
石のリングで相互に磁気的に分割するとともにそ
の回転体の円盤状部の両側に磁極体を夫々設け、
この磁極体の外周面と回転体の円筒状部の内周面
との間に空隙を構成し、この空隙に磁性粉体を封
入すると同時に同回転体の円筒状部の外周面とヨ
ークに連らなる磁極部との間に構成した空隙内に
も磁性粉体を封入させるようにしたもので磁性粉
体が磁化されたときに回転体18に対して拘束力
を発生する作動間隙は、その回転体の円筒状部の
内、外両周面上の2ケ所となり、回転体の円筒状
部の内、外周の両面に磁気結合力を生じることと
なり、従来の第1図に示す外方回転体の内周面の
1ケ所のみに磁器結合力を生じるものに比し、そ
の空隙を構成する周壁の平均径、および磁化に伴
なう剪断抵抗、空隙巾を同一とするとき2倍の拘
束力、従つて制動力乃至トルク容量を持たせるこ
とができ小形で容量の大きい磁気連結装置の提供
することができ、さらにコイルの励磁の方向を反
転させることにより、発生トルクを半分にするこ
とができ、従つて電流の調整範囲は2倍となり、
トルク調整範囲が倍化されると同時に電流調節装
置の調整範囲は小さくてすみ制御装置の小形、簡
素化が容易となる。
In the present invention, as described above, the rotating body 18 is formed to have a T-shaped cross section, and the left and right cylindrical wings, which are the left and right cylindrical wings, are magnetically divided by a ring of permanent magnets, and both sides of the disc-shaped part of the rotating body are A magnetic pole body is provided respectively in the
A gap is formed between the outer circumferential surface of the magnetic pole body and the inner circumferential surface of the cylindrical portion of the rotating body, and magnetic powder is sealed in this gap, and at the same time, the outer circumferential surface of the cylindrical portion of the rotating body is connected to the yoke. The working gap that generates a restraining force on the rotating body 18 when the magnetic powder is magnetized is the There are two locations on the inner and outer circumferential surfaces of the cylindrical part of the rotating body, and magnetic coupling forces are generated on both the inner and outer circumferential surfaces of the cylindrical part of the rotating body, thereby preventing the conventional outward rotation shown in Fig. 1. Compared to the case where magnetic bonding force is generated only at one place on the inner circumferential surface of the body, the constraint is twice as strong when the average diameter of the peripheral wall that makes up the gap, the shear resistance due to magnetization, and the gap width are the same. It is possible to provide a small magnetic coupling device with a large capacity, which can have a braking force or torque capacity, and furthermore, by reversing the direction of excitation of the coil, the generated torque can be halved. Therefore, the current adjustment range is doubled,
At the same time, the torque adjustment range is doubled, and at the same time, the adjustment range of the current adjustment device can be reduced, making it easier to downsize and simplify the control device.

更に回転体が断面T字状に形成されることか
ら、この回転体の円筒状部は中央部において円盤
状部で支持されることとなり、即ち回転体の円筒
状部は支持部に対して寸法的に左右に等分に振り
分けられることとなり、この円筒状部は支持部に
対して全巾に亘つて真円度と同心度を維持され易
く、従つて精度上、その回転体の機械加工が容易
であると同時に、その加工費を低減させることが
でき、なおこの種電磁連結装置はスリツプ状態で
の使用が可能である反面磁性粉体を封入する作動
空隙部に生じる発生熱量は大きく、殊に本願発明
による装置のように発生トルクの大なるものでは
一層発生熱量が増大することとなるがこの発生熱
の放散に対する熱流経路は各部の構成は左右対称
のため両側ブラケツトにほゞ均等に2分されるの
で熱放散能力の面でも有利である。
Furthermore, since the rotating body is formed with a T-shaped cross section, the cylindrical part of the rotating body is supported by the disk-shaped part at the center, that is, the cylindrical part of the rotating body has a dimension smaller than that of the supporting part. This means that the cylindrical part is distributed equally to the left and right sides, and the roundness and concentricity of this cylindrical part are easily maintained over the entire width with respect to the support part. This type of electromagnetic coupling device is easy to use and can reduce processing costs.Although this type of electromagnetic coupling device can be used in a slip state, on the other hand, the amount of heat generated in the operating gap that encloses the magnetic powder is large, making it particularly difficult to use. If the generated torque is large, such as the device according to the present invention, the amount of generated heat will further increase, but the heat flow path for the dissipation of this generated heat is distributed almost equally on both sides of the bracket because the configuration of each part is symmetrical. It is also advantageous in terms of heat dissipation ability.

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

第1図は従来の磁気連結装置の上半部を断面と
した正面図、第2図は本発明の実施例を示すもの
で上半部を断面とした正面図である。 12……ヨーク、14,14′……磁極部、1
5……非磁性遮断リング、18……回転体、19
……回転軸、20……永久磁石リング、21,2
4……磁性粉体、23,23′……磁極体。
FIG. 1 is a front view with the upper half of a conventional magnetic coupling device in cross section, and FIG. 2 is a front view of an embodiment of the present invention with the upper half in cross section. 12... Yoke, 14, 14'... Magnetic pole part, 1
5...Nonmagnetic blocking ring, 18...Rotating body, 19
... Rotating shaft, 20 ... Permanent magnet ring, 21,2
4...Magnetic powder, 23, 23'...Magnetic pole body.

Claims (1)

【特許請求の範囲】[Claims] 1 中央に位置する非磁性遮断リングを挾んで先
端部を突合せた一対の円筒状磁極部を有するヨー
ク、断面T字で円筒状部を、その中央部に介在さ
せた永久磁石リングで左右に磁気的に分離され、
かつ同円筒状部の外周と上記磁極部間に磁性粉体
封入用空隙を構成するとともに円盤状部において
被制動軸或は入、出力回転軸等の回転軸に機械的
に連結された回転体、および上記回転体の円盤状
部の左右に位置するとともに上記ヨークを支持す
る各ブラケツトに夫々固着され、各外周面と同上
記回転体の円筒状部の内周面との間に磁性粉体封
入用空隙を構成する一対の磁極体を備え、回転体
円筒状部の内、外両周面に又は選択的に外周面の
みに磁気結合力を生ぜしめたことを特徴とする磁
気連結装置。
1 A yoke that has a pair of cylindrical magnetic pole parts with a non-magnetic blocking ring located in the center in between and abutting their tips. separated,
and a rotating body that forms a gap for enclosing magnetic powder between the outer periphery of the cylindrical part and the magnetic pole part, and is mechanically connected to a rotating shaft such as a braked shaft or an input/output rotating shaft in the disc-shaped part. , and magnetic powder is fixed to each bracket located on the left and right sides of the disc-shaped portion of the rotating body and supporting the yoke, and between each outer circumferential surface and the inner circumferential surface of the cylindrical portion of the rotating body. A magnetic coupling device comprising a pair of magnetic pole bodies constituting an enclosing gap, and generating a magnetic coupling force on both the inner and outer circumferential surfaces of a cylindrical portion of a rotating body, or selectively only on the outer circumferential surface.
JP21551983A 1983-11-15 1983-11-15 Magnetic coupling device Granted JPS60109623A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21551983A JPS60109623A (en) 1983-11-15 1983-11-15 Magnetic coupling device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21551983A JPS60109623A (en) 1983-11-15 1983-11-15 Magnetic coupling device

Publications (2)

Publication Number Publication Date
JPS60109623A JPS60109623A (en) 1985-06-15
JPS645168B2 true JPS645168B2 (en) 1989-01-30

Family

ID=16673754

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21551983A Granted JPS60109623A (en) 1983-11-15 1983-11-15 Magnetic coupling device

Country Status (1)

Country Link
JP (1) JPS60109623A (en)

Also Published As

Publication number Publication date
JPS60109623A (en) 1985-06-15

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