JPH0510330Y2 - - Google Patents
Info
- Publication number
- JPH0510330Y2 JPH0510330Y2 JP1986043401U JP4340186U JPH0510330Y2 JP H0510330 Y2 JPH0510330 Y2 JP H0510330Y2 JP 1986043401 U JP1986043401 U JP 1986043401U JP 4340186 U JP4340186 U JP 4340186U JP H0510330 Y2 JPH0510330 Y2 JP H0510330Y2
- Authority
- JP
- Japan
- Prior art keywords
- armature
- yoke
- iron core
- electromagnet
- head
- 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
Links
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims description 20
- 238000000418 atomic force spectrum Methods 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
Landscapes
- Electromagnets (AREA)
Description
【考案の詳細な説明】
〔技術分野〕
本考案はリレー等に使用する電磁石に関する。
さらに詳しくはヒンジ型電磁石に関するものであ
る。[Detailed Description of the Invention] [Technical Field] The present invention relates to an electromagnet used in relays and the like.
More specifically, it relates to hinged electromagnets.
従来この種のヒンジ型電磁石を使用したリレー
は、傾向として開放電圧が低く、この電磁石の負
荷やその他の条件によつては復帰不良が発生する
おそれがあつた為、その復帰力を与える復帰ばね
を強くすることにより必要な復帰力を得ていた
が、その結果として同時に感動電圧も高くなつて
しまい高感度では動作し難くなるという問題があ
つた。又、復帰ばねを強くすると開閉時にヒンジ
部分の摩耗が激しく開閉回数が増すに従い特性が
不安定になるという問題がつた。
Conventionally, relays using this type of hinge-type electromagnet tended to have low open circuit voltages, and there was a risk of reset failure depending on the load on the electromagnet and other conditions, so a return spring was used to provide the reset force. The necessary restoring force was obtained by increasing the voltage, but as a result, the sensing voltage also increased, making it difficult to operate at high sensitivity. Furthermore, if the return spring is strengthened, the hinge portion will be worn severely during opening and closing, and as the number of openings and closings increases, the characteristics will become unstable.
本考案は上記事情に鑑み、復帰不良のない動作
の安定したリレーを得るため吸引力を高くするこ
となく、復帰力で高くすることができる電磁石を
提供するものである。
In view of the above-mentioned circumstances, the present invention provides an electromagnet that can increase the return force without increasing the attraction force in order to obtain a relay with stable operation and no return failure.
本考案は、コイル枠と共に鉄芯を取着したヨー
クと、前記ヨークの一端に基端部を係合し自由端
部を前記鉄芯の頭部に対向させると共に復帰ばね
を装架したアマチユアとを有する電磁石におい
て、前記アマチユアの基端部を係合するヨークの
一端と鉄芯の頭部間にアマチユアが鉄芯に吸引さ
れる時にヨークとアマチユア間の前記係合部に磁
気的ギヤツプをつくる第2支点を設けてなること
を特徴とするものであつて、前記第2支点により
吸引力を高くすることなく、復帰力を高くするこ
とができるとするものである。
The present invention includes a yoke to which an iron core is attached together with a coil frame, and an armature having a base end engaged with one end of the yoke, a free end facing the head of the iron core, and equipped with a return spring. In the electromagnet having the above, when the armature is attracted to the iron core between one end of the yoke that engages the base end of the armature and the head of the iron core, a magnetic gap is created at the engaging portion between the yoke and the armature. The device is characterized in that a second fulcrum is provided, and the second fulcrum makes it possible to increase the return force without increasing the suction force.
以下、本考案の一実施例を図面に基づき説明す
る。 Hereinafter, one embodiment of the present invention will be described based on the drawings.
第1図aにおいて、1はヨークであつて、コイ
ル枠2に巻装されたコイル3に並行し延びる一端
1bへアマチユア5の基端部5bをヒンジ係合す
ると共にコイル枠2の一方のつば部2aに並行し
折曲された他端1aへ前記コイル枠2を挿通した
鉄芯4の基端4aを取着し全体に略L形をしてい
る。又、前記ヨーク1の他端1bの中間にはヨー
ク1の一端1aと逆方向に延びる突起1cが設け
られ、その先方と前記アマチユア5の基端部5b
間にはアマチユア5に復帰力を与える復帰ばね6
が装架されている。前記アマチユア5の自由端部
5aの片面は鉄芯4の頭部4bに対向する。 In FIG. 1a, 1 is a yoke which hinge-engages the proximal end 5b of the armature 5 to one end 1b extending parallel to the coil 3 wound around the coil frame 2, and also connects the proximal end 5b of the armature 5 to one end 1b extending parallel to the coil 3 wound around the coil frame 2. The proximal end 4a of the iron core 4, through which the coil frame 2 is inserted, is attached to the other end 1a which is bent parallel to the portion 2a, so that the overall shape is approximately L-shaped. Further, a protrusion 1c extending in the opposite direction to the one end 1a of the yoke 1 is provided in the middle of the other end 1b of the yoke 1, and the protrusion 1c extends between the protrusion 1c and the proximal end 5b of the armature 5.
In between is a return spring 6 that provides a return force to the amateur 5.
is mounted. One side of the free end 5a of the armature 5 faces the head 4b of the iron core 4.
前記アマチユア5の基端部5bとヒンジ係合さ
れるヨーク1の一端1bと、鉄芯4の頭部4bの
間には、アマチユア5が鉄芯4へ吸引され移動す
る時にヨーク1の一端1bとアマチユア5の基端
部5b間へ磁気的ギヤツプをつくる突起10が設
けられている。尚、前記鉄芯4とヨーク1を一つ
の略U形ヨークで構成し、その一脚をコイル枠2
へ挿通し鉄芯4としてもよい。 Between one end 1b of the yoke 1 hinged to the base end 5b of the armature 5 and the head 4b of the iron core 4, when the armature 5 is attracted to the iron core 4 and moves, the one end 1b of the yoke 1 A protrusion 10 is provided to create a magnetic gap between the armature 5 and the proximal end 5b of the armature 5. The iron core 4 and the yoke 1 are composed of one approximately U-shaped yoke, and the one leg is connected to the coil frame 2.
The iron core 4 may be inserted into the iron core 4.
前記コイル3へ通電する電流を徐々に増加して
ゆき第2図に示す起磁力の吸引力曲線がばね負荷
曲線Lより大きくなり曲線Aになつた場合、点A
1で前記アマチユア5が鉄芯4に吸引され移動し
始め点A2でアマチユア5が突起10に当接され
る。さらに吸引され移動がすすむと同図bの如く
アマチユア5の基端部5bがヨーク1の一端1b
より離れて両者間に磁気的ギヤツプGが形成され
る。この磁気的ギヤツプGにより磁気回路の磁気
抵抗が増大し起磁力が低下した状態で、点A3で
前記アマチユア5の自由端部5aはヨーク1の頭
部4bに当接される。次に電流を徐々に減少させ
てゆくと吸引力曲線がばね負荷曲線Lより低くな
つて曲線Bになると点B1より復帰ばね6の復帰
力が吸引力より大きくなるので前記アマチユア5
の自由端5aはヨーク1の頭部4bより開離し始
め、すみやかに元の位置へ戻る。この場合、従来
ならば曲線cまで起磁力を低下させないと、すな
わち電流を減少させないと前記アマチユア5は復
帰しなかつたが、この突起10を設けることによ
り従来ならば点Dにあり復帰できなかつた曲線B
の起磁力までに低下させるだけでアマチユア5が
復帰する為、電流を減少する割合を少なくし復帰
させることができる。すなわち復帰される起磁力
を高くすることができる。 When the current flowing through the coil 3 is gradually increased and the attraction force curve of the magnetomotive force shown in FIG. 2 becomes larger than the spring load curve L and becomes curve A, point A
At point A2, the armature 5 is attracted to the iron core 4 and begins to move, and at point A2, the armature 5 comes into contact with the protrusion 10. As the suction continues and the movement progresses, the proximal end 5b of the armature 5 is moved to the one end 1b of the yoke 1, as shown in Figure b.
As they move further apart, a magnetic gap G is formed between them. With this magnetic gap G increasing the magnetic resistance of the magnetic circuit and reducing the magnetomotive force, the free end 5a of the armature 5 comes into contact with the head 4b of the yoke 1 at point A3. Next, as the current is gradually decreased, the attraction force curve becomes lower than the spring load curve L and reaches curve B. From point B1, the return force of the return spring 6 becomes greater than the attraction force, so the armature 5
The free end 5a of the yoke 1 begins to separate from the head 4b of the yoke 1 and quickly returns to its original position. In this case, conventionally, the armature 5 would not return unless the magnetomotive force was lowered to curve c, that is, the current was reduced, but by providing this protrusion 10, conventionally the armature 5 would be at point D and would not be able to return. curve B
Since the armature 5 is restored by simply reducing the magnetomotive force to , it is possible to restore the current by reducing the rate at which the current is reduced. In other words, the returned magnetomotive force can be increased.
尚、前記突起10はコイル枠2のつば部2bに
設けることに限定されず、アマチユア5が鉄芯4
に吸引される時にヨーク1とアマチユア5の間に
磁気的ギヤツプが形成できるのであれば第3図に
示す如くヨーク1の一端1bと鉄芯4の頭部4b
の間に対向したアマチユア5の中間に前記つば部
2bに延びる突起10を形成しても何ら差しつか
えない。 Note that the protrusion 10 is not limited to being provided on the collar portion 2b of the coil frame 2, and the armature 5 is provided on the iron core 4.
If a magnetic gap can be formed between the yoke 1 and the armature 5 when the armature 5 is attracted to the
There is no problem in forming a protrusion 10 extending to the collar portion 2b between the armatures 5 facing each other.
又、磁気的ギヤツプGを形成する為の前記突起
10の高さは、前記曲線A4の点A4の値が負荷
曲線Lより高ければ、吸引する動作は安定してお
り、この範囲内であるならば任意の高さに設定し
てかまわない。 Furthermore, if the height of the protrusion 10 for forming the magnetic gap G is within this range, if the value at point A4 of the curve A4 is higher than the load curve L, the suction operation is stable. You can set it to any height you want.
本考案は以上の如く、アマチユアの基端部と係
合されるヨークの一端と鉄芯の頭部間へ、アマチ
ユアが鉄芯に吸引される時にヨークとアマチユア
間に磁気的ギヤツプをつくる第2支点を設けるこ
とにより、吸引力を高くすることなく小さな起磁
力の減少によつてアマチユアを復帰させることが
できるので、本考案の電磁石をリレーに使用すれ
ば感動電圧を高くすることなく開放電圧のみを高
くでき特性の安定したリレーを得ることができ
る。又、開放電圧を高くするのに復帰ばねを強く
する必要がないのでヒンジ部の摩耗が少なく開閉
寿命の長いリレーとすることができる等有益であ
る。
As described above, the present invention provides a second magnetic gap between one end of the yoke engaged with the base end of the armature and the head of the iron core, which creates a magnetic gap between the yoke and the armature when the armature is attracted to the iron core. By providing a fulcrum, the armature can be returned to normal position by a small decrease in magnetomotive force without increasing the attractive force, so if the electromagnet of this invention is used in a relay, only the open voltage can be reduced without increasing the impressed voltage. It is possible to obtain a relay with stable characteristics. Further, since it is not necessary to strengthen the return spring to increase the open circuit voltage, it is advantageous that the hinge part is less worn and the relay has a long opening/closing life.
第1図a,bは本考案の一実施例を示すもので
あり、同図aは励磁前の状態を示す側面図、同図
bは励磁時を示す側面図である。第2図は同上の
動作を説明する吸引力−ストローク曲線図であ
る。第3図は本考案の他の実施例を示す要部側面
図である。
1……ヨーク、1b……一端、2……コイル
枠、4……鉄芯、4b……頭部、5……アマチユ
ア、5a……自由端部、5b……基端部、6……
復帰ばね、10……第2支点。
1A and 1B show an embodiment of the present invention, in which FIG. 1A is a side view showing the state before excitation, and FIG. 1B is a side view showing the state during excitation. FIG. 2 is a suction force-stroke curve diagram illustrating the same operation as above. FIG. 3 is a side view of main parts showing another embodiment of the present invention. 1...Yoke, 1b...One end, 2...Coil frame, 4...Iron core, 4b...Head, 5...Armature, 5a...Free end, 5b...Proximal end, 6...
Return spring, 10...second fulcrum.
Claims (1)
記ヨークの一端に基端部を係合し自由端部を前
記鉄芯の頭部に対向させると共に復帰ばねを装
架したアマチユアを有する電磁石において、前
記アマチユアの基端部を係合するヨークの一端
と鉄芯の頭部間に、アマチユアが鉄芯に吸引さ
れる時にヨークとアマチユア間の前記係合部に
磁気的ギヤツプをつくる第2支点を設けてなる
ことを特徴とする電磁石。 (2) 前記第2支点がコイル枠より突設した突起よ
りなる実用新案登録請求の範囲第1項記載の電
磁石。 (3) 前記第2支点がアマチユアに設けた突起より
なる実用新案登録請求の範囲第1項記載の電磁
石。[Claims for Utility Model Registration] (1) A yoke to which an iron core is attached together with a coil frame, a base end portion of which is engaged with one end of the yoke, and a free end portion of which is opposed to the head of the iron core and returned. In an electromagnet having an armature mounted with a spring, the engagement between the yoke and the armature is provided between one end of the yoke that engages the base end of the armature and the head of the iron core when the armature is attracted to the iron core. An electromagnet characterized by having a second fulcrum that creates a magnetic gap at the top of the electromagnet. (2) The electromagnet according to claim 1, wherein the second fulcrum is a projection protruding from the coil frame. (3) The electromagnet according to claim 1, wherein the second fulcrum is a protrusion provided on the armature.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1986043401U JPH0510330Y2 (en) | 1986-03-25 | 1986-03-25 |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1986043401U JPH0510330Y2 (en) | 1986-03-25 | 1986-03-25 |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS62154610U JPS62154610U (en) | 1987-10-01 |
JPH0510330Y2 true JPH0510330Y2 (en) | 1993-03-15 |
Family
ID=30860222
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1986043401U Expired - Lifetime JPH0510330Y2 (en) | 1986-03-25 | 1986-03-25 |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0510330Y2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP4700398B2 (en) * | 2005-04-26 | 2011-06-15 | Idec株式会社 | Safety switch |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4832524U (en) * | 1971-09-02 | 1973-04-19 |
-
1986
- 1986-03-25 JP JP1986043401U patent/JPH0510330Y2/ja not_active Expired - Lifetime
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4832524U (en) * | 1971-09-02 | 1973-04-19 |
Also Published As
Publication number | Publication date |
---|---|
JPS62154610U (en) | 1987-10-01 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CA1250335A (en) | Polarized electromagnetic relay | |
US3470510A (en) | Magnetic latch relay | |
JPH0510330Y2 (en) | ||
US4366459A (en) | Miniature magnetic latch relay | |
JP2588956Y2 (en) | Electromagnetic relay | |
US3599133A (en) | Latch relay motor structure | |
GB2114817A (en) | Electromagnetic relay | |
US4581597A (en) | Electromagnetic actuator | |
JP2505011B2 (en) | Electromagnetic device of circuit breaker | |
US3061765A (en) | Electrical relay armature assembly | |
JP3354189B2 (en) | Electromagnetic relay | |
JP2539099B2 (en) | Electromagnetic relay | |
JP3145811B2 (en) | Electromagnetic relay | |
JPS6051764B2 (en) | AC relay device | |
JPH05174689A (en) | Polarized relay | |
JPS6344931Y2 (en) | ||
JPH0129707Y2 (en) | ||
JPH0668765A (en) | Contact point opening and closing device | |
JP2674385B2 (en) | Electromagnetic relay | |
JP2555722Y2 (en) | Polarized relay | |
JPH0136273Y2 (en) | ||
JPH05298997A (en) | Polarized relay | |
JP2549943B2 (en) | Release type electromagnet device | |
JPH028353Y2 (en) | ||
JPH0327315Y2 (en) |