JPS5842603B2 - Electromagnet for high speed operation - Google Patents

Electromagnet for high speed operation

Info

Publication number
JPS5842603B2
JPS5842603B2 JP51000367A JP36776A JPS5842603B2 JP S5842603 B2 JPS5842603 B2 JP S5842603B2 JP 51000367 A JP51000367 A JP 51000367A JP 36776 A JP36776 A JP 36776A JP S5842603 B2 JPS5842603 B2 JP S5842603B2
Authority
JP
Japan
Prior art keywords
armature
electromagnet
suction
suction plate
iron core
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
JP51000367A
Other languages
Japanese (ja)
Other versions
JPS5284455A (en
Inventor
恒松 高橋
善八 大信田
亨 田村
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.)
Nippon Telegraph and Telephone Corp
Shinko Seisakusho KK
Original Assignee
Nippon Telegraph and Telephone Corp
Shinko Seisakusho KK
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 Nippon Telegraph and Telephone Corp, Shinko Seisakusho KK filed Critical Nippon Telegraph and Telephone Corp
Priority to JP51000367A priority Critical patent/JPS5842603B2/en
Publication of JPS5284455A publication Critical patent/JPS5284455A/en
Publication of JPS5842603B2 publication Critical patent/JPS5842603B2/en
Expired legal-status Critical Current

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  • Electromagnets (AREA)

Description

【発明の詳細な説明】 本発明は印刷装置用および選択装置用として、並列に高
密度で配置することが可能な、小型にして動作速度が速
く、構成が単純な電磁石に関するも、のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnet of small size, high operating speed, and simple construction, which can be arranged in parallel in high density for use in printing devices and selection devices.

従来、この種の装置は第1図に示すように複雑な構成に
なっているので、部品数量が多く、少ない空間で並列に
多数の電磁石を収容することが困難であり、製造コスト
も高い欠点があった。
Conventionally, this type of device has a complicated structure as shown in Figure 1, so it has a large number of parts, it is difficult to accommodate a large number of electromagnets in parallel in a small space, and the manufacturing cost is high. was there.

次に従来の実施例を第1図により詳細に説明する。Next, a conventional embodiment will be explained in detail with reference to FIG.

第1図において、一般にU字形に曲った継鉄1と、それ
に固定された鉄心2にコイル3が装着され、純鉄材料の
吸引板(接極子)4が保持板5と吸引板4を復旧側に寄
せるための復旧用はね6とで支えられている。
In Fig. 1, a coil 3 is attached to a yoke 1 bent in a generally U-shape and an iron core 2 fixed to it, and a suction plate (armature) 4 made of pure iron restores a retaining plate 5 and a suction plate 4. It is supported by recovery springs 6 to move it to the side.

ばね6は止め金7に引掛け、常に吸引板4を引張ってい
る。
The spring 6 is hooked on the stopper 7 and constantly pulls the suction plate 4.

保持板5は吸引板4の復旧側と励磁側の受は止めであっ
て、磁気抵抗の大きい材料で作られている。
The holding plate 5 serves as a stop for the recovery side and excitation side of the suction plate 4, and is made of a material with high magnetic resistance.

励磁によって吸引板4は鉄心2に吸引され、励磁が解か
れるとばね6の張力で鉄心2より離れるが、残留磁気の
ために吸引板4は鉄心2より離れがたく、復1田こ要す
る時間が長くなり、その変動時間も大きい。
The attraction plate 4 is attracted to the iron core 2 by excitation, and when the excitation is released, it separates from the iron core 2 due to the tension of the spring 6, but due to the residual magnetism, the attraction plate 4 is difficult to separate from the iron core 2, and it takes a long time. becomes longer, and its fluctuation time is also large.

従って磁気回路に小量の磁気抵抗として、吸引状態で吸
引板4と鉄心2の間に0.1間程度の間隙を設けている
が、この間隙により吸引力は低下する。
Therefore, as a small amount of magnetic resistance in the magnetic circuit, a gap of about 0.1 is provided between the suction plate 4 and the iron core 2 in the suction state, but this gap reduces the suction force.

これら構造上の必要条件を満たすには、構成が複雑であ
って吸引板4の質量は小さくできず、高速動作用として
使用するには、コイル3に流す電流を過大にする必要が
あり、消費電力が多く発熱が高いので放熱対策を要し、
多量の電磁石を高密度に収容できず、吸引の際、衝突音
が太きい等、多くの欠点があった。
In order to satisfy these structural requirements, the structure is complicated and the mass of the suction plate 4 cannot be made small.If used for high-speed operation, it is necessary to increase the current flowing through the coil 3, which increases consumption. Since it consumes a lot of electricity and generates a lot of heat, heat dissipation measures are required.
It had many drawbacks, such as not being able to accommodate a large number of electromagnets in a high density, and producing a loud collision sound during suction.

本発明はこれらの欠点を解決するため、継鉄と鉄心が一
体構造で、吸引板をたとえば17−7PH材料の薄板に
し、吸引状態で鉄心と吸引板との間に間隙を与えず、運
動薄囲の規制用受は止めを付けず、吸引板および鉄心を
各々並列に多数個一体化したことを特徴とし、その目的
は高密度に実装することにより、装置の容積を小さくし
、低価格で、供給電力および騒音の小さい高能率な高速
作動用電磁石を提供することにある。
In order to solve these drawbacks, the present invention has an integral structure of the yoke and the iron core, and the suction plate is made of a thin plate made of, for example, 17-7PH material. The regulating receiver for the enclosure is characterized by having a large number of suction plates and iron cores integrated in parallel, without any stoppers.The purpose of this is to reduce the volume of the device by packaging it in high density, and to reduce the cost. The purpose of the present invention is to provide a high-efficiency, high-speed operation electromagnet with low power supply and low noise.

第2図は本発明の一実施例の斜視図であって、第3図、
第4図および第5図はその分解図である。
FIG. 2 is a perspective view of an embodiment of the present invention, and FIG.
4 and 5 are exploded views thereof.

第2図は4個の電磁石を並列に一体化実装した場合を示
す図であって、一体形の鉄心8に熱伝導率の高い材料で
モールドしたコイル9を装着固定し、吸引板(接極子)
10は鉄心8の下部に固定されている。
Fig. 2 shows a case where four electromagnets are integrally mounted in parallel, in which a coil 9 molded with a material with high thermal conductivity is attached and fixed to an integral iron core 8, and an attraction plate (armature )
10 is fixed to the lower part of the iron core 8.

励磁されていない状態における鉄心8と吸引板10の間
隙は吸引板10の必要行程距離より求められた値にする
The gap between the iron core 8 and the suction plate 10 in the non-excited state is determined from the required stroke distance of the suction plate 10.

第3図は吸引板10を示す図で、鉄心8と対応する部分
の幅を広くして磁気回路の抵抗を少なくし、支点部分と
先端部分を狭くし、動作時間の短縮と吸引力増加の効果
を得る形状とし、支点部分は各々連結し、一体形としで
ある。
FIG. 3 shows the suction plate 10. The width of the part corresponding to the iron core 8 is widened to reduce the resistance of the magnetic circuit, and the fulcrum part and tip part are narrowed to shorten the operating time and increase the suction force. The shape is such that the fulcrum parts are connected and integrated.

第4図はコイル9を装着する前の鉄心8を示す図で、本
体より上段、中段、下段と各々の張り出しがあり、これ
にコイル9が装着される。
FIG. 4 is a diagram showing the iron core 8 before the coil 9 is attached thereto. There are upper, middle, and lower protrusions from the main body, and the coil 9 is attached to these.

張り出し部分の長さは中段が下段より短く、上段は中段
より短くして、吸引板10が吸引された時に、たわみ曲
線に合わせ、各鉄心8の張り出し面と吸弓板10が密着
できるようにしである。
The length of the overhanging portion is made such that the middle tier is shorter than the lower tier and the upper tier is shorter than the middle tier, so that when the suction plate 10 is sucked, the overhanging surface of each iron core 8 and the suction plate 10 can come into close contact with each other in accordance with the deflection curve. It is.

第5図は鉄心8にコイル9を装着した図で、装着部のコ
イル9と鉄心8を密着させ、コイル9から発生する熱が
鉄心8の本体からも放熱することができ、またコイル9
は上段と中段および下段の巻線端末を接続し、その上を
モールドし、リード線はモールドの外に2本引き出す。
FIG. 5 shows a coil 9 attached to the iron core 8. The coil 9 at the attachment part and the iron core 8 are brought into close contact with each other, so that the heat generated from the coil 9 can also be radiated from the main body of the iron core 8.
Connect the winding terminals of the upper, middle, and lower stages, mold the upper part, and pull out two lead wires outside the mold.

これを動作するには、コイル9に電流を流して吸引板1
0を鉄心8に引き寄せる。
To operate this, a current is applied to the coil 9 and the suction plate 1
0 to iron core 8.

吸引開始においてコイル9に電流が流れると、吸引板1
0と鉄心8の間隙が最小にしである下段部分の吸引力が
大きく、この部分を主とする吸引力で、吸引板10を鉄
心8に引き寄せる。
When a current flows through the coil 9 at the start of suction, the suction plate 1
The suction force in the lower part where the gap between the iron core 8 and the iron core 8 is the smallest is large, and the suction plate 10 is drawn to the iron core 8 by the suction force mainly in this part.

この過程で中段の鉄心8と吸引板10の間隙が小さくな
るので、この部分の吸引力も増加し、吸引板10はさら
にたわみ、上段の鉄心8との間隙が同様に小さくなり、
全面に大きな吸引力が発生する。
In this process, the gap between the middle iron core 8 and the suction plate 10 becomes smaller, so the suction force in this part also increases, the suction plate 10 bends further, and the gap with the upper iron core 8 becomes smaller as well.
A large suction force is generated on the entire surface.

吸引板10の復旧は、吸引によって生じる吸引板自体の
たわみエネルギーで戻される。
The suction plate 10 is restored by the deflection energy of the suction plate itself generated by suction.

第6図は本発明の電磁石をさらに高速に吸引動作させる
場合に供給される電流の波形を示す。
FIG. 6 shows the waveform of the current supplied when the electromagnet of the present invention is operated to attract at a higher speed.

般にこの種の電磁石機構では、吸引板の復旧動作を安定
にするため、バックテンション(第1図ではばね6)を
かけており、その状態で電磁石に電流を流した場合、そ
の吸引力が前記バックテンションの大きさに達するまで
は、吸引板は動作しない。
Generally, in this type of electromagnet mechanism, back tension (spring 6 in Figure 1) is applied in order to stabilize the recovery operation of the suction plate, and when current is passed through the electromagnet in this state, the suction force is The suction plate does not operate until the magnitude of the back tension is reached.

従って吸引板を駆動電流供給後、速やかに動作させるた
めには、駆動電流の供給開始に備えて、バックテンショ
ンと同等以下の吸引力で電磁石を励起状態にしておけば
よい。
Therefore, in order to quickly operate the attraction plate after supplying the drive current, the electromagnet may be excited with an attraction force equal to or less than the back tension in preparation for the start of supply of the drive current.

すなわち、波形11はそのためのもので、あらかじめ全
数の電磁石に流しておくための、電流が小量で一定周期
で断続する電流波形であり、12は吸引し、その状態を
保持するための吸引用電流波形、13は吸引するが保持
を不要とする場合の吸引用電流波形であって、14.1
5は波形11に、波形12または13をそれぞれ同期し
て合成した合成波形である。
In other words, waveform 11 is for this purpose, and is a current waveform in which a small amount of current is intermittent at a constant cycle in order to flow through all the electromagnets in advance, and waveform 12 is a current waveform for attracting and maintaining that state. Current waveform 13 is a current waveform for attraction when attraction is not required, and 14.1
5 is a composite waveform obtained by synchronously combining waveform 11 with waveform 12 or 13, respectively.

そして、電磁石には、あらかじめ波形11に示す小量の
断続電流を供給して吸引板が吸着されない程度の微小行
程で吸引板を振動させておき、吸引し、かつ保持を要す
るときには、波形12に示すように所要保持時間だけ持
続して流される吸引用電流を断続電流と同期して電磁石
に流す。
Then, a small amount of intermittent current shown in waveform 11 is supplied to the electromagnet in advance to vibrate the suction plate with a minute stroke that prevents the suction plate from being attracted. When suction and holding are required, waveform 12 As shown, an attraction current that continues for the required holding time is applied to the electromagnet in synchronization with the intermittent current.

従って波形14の合成電流が流れて吸引板は鉄心に吸着
され、電流が流れている時間だけ保持される。
Therefore, the composite current of waveform 14 flows, and the suction plate is attracted to the iron core, and is held for only the time that the current is flowing.

また吸引状態の保持を要IA’いときは、波形13に示
す電流を波形11に同期して電磁石に流す。
Further, when it is necessary to maintain the attracted state, a current shown in waveform 13 is caused to flow through the electromagnet in synchronization with waveform 11.

その結果、波形15の合戒電流が流れ、吸引板は吸着さ
れた後、瞬時にして復旧する。
As a result, a current of waveform 15 flows, and after the suction plate is attracted, it is instantly restored.

このようにあらかじめ吸引板を振動させて、吸引動作が
容易にできるよう準備しておき、これに同期して吸引用
電流を供給することにより、所定タイミングで吸引動作
を高速に行うことが実現できる。
In this way, by vibrating the suction plate in advance to prepare for the suction operation to be performed easily, and then supplying the suction current in synchronization with this, it is possible to perform the suction operation at high speed at a predetermined timing. .

この様な構造になっている力)ら、その効果として多数
の電磁石を並列に一体形で配置することが可能であり、
吸引板は1枚の部品となり、鉄心も1個のブロックから
なり、部品数量が少なく、高密度に収容することができ
る。
The effect of this structure is that it is possible to arrange a large number of electromagnets in parallel in one piece.
The suction plate is a single component, and the iron core is also a single block, so the number of components is small and can be housed in high density.

また吸引の場合に吸引板の動作が、鉄心の下段部から上
段部に向って滑らかに移行することができ、衝突音が少
なく、動作時間の速い電磁石が得られる。
In addition, in the case of suction, the operation of the suction plate can smoothly transition from the lower part of the iron core to the upper part, resulting in an electromagnet with less collision noise and a faster operating time.

なお吸引板の厚さおよび幅は、電磁石の磁束から決定さ
れるが、その場合、吸引板の弾性的なたわみに対する弾
性定数(スチフネス)が大きすぎると、電磁石の吸引エ
ネルギーは吸引板の弾性エネルギーに費やされ、吸引板
の運動エネルギーが大きくならない。
The thickness and width of the suction plate are determined from the magnetic flux of the electromagnet, but in that case, if the elastic constant (stiffness) for elastic deflection of the suction plate is too large, the suction energy of the electromagnet will exceed the elastic energy of the suction plate. , and the kinetic energy of the suction plate does not increase.

これを解決するためには、吸弓板の根元部に隣接する吸
引板の部分の幅を、応力集中が問題とならないような適
当な形で吸引板の中央部分の幅より小さくするとよい。
To solve this problem, the width of the portion of the suction plate adjacent to the root of the suction plate may be made smaller than the width of the central portion of the suction plate in an appropriate manner so that stress concentration does not become a problem.

以上説明したように、本発明の高速作動用電磁石は吸引
板が薄板で軽く、部品数量が少ない簡単な構造であるか
ら、消費電力が少なく、低騒音にして、高速動作が可能
であって、高密度に多数の電磁石を収容することができ
、さらに低価格に製造することができる利点がある。
As explained above, the high-speed operation electromagnet of the present invention has a thin and light suction plate, and has a simple structure with a small number of parts, so it consumes less power, has low noise, and is capable of high-speed operation. It has the advantage of being able to accommodate a large number of electromagnets in a high density and also being able to be manufactured at a low cost.

従って、多数の電磁石で構成されるマトリックス印刷機
およびラインプリンタ等に応用することが可能であり、
特にマトリックスのラインプリンタには最適である。
Therefore, it can be applied to matrix printing machines, line printers, etc. that are composed of a large number of electromagnets.
It is especially suitable for matrix line printers.

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

第1図は従来の一般的な電磁石の側面図、第2図は本発
明の一実施例の斜視図、第3図第4図および第5図はそ
の分解斜視図、第6図は本発明の電磁石を特に高速動作
させる場合に供給される電流の波形図である。 1・・・・・・継鉄、2,8・・・・・・鉄心、3,9
・・・・・・コイル、4,10・・・・・・吸引板(接
極子)、5・・・・・・保持板、6・・・・・・ばね、
7・・・・・・止め金、11,12゜1300060.
電流波形、14,15・・・・・・合成電流波形。
Fig. 1 is a side view of a conventional general electromagnet, Fig. 2 is a perspective view of an embodiment of the present invention, Fig. 3, Figs. 4 and 5 are exploded perspective views thereof, and Fig. 6 is a perspective view of an embodiment of the present invention. FIG. 3 is a waveform diagram of current supplied when operating the electromagnet particularly at high speed. 1...Yoke, 2,8...Iron core, 3,9
... Coil, 4, 10 ... Attraction plate (armature), 5 ... Holding plate, 6 ... Spring,
7... Clasp, 11, 12° 1300060.
Current waveform, 14, 15... Composite current waveform.

Claims (1)

【特許請求の範囲】 1 曲げ疲労強度が高く、磁束密度が大きく、かつ残留
磁気の小さい1枚の金属板により、複数個の接極子群を
、それらの根元を共通通にして一体に形成し、該接極子
釜1個に対応して複数個の鉄心を設け、複数個の該鉄心
には、該接極子釜1個に対応して一体に成形した各1個
のコイルを取り付けて電磁石を構成し前記複数個の接極
子群の各1接極子は各々独立に制御可能とし、各接極子
が励磁によってマグネットの磁極に吸引されている状態
から励磁を解放したとき、接極子が自らの弾性エネルギ
ーによって、元の状態に復帰する機能を備えていること
を特徴とする高速作動用電磁石。 2 曲げ疲労強度が高く、磁束密度が大きく、かつ残留
磁気の小さい1枚の金属板により、複数個の接極子群を
、それらの根元を共通にして一体に形成し、該金属板か
らなる接極子の根元に隣接する部分の幅を、該接極子の
中央部分の幅より小さくし、該接極子釜1個に対応して
複数個の鉄心を設け、複数個の該鉄心には、該接極子釜
1個に対応して一体に成形した各1個のコイルを取り付
けて電磁石を構成し、前記複数個の接極子群の各接極子
は各々独立に制御可能とし、各接極子が励磁によってマ
グネットの磁極に吸引されている状態から励磁を解放し
たとき、接極子が自らの弾性エネルギーによって、元の
状態に復帰する機能を備えていることを特徴とする高速
作動用電磁石。
[Scope of Claims] 1 A plurality of armature groups are integrally formed using a single metal plate having high bending fatigue strength, high magnetic flux density, and low residual magnetism, with their roots common to each other. , a plurality of iron cores are provided corresponding to one armature hook, and each of the plurality of iron cores is attached with a coil molded integrally corresponding to one armature hook to form an electromagnet. Each armature of the plurality of armature groups can be controlled independently, and when each armature is released from the state in which it is attracted to the magnetic pole of the magnet by excitation, the armature has its own elasticity. A high-speed operating electromagnet characterized by the ability to return to its original state using energy. 2 A plurality of armature groups are integrally formed by a single metal plate with high bending fatigue strength, high magnetic flux density, and low residual magnetism, and the joints made of the metal plate are The width of the part adjacent to the base of the pole is made smaller than the width of the central part of the armature, and a plurality of iron cores are provided corresponding to one armature hook, and the plurality of iron cores are provided with the armature. An electromagnet is constructed by attaching one integrally molded coil corresponding to one pole pot, and each armature of the plurality of armature groups can be independently controlled, and each armature can be controlled by excitation. A high-speed operating electromagnet characterized by having a function in which the armature returns to its original state by its own elastic energy when excitation is released from a state where it is attracted to the magnetic poles of the magnet.
JP51000367A 1976-01-05 1976-01-05 Electromagnet for high speed operation Expired JPS5842603B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51000367A JPS5842603B2 (en) 1976-01-05 1976-01-05 Electromagnet for high speed operation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51000367A JPS5842603B2 (en) 1976-01-05 1976-01-05 Electromagnet for high speed operation

Publications (2)

Publication Number Publication Date
JPS5284455A JPS5284455A (en) 1977-07-14
JPS5842603B2 true JPS5842603B2 (en) 1983-09-21

Family

ID=11471814

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51000367A Expired JPS5842603B2 (en) 1976-01-05 1976-01-05 Electromagnet for high speed operation

Country Status (1)

Country Link
JP (1) JPS5842603B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS623001U (en) * 1985-06-21 1987-01-09
JPH02106472U (en) * 1989-02-14 1990-08-23

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5836466A (en) * 1981-08-26 1983-03-03 Hitachi Ltd Printer head
JPS6445654A (en) * 1988-04-08 1989-02-20 Oki Electric Ind Co Ltd Printing head for dot printer
JPS6445653A (en) * 1988-04-08 1989-02-20 Oki Electric Ind Co Ltd Printing head for dot printer

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS623001U (en) * 1985-06-21 1987-01-09
JPH02106472U (en) * 1989-02-14 1990-08-23

Also Published As

Publication number Publication date
JPS5284455A (en) 1977-07-14

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