JPH0381288B2 - - Google Patents

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Publication number
JPH0381288B2
JPH0381288B2 JP62120088A JP12008887A JPH0381288B2 JP H0381288 B2 JPH0381288 B2 JP H0381288B2 JP 62120088 A JP62120088 A JP 62120088A JP 12008887 A JP12008887 A JP 12008887A JP H0381288 B2 JPH0381288 B2 JP H0381288B2
Authority
JP
Japan
Prior art keywords
core
fixed
movable
iron core
magnetic pole
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
JP62120088A
Other languages
Japanese (ja)
Other versions
JPS63285914A (en
Inventor
Tsuneo Kamitsubara
Kenji Iio
Juichi Ando
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.)
MITSUKU KOGYO KK
OOSAKA GASU KK
Original Assignee
MITSUKU KOGYO KK
OOSAKA GASU 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 MITSUKU KOGYO KK, OOSAKA GASU KK filed Critical MITSUKU KOGYO KK
Priority to JP12008887A priority Critical patent/JPS63285914A/en
Publication of JPS63285914A publication Critical patent/JPS63285914A/en
Publication of JPH0381288B2 publication Critical patent/JPH0381288B2/ja
Granted 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〕 本発明は、電気巻線に通電して固定鉄心に対し
て可動鉄心が接離するように機械的吸引力を発生
させる電磁石に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an electromagnet that energizes an electric winding to generate a mechanical attractive force so that a movable core moves toward and away from a fixed core.

〔従来の技術〕[Conventional technology]

従来、電気巻線に通電して固定鉄心に対して可
動鉄心が接離するように機械的吸引力を発生させ
る電磁石は例えば、第7図および第7図の部分構
成図である第6図に示されるように柱状の固定鉄
心1と、固定鉄心1が固定される継鉄2と、固定
鉄心1の磁極面3に対して間隙4を介して磁極面
5が接離する柱状の可動鉄心6と、固定鉄心1、
継鉄2、可動鉄心6および間隙4で形成される磁
路と、通電されることによりこの磁路を励磁する
電気巻線8と、可動鉄心6に接続されるスプリン
グ12とから成り、固定鉄心1の磁極面3および
可動鉄心6の磁極面5のいずれか一方の磁極面を
ほぼ円錐台状の凹部9に、他方の磁極面を凹部9
にほぼ嵌合するようなほぼ円錐台状の凸部10に
形成する。
Conventionally, an electromagnet that generates a mechanical attraction force by energizing an electric winding so that a movable core moves toward and away from a fixed core is shown in FIG. 7 and FIG. 6, which is a partial configuration diagram of FIG. 7, for example. As shown, a columnar fixed core 1, a yoke 2 to which the fixed core 1 is fixed, and a columnar movable core 6 whose magnetic pole surface 5 approaches and separates from the magnetic pole surface 3 of the fixed core 1 through a gap 4. and fixed core 1,
It consists of a magnetic path formed by the yoke 2, the movable iron core 6, and the gap 4, an electric winding 8 that excites this magnetic path by being energized, and a spring 12 connected to the movable iron core 6. One of the magnetic pole surfaces 3 of 1 and the magnetic pole surface 5 of the movable iron core 6 is formed into a substantially truncated conical recess 9, and the other magnetic pole surface is formed into a recess 9.
The convex portion 10 is formed into a substantially truncated conical shape that approximately fits into the convex portion 10.

所定電力で所要ストロークと吸引力を発生する
電磁石の設計、製作に対して厳密な解析的な取り
扱いはほとんど不可能に近く、従来、所要吸引力
の平行根をストローク長で除した、いわゆる、イ
ンデツクス数を基準として空隙密度を仮定し、経
験値の累積による設計、製作を実施していた。
It is almost impossible to perform a rigorous analytical approach to the design and manufacture of electromagnets that generate the required stroke and attraction force with a given power, and conventionally, the so-called index is calculated by dividing the parallel root of the required attraction force by the stroke length. The void density was assumed based on the number of voids, and design and manufacturing were carried out based on accumulated empirical values.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

このため、上述の従来装置は漏洩磁束の存在、
磁性材の飽和現像等により、吸引力特性が必ずし
良くないという問題点があつた。
For this reason, the above-mentioned conventional device suffers from the presence of leakage magnetic flux.
There was a problem in that the attractive force characteristics were not always good due to saturation development of the magnetic material.

そこで、本発明は上述の問題点を解決するため
に提案されたもので、吸引力特性が良好な電磁石
を提供することを目的とする。
Therefore, the present invention was proposed in order to solve the above-mentioned problems, and an object of the present invention is to provide an electromagnet with good attractive force characteristics.

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

本発明者は、第6図、第7図に示される従来装
置について検討した。
The present inventor studied the conventional devices shown in FIGS. 6 and 7.

ここで、固定鉄心1と可動鉄心6の間の吸引力
Fは磁路の励磁によつて矢印11方向に作用し、
その大きさは周知のように次式で示される。
Here, the attractive force F between the fixed iron core 1 and the movable iron core 6 acts in the direction of arrow 11 due to the excitation of the magnetic path,
As is well known, its size is expressed by the following equation.

F=(μπrah/x2sinα・cosα)U2 ……(1) ただし、 x;可動鉄心6の移動可能距離 h;凸部10の高さ ra;凸部10の平均的半径 α;凸部10の側面10aと可動鉄心6の柱軸6
aとの直交面6bとの角度 さて、(1)式の右辺の1/(sinα・cosα)につ
いて、αの40°以上の角度については数値計算す
れば、第8図のグラフに示される結果を得る。
F=(μπr a h/x 2 sinα・cosα) U 2 ... (1) where, ; Side surface 10a of convex portion 10 and column axis 6 of movable iron core 6
Angle between a and the orthogonal plane 6b Now, regarding 1/(sinα・cosα) on the right side of equation (1), if you perform numerical calculations for angles of α of 40° or more, the results are shown in the graph of Figure 8. get.

この第8図からαが70°以上90°以下において顕
著に吸引力が増大することは明白である。
It is clear from FIG. 8 that the suction force increases significantly when α is greater than or equal to 70 degrees and less than 90 degrees.

次に、第1図に示される本発明に係るプランジ
ヤー電磁石を試作し凸部10の高さhの変化に伴
なう吸引力の変化を励磁電力0.73ワツト、可動鉄
心6の移動可能距離x=3.0mmで実測すると第3
図に示されるように可動鉄心6が固定鉄心1に対
して最も離隔したときに凸部10が凹部9に若干
挿入されるように、凸部10の高さhを可動鉄心
6の移動可能距離x=3.0mmより若干高くして3.2
mmにおいて約25%吸引力が増大した。
Next, a plunger electromagnet according to the present invention shown in FIG. 3rd when measured at 3.0mm
As shown in the figure, the height h of the convex part 10 is adjusted to the movable distance of the movable core 6 so that the convex part 10 is slightly inserted into the concave part 9 when the movable core 6 is farthest from the fixed core 1. x = 3.2 slightly higher than 3.0mm
The suction force increased by approximately 25% in mm.

本発明は、上述の知見にもとづいて成立するも
ので、 柱状の固定鉄心と、該固定鉄心が固定される継
鉄と、該固定鉄心の磁極面に対して間隙を介して
磁極面が接離する柱状の可動鉄心と、該固定鉄
心、継鉄、可動鉄心および間隙で形成される磁路
と、通電されることにより該磁路を励磁する電気
巻線とから成り、該固定鉄心の磁極面および該可
動鉄心の磁極面のいずれか一方の磁極面をほぼ円
錐台状の凹部に、他方の磁極面を該凹部にほぼ嵌
合するようなほぼ円錐台状の凸部に形成する電磁
石を改良し、 該凸部の側面と該可動鉄心の柱軸に直交する平
面との傾斜角αを70度以上90度以下に形成し、該
可動鉄心が該固定鉄心に対して最も離隔したとき
に該凸部が該凹部に若干挿入されるように該凸部
の高さhを形成したことを特徴とする電磁石であ
る。
The present invention was established based on the above-mentioned knowledge, and includes a columnar fixed core, a yoke to which the fixed core is fixed, and a magnetic pole surface that approaches and separates from the magnetic pole surface of the fixed core through a gap. It consists of a columnar movable core, a magnetic path formed by the fixed core, a yoke, a movable core, and a gap, and an electric winding that excites the magnetic path when energized. and an improved electromagnet in which one of the magnetic pole surfaces of the movable iron core is formed into a substantially truncated conical concave portion, and the other magnetic pole surface is formed into a substantially truncated conical convex portion that approximately fits into the concave portion. and an inclination angle α between the side surface of the convex portion and a plane perpendicular to the column axis of the movable iron core is formed to be 70 degrees or more and 90 degrees or less, and when the movable iron core is farthest from the fixed iron core, This electromagnet is characterized in that the height h of the convex portion is formed so that the convex portion is slightly inserted into the concave portion.

〔作用〕[Effect]

本発明によれば、凸部の側面と可動鉄心の柱軸
に直交する平面との傾斜角αを70度以上90度以下
に形成するため上述の(1)式により吸引力が増大
し、 可動鉄心が固定鉄心に対して最も離隔したとき
に凸部が凹部に若干挿入されるように凸部の高さ
hを形成するためさらに吸引力が増大する。
According to the present invention, since the inclination angle α between the side surface of the convex portion and the plane orthogonal to the column axis of the movable iron core is formed to be 70 degrees or more and 90 degrees or less, the suction force is increased by the above equation (1), and the movable iron core is movable. Since the height h of the protrusion is formed so that the protrusion is slightly inserted into the recess when the iron core is farthest apart from the fixed iron core, the suction force is further increased.

〔実施例〕〔Example〕

以下、本発明を図面を参照してその実施例に基
づいて説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below based on embodiments with reference to the drawings.

第1図は本発明の一実施例の部分断面図であ
る。第6図の従来装置と構成は共通するが以下の
点において異なる。
FIG. 1 is a partial cross-sectional view of one embodiment of the present invention. Although the configuration is common to the conventional device shown in FIG. 6, it differs in the following points.

凸部10の側面10aと可動鉄心6の柱軸6a
に直交する平面6bとの傾斜角αを70度以上90度
以下に形成する。
Side surface 10a of convex portion 10 and column shaft 6a of movable iron core 6
The inclination angle α with respect to the plane 6b orthogonal to the plane 6b is formed to be 70 degrees or more and 90 degrees or less.

空気抜き孔部13を設けたが設けなくともよ
い。
Although the air vent portion 13 is provided, it may not be provided.

さらに、可動鉄心6が固定鉄心1に対して最も
離隔したときに凸部10が凹部9に若干挿入され
るように凸部10の高さhを形成する。
Furthermore, the height h of the convex portion 10 is formed so that the convex portion 10 is slightly inserted into the concave portion 9 when the movable iron core 6 is farthest apart from the fixed iron core 1.

つまり、本実施例では凸部10の高さhを可動
鉄心6の移動可能距離xよりも若干高くする。
That is, in this embodiment, the height h of the convex portion 10 is made slightly higher than the movable distance x of the movable iron core 6.

なお、点線図示はx=0の固定鉄心1と可動鉄
心6の吸着状態を示す。
In addition, the dotted line illustration shows the adsorption state of the fixed iron core 1 and the movable iron core 6 when x=0.

第2図の第2の実施例では凸部10の先端と凹
部9とが直接当接するように構成した。
In the second embodiment shown in FIG. 2, the tip of the convex portion 10 and the concave portion 9 are configured to be in direct contact with each other.

第4図および第5図の実施例では傾斜角αを90
度に構成した。
In the embodiments shown in FIGS. 4 and 5, the inclination angle α is 90
It was configured once.

なお、固定鉄心1および可動鉄心6は円柱状に
形成することが好適であるが柱状であればよく、
凹部9と凸部10共に円錐台形状が好適であるが
厳密な円錐台である必要はなく、ほぼ円錐台形状
に構成されればよい。
Note that it is preferable that the fixed core 1 and the movable core 6 be formed in a cylindrical shape, but they may be formed in a cylindrical shape.
It is preferable that both the recess 9 and the convex part 10 have a truncated cone shape, but they do not need to be strictly truncated cones, and may be formed approximately in the shape of a truncated cone.

〔発明の効果〕〔Effect of the invention〕

本発明は以上説明したように、吸引力が増大
し、特に、ストロークの初期吸引力が増大すると
いう効果を奏する。
As explained above, the present invention has the effect of increasing the suction force, particularly the initial suction force of the stroke.

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

第1図は本発明の第1の実施例の部分構成図、
第2図は本発明の第2の実施例の部分構成図、第
3図は第1図の実施例の吸引力特性グラフ、第4
図は本発明の第3の実施例の部分構成図、第5図
本発明の第4の実施例の部分構成図、第6図は従
来装置の部分説明図、第7図は第6図の従来装置
の構成図、第8図は第6図の従来装置の吸引力特
性グラフである。 1……固定鉄心、2……継鉄、3,5……磁極
面、4……間隙、6……可動鉄心、8……電気巻
線、9……凹部、10……凸部、10a……側
面。
FIG. 1 is a partial configuration diagram of the first embodiment of the present invention,
FIG. 2 is a partial configuration diagram of the second embodiment of the present invention, FIG. 3 is a suction force characteristic graph of the embodiment of FIG. 1, and FIG.
Figure 5 is a partial configuration diagram of the third embodiment of the present invention, Figure 5 is a partial configuration diagram of the fourth embodiment of the invention, Figure 6 is a partial explanatory diagram of a conventional device, and Figure 7 is the same as in Figure 6. FIG. 8 is a block diagram of the conventional device, and is a graph of the suction force characteristics of the conventional device shown in FIG. DESCRIPTION OF SYMBOLS 1... Fixed iron core, 2... Yoke, 3, 5... Magnetic pole surface, 4... Gap, 6... Movable core, 8... Electric winding, 9... Concave part, 10... Convex part, 10a ……side.

Claims (1)

【特許請求の範囲】 1 柱状の固定鉄心と、該固定鉄心が固定される
継鉄と、該固定鉄心の磁極面に対して間隙を介し
て磁極面が接離する柱状の可動鉄心と、該固定鉄
心、継鉄、可動鉄心および間隙で形成される磁路
と、通電されることにより該磁路を励磁する電気
巻線とから成り、該固定鉄心の磁極面および該可
動鉄心の磁極面のいずれか一方の磁極面をほぼ円
錐台状の凹部に、他方の磁極面を該凹部にほぼ嵌
合するようなほぼ円錐台状の凹部に形成する電磁
石において、 該凸部の側面と該可動鉄心の柱軸に直交する平
面との傾斜角αを70度以上90度以下に形成し、該
可動鉄心が該固定鉄心に対して最も離隔したとき
に該凸部が該凹部に若干挿入されるように該凸部
の高さhを形成したことを特徴とする電磁石。
[Scope of Claims] 1. A columnar fixed core, a yoke to which the fixed core is fixed, a columnar movable core whose magnetic pole surface approaches and separates from the magnetic pole surface of the fixed core through a gap, and a yoke to which the fixed core is fixed. It consists of a magnetic path formed by a fixed iron core, a yoke, a movable iron core, and a gap, and an electric winding that excites the magnetic path when energized. In an electromagnet in which one of the magnetic pole surfaces is formed in a substantially truncated conical recess and the other magnetic pole surface is formed in a substantially truncated conical recess that approximately fits into the recess, the side surface of the convex portion and the movable iron core. An inclination angle α with a plane orthogonal to the column axis is formed to be 70 degrees or more and 90 degrees or less, so that the convex portion is slightly inserted into the concave portion when the movable core is farthest from the fixed core. An electromagnet characterized in that the convex portion has a height h.
JP12008887A 1987-05-19 1987-05-19 Electromagnet Granted JPS63285914A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12008887A JPS63285914A (en) 1987-05-19 1987-05-19 Electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12008887A JPS63285914A (en) 1987-05-19 1987-05-19 Electromagnet

Publications (2)

Publication Number Publication Date
JPS63285914A JPS63285914A (en) 1988-11-22
JPH0381288B2 true JPH0381288B2 (en) 1991-12-27

Family

ID=14777611

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12008887A Granted JPS63285914A (en) 1987-05-19 1987-05-19 Electromagnet

Country Status (1)

Country Link
JP (1) JPS63285914A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0525203Y2 (en) * 1989-01-11 1993-06-25

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5512407U (en) * 1978-07-08 1980-01-26
JPS59177904A (en) * 1983-03-28 1984-10-08 Matsushita Electric Works Ltd Solenoid
JPS6016734A (en) * 1983-07-08 1985-01-28 Yaesu Musen Co Ltd Communication equipment circuit
JPS611697U (en) * 1984-06-11 1986-01-08 三菱電機株式会社 Air cleaner
JPS6127630A (en) * 1984-07-18 1986-02-07 Nec Corp Manufacture of semiconductor device
JPS6141123A (en) * 1984-08-01 1986-02-27 Sharp Corp Glare proof mirror of liquid crystal type

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58178578U (en) * 1982-05-25 1983-11-29 株式会社ウオルブロ−フア−イ−スト dc solenoid valve

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5512407U (en) * 1978-07-08 1980-01-26
JPS59177904A (en) * 1983-03-28 1984-10-08 Matsushita Electric Works Ltd Solenoid
JPS6016734A (en) * 1983-07-08 1985-01-28 Yaesu Musen Co Ltd Communication equipment circuit
JPS611697U (en) * 1984-06-11 1986-01-08 三菱電機株式会社 Air cleaner
JPS6127630A (en) * 1984-07-18 1986-02-07 Nec Corp Manufacture of semiconductor device
JPS6141123A (en) * 1984-08-01 1986-02-27 Sharp Corp Glare proof mirror of liquid crystal type

Also Published As

Publication number Publication date
JPS63285914A (en) 1988-11-22

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