JPH0969432A - Electromagnetic solenoid - Google Patents

Electromagnetic solenoid

Info

Publication number
JPH0969432A
JPH0969432A JP22294695A JP22294695A JPH0969432A JP H0969432 A JPH0969432 A JP H0969432A JP 22294695 A JP22294695 A JP 22294695A JP 22294695 A JP22294695 A JP 22294695A JP H0969432 A JPH0969432 A JP H0969432A
Authority
JP
Japan
Prior art keywords
iron core
fixed iron
mover
needle
electromagnetic solenoid
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.)
Granted
Application number
JP22294695A
Other languages
Japanese (ja)
Other versions
JP3473208B2 (en
Inventor
Yoshio Mitsutake
義雄 光武
Yoshitaka Ichii
義孝 一井
Katsuhiro Hirata
勝弘 平田
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP22294695A priority Critical patent/JP3473208B2/en
Publication of JPH0969432A publication Critical patent/JPH0969432A/en
Application granted granted Critical
Publication of JP3473208B2 publication Critical patent/JP3473208B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To provide the title electromagnetic solenoid subject to the least fluctuation in the characteristics of magnetic attraction extending over them whole stroke region wherein a needle is shifting. SOLUTION: The title recession type electromagnetic solenoid 1 is provided with an electromagnetic coil 2, a yoke 3 and a fixed iron core 4 magnetization- controlled by an exciting current running in the electromagnetic coil 2, a needle 5 arranged to be shifted on the same axis of the fixed iron core 4 magnetically conducted thereby 4 as well as a spring 7 opposing to the magnetic attraction between the fixed iron core 4 and the needle 5. At this time, respective opposing parts of the fixed iron core 4 and the needle 5 correspond to each other in truncated cone shape in the needle 5 while the fixed iron core 4 almost correspond to the same. In such a constitution, the distance between respective opposing parts in the orthogonal direction to the axial direction is made the longer toward the front end side of the needle 5 when the needle 5 is closest to the fixed iron core 4.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は電磁ソレノイドに関
する。
TECHNICAL FIELD The present invention relates to an electromagnetic solenoid.

【0002】[0002]

【従来の技術】電動によりバルブの開口を操作をする、
例えばディーゼルエンジンの排気ガス再循環装置のバル
ブの開口制御の駆動源として用いられる電磁ソレノイド
は、その制御回路の簡略化のために、電磁コイルに流す
励磁電流に比例した磁気的引力特性が要望される。そし
て一般に、電磁ソレノイドを、スプリングと組み合わ
せ、励磁電流により比例的に操作してバルブの開口制御
を行っている。この様な用途の電磁ソレノイドは、可動
子の移動する全ストローク域に渡って磁気的引力の変動
を少なくするために、固定鉄心と可動子の互いに対向す
る各対向部を、可動子の方を円錐台状に、固定鉄心の方
をそれに略対応する凹状にしている。なお、この固定鉄
心と可動子の軸方向の磁気的引力特性については、軸方
向のある特定の範囲について大きくするために、固定鉄
心と可動子との対向部の円錐台状形状において、一方の
テーパ角度を軸方向位置につれて変化させた略円錐状テ
ーパとすることが開示されている。(例えば特開昭58
−86709)
2. Description of the Related Art A valve opening is operated electrically.
For example, an electromagnetic solenoid used as a drive source for controlling the opening of a valve of an exhaust gas recirculation device of a diesel engine is required to have a magnetic attractive force characteristic proportional to an exciting current flowing in an electromagnetic coil in order to simplify its control circuit. It In general, an electromagnetic solenoid is combined with a spring and operated proportionally by an exciting current to control the valve opening. Electromagnetic solenoids for such applications are designed to reduce the fluctuation of the magnetic attractive force over the entire stroke range of the mover by placing the facing parts of the fixed iron core and the mover on the mover side. The fixed iron core has a concave shape substantially corresponding to the truncated cone shape. Regarding the magnetic attraction characteristics of the fixed iron core and the mover in the axial direction, in order to increase the magnetic attraction in a certain specific range in the axial direction, one of the conical trapezoidal shapes of the facing portion of the fixed iron and the mover is used. It is disclosed that the taper angle is a substantially conical taper that changes in accordance with the axial position. (For example, JP-A-58
-86709)

【0003】[0003]

【発明が解決しようとする課題】上記のものは、対向部
を互いに平坦にしたものとの比較において、磁気的引力
の変動は少ないものとなる。しかし、そのものを細かく
みた場合、ストロークの始まり、すなわち励磁電流の流
れ始めの範囲において、その他の範囲と比較して可動子
への磁気的吸引力の大きいものとなる。従って、ストロ
ークの全域において励磁電流によるバルブの開口の比例
的な操作を行ったとき、ストロークの始まりにて誤差が
生ずるものとなる。そして、その誤差が無視できない場
合には、バルブの開口の操作に供する電磁ソレノイドの
ストロークの範囲を縮小するか、可動子の位置を電気的
に検出し、その検出値を正しい値に調節するために励磁
電流を調節する演算回路を必要とし、低コスト化におい
ての大きな障害となっていた。
In the above-mentioned one, the fluctuation of the magnetic attractive force is small in comparison with the one in which the facing portions are made flat with each other. However, when it is finely divided, the magnetic attraction force to the mover becomes large in the range where the stroke starts, that is, when the exciting current starts to flow, compared to the other ranges. Therefore, when a proportional operation of the valve opening by the exciting current is performed in the entire stroke, an error occurs at the beginning of the stroke. If the error cannot be ignored, the stroke range of the electromagnetic solenoid used to operate the valve opening should be reduced, or the position of the mover should be detected electrically and the detected value should be adjusted to the correct value. In addition, an arithmetic circuit for adjusting the exciting current is required, which is a major obstacle to cost reduction.

【0004】本発明は、かかる事由に鑑みてなしたもの
で、その目的とするところは、可動子の移動するストロ
ーク全域に渡って磁気的引力特性の変動の少ない電磁ソ
レノイドを提供することにある。
The present invention has been made in view of the above circumstances, and an object of the present invention is to provide an electromagnetic solenoid having a small variation in magnetic attractive force characteristics over the entire stroke of movement of a mover. .

【0005】[0005]

【課題を解決するための手段】上記目的を達成するため
に、請求項1記載の電磁ソレノイドは、電磁コイルと、
電磁コイルに流れる励磁電流により磁化制御される継鉄
及び固定鉄心と、固定鉄心より磁気的引力を受けてその
同軸上を移動し得るよう配設される可動子と、固定鉄心
と可動子との間の磁気的引力に対抗するスプリングを具
備し、固定鉄心と可動子の互いに対向する各対向部は、
可動子の方を円錐台状に、固定鉄心の方をそれに略対応
する凹状とした電磁ソレノイドにおいて、軸方向と直交
方向における各対向部間の距離を、前記可動子が固定鉄
心に最も近接したとき、可動子の先端側にいくに従い大
きくなるよう形成した構成としている。これにより、可
動子の変位するストローク全域にて磁気的引力の変化を
小さくできる。
In order to achieve the above object, an electromagnetic solenoid according to claim 1 is provided with an electromagnetic coil,
A yoke and a fixed iron core whose magnetization is controlled by an exciting current flowing through the electromagnetic coil, a mover arranged so as to move on the same axis by receiving a magnetic attractive force from the fixed iron core, and the fixed iron core and the mover. Each of the facing portions of the fixed iron core and the mover, which includes a spring that opposes the magnetic attraction between the
In the electromagnetic solenoid in which the mover has a truncated cone shape and the fixed iron core has a concave shape substantially corresponding thereto, the distance between the facing portions in the axial direction and the orthogonal direction is such that the mover is closest to the fixed iron core. At this time, the movable element is formed so that it becomes larger toward the tip side. As a result, it is possible to reduce the change in the magnetic attractive force over the entire stroke of displacement of the mover.

【0006】また、請求項2記載の電磁ソレノイドは、
前記各対向部を、前記可動子が固定鉄心に最も近接した
とき、その起点が軸方向において略一致する位置に形成
した構成としている。これにより、可動子の変位するス
トローク全域にて変化の小さい、高い磁気的引力が得ら
れる。
The electromagnetic solenoid according to claim 2 is
Each of the facing portions is formed at a position where the starting points of the moving elements are substantially coincident with each other in the axial direction when the mover is closest to the fixed iron core. As a result, a high magnetic attractive force that is small in change throughout the displacement stroke of the mover can be obtained.

【0007】[0007]

【発明の実施の形態】以下、本発明の実施形態を図1及
び図2に基づいて説明する。この電磁ソレノイド1は、
電磁コイル2と、継鉄3及び固定鉄心4と、軸6を有す
る可動子5と、軸を支持する軸受け8及び9と、軸の位
置を検出するポジションセンサ10と、スプリング7
と、ケーシング11とを主要構成部材とする。
DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIGS. This electromagnetic solenoid 1
The electromagnetic coil 2, the yoke 3, the fixed iron core 4, the mover 5 having the shaft 6, the bearings 8 and 9 for supporting the shaft, the position sensor 10 for detecting the position of the shaft, and the spring 7.
And the casing 11 as main constituent members.

【0008】電磁コイル2は、円筒状の巻胴部2aと、
その両端に連設した鍔部2bを有して合成樹脂にて型造
されてなるボビン2cの巻胴部2aの外周に、表面を絶
縁層にて被覆された軟銅線を巻回して形成される。ボビ
ン2cは、後述する継鉄3及び固定鉄心4を、巻胴部2
aの内側において一定距離を隔てて同軸的に対向配設さ
せる位置決め機能も有する。
The electromagnetic coil 2 includes a cylindrical winding drum portion 2a,
A bobbin 2c, which is formed of synthetic resin and has flanges 2b continuously provided at both ends thereof, is formed by winding an annealed copper wire whose surface is covered with an insulating layer on the outer periphery of the winding body 2a. It The bobbin 2c is provided with a yoke 3 and a fixed iron core 4, which will be described later, and a winding barrel 2
It also has a positioning function of coaxially opposingly arranging a certain distance inside a.

【0009】継鉄3は、磁性金属材料により、ボビン2
cの巻胴部2aの内径に略等しい外径の円筒部3aと、
ボビン2cの鍔部2bの外径と略等しい外径の鍔部3b
とを有する形状に、切削加工等により一体に形成され
る。円筒部3aは、ボビン2cの巻胴部2aの略半分の
長さを有し、その内方には後述する可動子5を同軸上に
遊嵌する。この継鉄3は、円筒部3aをボビン2cの巻
胴部2aの一端側より挿入し、鍔部3bにて位置決めさ
れて配設される。
The yoke 3 is a bobbin 2 made of a magnetic metal material.
a cylindrical portion 3a having an outer diameter substantially equal to the inner diameter of the winding drum portion 2a of c,
A collar portion 3b having an outer diameter substantially equal to the outer diameter of the collar portion 2b of the bobbin 2c.
And is integrally formed by cutting or the like. The cylindrical portion 3a has a length that is substantially half the length of the winding drum portion 2a of the bobbin 2c, and a movable element 5 described later is coaxially loosely fitted therein. The yoke 3 is arranged such that the cylindrical portion 3a is inserted from one end side of the winding barrel portion 2a of the bobbin 2c and the collar portion 3b positions it.

【0010】固定鉄心4は、磁性金属材料により、ボビ
ン2cの巻胴部2aの内径に略等しい外径の円筒部4a
と、ボビン2cの鍔部2bの外径と略等しい外径の鍔部
4bとを有する形状に、切削加工等により一体に形成さ
れる。円筒部4aは、後述する可動子5の対向部に対向
する凹状の対向部4cと、後述する軸6及びスプリング
7を挿通する軸穴とを有する。この固定鉄心4は、円筒
部4aをボビン2cの巻胴部2aの継鉄3を配設した他
端側より挿入し、鍔部4bにて位置決めされて継鉄3の
円筒部3aと一定距離を隔てて対向して配設される。な
お、可動子と関係する構成の詳細は後述する。
The fixed iron core 4 is made of a magnetic metal material and has a cylindrical portion 4a having an outer diameter substantially equal to the inner diameter of the winding barrel portion 2a of the bobbin 2c.
And a collar 4b having an outer diameter substantially equal to the outer diameter of the collar 2b of the bobbin 2c are integrally formed by cutting or the like. The cylindrical portion 4a has a concave facing portion 4c that faces a facing portion of the mover 5 described below, and a shaft hole into which a shaft 6 and a spring 7 described below are inserted. In this fixed iron core 4, the cylindrical portion 4a is inserted from the other end side where the yoke 3 of the winding barrel portion 2a of the bobbin 2c is arranged, and is positioned by the collar portion 4b so that the cylindrical portion 3a of the yoke 3 has a constant distance. Are arranged to face each other. The details of the configuration related to the mover will be described later.

【0011】可動子5は、磁性金属材料により、中心に
肉逃がしの穴を設けた円柱部5aと、固定鉄心4の対向
部4cと対向する対向部5bを有して形成される。さら
に詳しくは、円柱部5aは、その外径を継鉄3の円筒部
3aの内径より僅かに小さい寸法とし、中心の肉逃がし
穴寸法は適宜とし、後述する軸6を固着する固着穴を中
心に有する。対向部5bは、円柱部5aと連なる円錐台
状とし、中心には後述する軸6及びスプリング7を挿通
する軸穴を有する。この可動子5は、軸6を固着穴に貫
通して所定の位置に固着し、後述する第1軸受け8及び
第2軸受け9にて軸6の両端が往復動自在に支持され
て、継鉄3の円筒部3aの内側の同軸上に配設される。
The mover 5 is formed of a magnetic metal material and has a columnar portion 5a having a hole for flesh relief in the center and an opposed portion 5b opposed to the opposed portion 4c of the fixed iron core 4. More specifically, the outer diameter of the cylindrical portion 5a is set to be slightly smaller than the inner diameter of the cylindrical portion 3a of the yoke 3, and the size of the central meat relief hole is set appropriately so that the center of the fixing hole for fixing the shaft 6 will be described later. Have. The facing portion 5b has a truncated cone shape that is continuous with the columnar portion 5a, and has a shaft hole through which a shaft 6 and a spring 7, which will be described later, are inserted, at the center. The mover 5 penetrates the shaft 6 through the fixing hole and is fixed at a predetermined position, and both ends of the shaft 6 are reciprocally supported by a first bearing 8 and a second bearing 9, which will be described later. 3 is coaxially arranged inside the cylindrical portion 3a.

【0012】次に固定鉄心4と可動子5との関係する構
成について、図2に基づき説明する。固定鉄心4と可動
子5の互いに対向する対向部4c及び5bは、その各テ
ーパ角度を、固定鉄心の凹状の対向部4cをθ2とし、
可動子5の円錐台状をθ1としたとき、θ2<θ1の関
係としている。すなわち、軸方向と直交方向における各
対向部間の距離を、可動子5が固定鉄心4に最も近接し
たとき、可動子5の先端側にいくに従い大きくなるよう
形成している。また、これらの各対向部は、可動子5が
固定鉄心4に最も近接したとき、その起点が軸方向にお
いて略一致する位置に形成している。
Next, the related structure between the fixed iron core 4 and the mover 5 will be described with reference to FIG. The facing portions 4c and 5b of the fixed iron core 4 and the mover 5 that face each other have respective taper angles set to θ2 for the concave facing portion 4c of the fixed iron core,
When the truncated cone shape of the mover 5 is θ1, the relationship of θ2 <θ1 is established. That is, the distance between the facing portions in the direction orthogonal to the axial direction is formed so as to increase toward the tip side of the mover 5 when the mover 5 is closest to the fixed iron core 4. Further, each of these facing portions is formed at a position where the starting points thereof substantially coincide with each other in the axial direction when the mover 5 comes closest to the fixed iron core 4.

【0013】軸6は、黄銅等の非磁性金属材料により、
可動子5の固着穴と略等しい外径寸法でもって可動子5
より十分長い長さを有して形成され、可動子5に所定位
置に位置するよう固着される。なお、電磁ソレノイド1
から下方に突出する軸6の他端には、図には示されてい
ないが、例えばバルブの開口の調節部材と連結固定され
て、矢印6aに示す直線方向に駆動されることにより、
バルブの開口制御などを行う。
The shaft 6 is made of a non-magnetic metal material such as brass.
The mover 5 has an outer diameter substantially equal to the fixing hole of the mover 5.
It is formed to have a sufficiently longer length and is fixed to the mover 5 so as to be located at a predetermined position. The electromagnetic solenoid 1
Although not shown in the figure, the other end of the shaft 6 projecting downward from is connected and fixed to, for example, an adjusting member for the opening of the valve and driven in the linear direction shown by the arrow 6a,
Controls valve opening.

【0014】スプリング7は、ステンレス等により形成
されたコイルスプリングであり、一端を可動子5、他端
を後述する第1軸受け8にそれぞれ当接させて軸6に遊
嵌され、前述の固定鉄心4に形成された軸穴に遊挿され
る。
The spring 7 is a coil spring made of stainless steel or the like, one end of which is brought into contact with the mover 5 and the other end thereof is brought into contact with a first bearing 8 which will be described later, and is loosely fitted to the shaft 6, and the fixed iron core described above is used. It is loosely inserted in the shaft hole formed in 4.

【0015】第1軸受け8は、合成樹脂により型造さ
れ、固定鉄心4の鍔部4bと略同一の外径寸法を有する
円盤形状をなし、中心部に軸6を往復動自在に支持する
軸穴を有して形成される。
The first bearing 8 is made of synthetic resin and has a disk shape having an outer diameter substantially the same as that of the collar portion 4b of the fixed iron core 4. The shaft 6 reciprocally supports the shaft 6 at its center. It is formed with holes.

【0016】第2軸受け9は、合成樹脂により型造さ
れ、継鉄3の円筒部3aの内径より僅かに大きい外径寸
法を有する円盤形状をなし、可動子5の肉逃がし穴に対
応する円柱状の突起を有し、中心に軸6を往復動自在に
支持する軸穴を有して形成される。この第2軸受け9
は、外径寸法を継鉄3の円筒部3aの内側に圧入固着で
きる程度に設定し、平面9aが継鉄3の鍔部3bの表面
と略同一平面となるよう圧入固着されて、スプリング7
により押圧された可動子5の軸方向の位置決めを行う。
The second bearing 9 is made of synthetic resin, has a disk shape having an outer diameter dimension slightly larger than the inner diameter of the cylindrical portion 3a of the yoke 3, and is a circle corresponding to the meat relief hole of the mover 5. It has a columnar protrusion, and is formed with a shaft hole that supports the shaft 6 in a reciprocating manner at the center. This second bearing 9
Is set so that the outer diameter dimension can be press-fitted and fixed to the inside of the cylindrical portion 3a of the yoke 3, and the flat surface 9a is press-fitted and fixed so as to be substantially flush with the surface of the collar portion 3b of the yoke 3, and the spring 7
The mover 5 pressed by is positioned in the axial direction.

【0017】ポジションセンサ10は、軸6の一端に接
し、軸6の直線方向の位置変位に対応して電気信号を出
力し、図示されない外部回路により、軸6の位置をフィ
ードバック制御するのに供される。このポジションセン
サ10は、例えば摺動型の可変抵抗器により、軸6の変
位を電気抵抗の変化として検出するものが用いられ、電
磁ソレノイド1に固着される鍔部を有したセンサ取付台
10aにて取着される。
The position sensor 10 is in contact with one end of the shaft 6 and outputs an electric signal corresponding to the linear displacement of the shaft 6, and is used for feedback control of the position of the shaft 6 by an external circuit (not shown). To be done. The position sensor 10 uses, for example, a sliding type variable resistor to detect the displacement of the shaft 6 as a change in electric resistance. The position sensor 10 is mounted on a sensor mounting base 10a having a flange portion fixed to the electromagnetic solenoid 1. Be attached.

【0018】ケーシング11は、磁性金属材料により、
継鉄3の鍔部3b及び固定鉄心4の鍔部4bの外径より
僅かに大きい内径の中空円筒部11aと、一端側に第1
軸受け8の周縁部を載置する円環部11bを有して形成
される。中空円筒部11aは、その長さを、第1軸受け
8、固定鉄心4、電磁コイル2、継鉄3及びセンサ取付
台10aを積層した寸法よりやや大きい寸法として、そ
の先端部は、全体を内包固着するための固着部11cと
なる。また、ケーシング11は、電磁コイル2に励磁電
流が流れることにより、継鉄3と、可動子5と、固定鉄
心4とともに磁路を形成する。
The casing 11 is made of a magnetic metal material.
A hollow cylindrical portion 11a having an inner diameter slightly larger than the outer diameters of the collar portion 3b of the yoke 3 and the collar portion 4b of the fixed iron core 4, and a first cylindrical member on one end side.
The bearing 8 is formed to have an annular portion 11b on which the peripheral portion of the bearing 8 is placed. The length of the hollow cylindrical portion 11a is slightly larger than the size in which the first bearing 8, the fixed iron core 4, the electromagnetic coil 2, the yoke 3 and the sensor mounting base 10a are stacked, and the tip portion includes the entire inner surface. It becomes the fixing portion 11c for fixing. Further, the casing 11 forms a magnetic path together with the yoke 3, the mover 5, and the fixed iron core 4 when an exciting current flows through the electromagnetic coil 2.

【0019】電磁ソレノイド1は、以上の部材で構成さ
れ、その組み立てはケーシング11に、まず、第1軸受
け8、固定鉄心4、電磁コイル2、継鉄3の順に挿入
し、次いで、スプリング7と、軸6を所定の位置に固着
した可動子5を挿入し、次いで、第2軸受け9を継鉄3
へ圧入固着した後ポジションセンサ10を挿入する。そ
して、センサ取付台10aから突出しているケーシング
11の縁端部を、所定の押圧力で、センサ取付台10a
の端部外方を押圧するように加圧変形する。
The electromagnetic solenoid 1 is composed of the above-mentioned members, and its assembly is as follows. First, the first bearing 8, the fixed iron core 4, the electromagnetic coil 2 and the yoke 3 are inserted in this order in the casing 11, and then the spring 7 is inserted. , The mover 5 with the shaft 6 fixed at a predetermined position is inserted, and then the second bearing 9 is attached to the yoke 3
The position sensor 10 is inserted after being press-fitted and fixed. Then, the edge of the casing 11 protruding from the sensor mount 10a is pressed with a predetermined pressing force.
Is deformed under pressure so as to press the outside of the end of the.

【0020】上記のように構成される電磁ソレノイド1
において、電磁コイル2の励磁電流が零の場合、可動子
5は、軸6に遊嵌されたスプリング7のばね力により、
図1に示す第1位置(固定鉄心4より最も離れた位置)
にある。電磁コイル2に励磁電流が流れることにより、
継鉄3と、可動子5と、略平行のギャップを設けて配設
された固定鉄心4と、ケーシング11とにより磁路が形
成され、ギャップにおいて、可動子5に対し固定鉄心4
の側に向かう磁気的引力が働く。可動子5及び軸6は、
この磁気的引力とスプリング7のばね力が平衡する位置
まで、矢印6aに示す方向に移動する。可動子5は、電
磁コイル2を流れる励磁電流の所定範囲における最大値
のとき、図1の一点鎖線で示す第2位置(固定鉄心4に
最も近い位置)に到達する。
Electromagnetic solenoid 1 constructed as described above
In the case where the exciting current of the electromagnetic coil 2 is zero, the mover 5 is moved by the spring force of the spring 7 loosely fitted to the shaft 6,
First position shown in FIG. 1 (position farthest from the fixed iron core 4)
It is in. By the exciting current flowing through the electromagnetic coil 2,
A magnetic path is formed by the yoke 3, the mover 5, the fixed iron core 4 provided with a substantially parallel gap, and the casing 11, and the fixed iron core 4 with respect to the mover 5 is formed in the gap.
A magnetic attractive force is applied to the side of. The mover 5 and the shaft 6 are
It moves in the direction indicated by the arrow 6a to a position where this magnetic attractive force and the spring force of the spring 7 are balanced. The mover 5 reaches the second position (position closest to the fixed iron core 4) shown by the alternate long and short dash line in FIG. 1 when the exciting current flowing through the electromagnetic coil 2 has a maximum value in a predetermined range.

【0021】図3は、軸方向の対向部間のギャップの変
化量(以下ストロークと称する)と磁気的引力の関係す
なわち、ストローク−磁気的引力特性の実測データのグ
ラフである。このグラフは、図2に示す本発明の実施形
態の電磁ソレノイド1の、固定鉄心4の凹状の対向部4
cのテーパ角度θ2を60度一定とし、可動子5の円錐
台状の対向部5bのテーパ角度θ1をパラメータとして
変化させたたものの実測データに基づく。このパラメー
タの値については、θ1=60度は従来例の場合、θ1
=65度、及びθ1=70度は本発明の実施形態の場合
を示す。またこのテーパ角度θ1は、テーパを形成する
起点を可動子5の先端面にて一致させ変化させたもので
ある。そしてθ1=70度において、可動子5が固定鉄
心4に最も近接したときに、可動子のテーパ面の終点が
固定鉄心のテーパ面の起点と軸方向において略一致す
る。
FIG. 3 is a graph of the relationship between the amount of change in the gap between the facing portions in the axial direction (hereinafter referred to as the stroke) and the magnetic attractive force, that is, the measured data of the stroke-magnetic attractive force characteristics. This graph shows the concave facing portion 4 of the fixed iron core 4 of the electromagnetic solenoid 1 according to the embodiment of the present invention shown in FIG.
The taper angle θ2 of c is constant at 60 degrees, and the taper angle θ1 of the truncated cone-shaped facing portion 5b of the mover 5 is changed as a parameter, which is based on actual measurement data. Regarding the value of this parameter, θ1 = 60 degrees is θ1 in the case of the conventional example.
= 65 degrees and θ1 = 70 degrees show the case of the embodiment of the present invention. The taper angle θ1 is obtained by changing the starting point for forming the taper on the tip end surface of the mover 5. When θ1 = 70 degrees, when the mover 5 comes closest to the fixed iron core 4, the end point of the tapered surface of the mover substantially coincides with the start point of the tapered surface of the fixed iron core in the axial direction.

【0022】この実測データから明らかなように、従来
例の場合、磁気的引力は、ストロークが2mm以下すな
わち可動子5の第1位置付近において約50Nで、スト
ロークの2mm以上の平均値43.5Nに比べて約15
%程度高いものとなっている。すなわち、固定鉄心4と
可動子5の互いに対向する対向部の各テーパ角度を等し
くしたものは、可動子5が第1位置付近にある状態で
は、励磁電流が流れることにより、磁束は、凹部4cと
対向部5bの対向部間で最も近接する固定鉄心4の凹部
4cの上方縁端に偏って発生し、磁気的引力として大き
く作用することとなる。この磁束の発生が、電磁ソレノ
イドのストローク−磁気的引力特性の変動を大きくさせ
る大きな要因となっている。
As is clear from the measured data, in the case of the conventional example, the magnetic attraction is about 50 N in the stroke of 2 mm or less, that is, near the first position of the mover 5, and the average value of 43.5 N in the stroke of 2 mm or more. About 15 compared to
It is about% high. That is, in the case where the fixed iron core 4 and the mover 5 have the same taper angles in the facing portions, the magnetic flux flows in the concave portion 4c due to the excitation current flowing when the mover 5 is in the vicinity of the first position. Between the facing portions of the facing portion 5b and the facing portion 5b, the unevenness is generated in the upper edge of the concave portion 4c of the fixed iron core 4 closest to the facing portion 5b, and a large magnetic attraction is exerted. The generation of this magnetic flux is a major factor in increasing the fluctuation of the stroke-magnetic attraction characteristic of the electromagnetic solenoid.

【0023】また、本発明の実施の形態における円錐台
状テーパ角度θ1を65度とした場合、磁気的引力は、
ストロークの1mmから7mmの間においての平均は4
3.7Nでその最大変動幅は2.3Nで、その変動の比
率は約±2.6%であり、安定した値であることがわか
る。すなわち、固定鉄心4と可動子5の互いに対向する
対向部の、軸方向と直交方向における各対向部間の距離
を、前記可動子5が固定鉄心4に最も近接したとき、可
動子5の先端側にいくに従い大きくなるよう形成したも
のは、可動子5が第1位置付近にある状態では、励磁電
流が流れることにより、磁束は、凹状の対向部4cと円
錐台状の対向部5bとの対向部間で分散してほぼ均等に
発生し、磁気的引力として、ストロークの大きい場合と
の差が解消されることとなる。その結果、バルブ操作を
行うストローク全域に渡って変動の少ない磁気的引力を
達成できので、励磁電流による比例操作が実現できる。
When the truncated cone taper angle θ1 in the embodiment of the present invention is 65 degrees, the magnetic attractive force is
The average of strokes from 1mm to 7mm is 4
At 3.7 N, the maximum fluctuation range is 2.3 N, and the fluctuation ratio is about ± 2.6%, which is a stable value. That is, the distance between the facing parts of the fixed core 4 and the mover 5 facing each other in the axial direction and the direction orthogonal to each other is such that when the mover 5 is closest to the fixed core 4, the tip of the mover 5 is When the mover 5 is in the vicinity of the first position, the magnetic flux formed between the concave facing portion 4c and the frustoconical facing portion 5b is formed such that the magnetic flux becomes larger toward the side. Dispersion between the opposing portions occurs almost evenly, and the difference between the magnetic attraction and the case where the stroke is large is eliminated. As a result, it is possible to achieve a magnetic attractive force that does not fluctuate over the entire stroke of the valve operation, so that a proportional operation by an exciting current can be realized.

【0024】さらに、本発明の実施の形態における円錐
台状テーパ角度θ1を70度とした場合の磁気的引力
は、ストロークの1mmから7mmの間においての平均
は48Nでその最大変動幅は1.9Nで、その変動の比
率は約±2%であり、θ1=65度と同様に安定した値
を示し、その平均値が約10%大きいものであることが
わかる。すなわち、対向部を、可動子5が固定鉄心4に
最も近接したとき、対向部の起点が軸方向において略一
致する位置に形成したものは、可動子5が第1位置付近
にある状態で励磁電流が流れることにおいて、磁束は、
凹状の対向部4cと円錐台状の対向部5bとの対向部間
で分散してほぼ均等に発生するとともに、対向部間の磁
気抵抗が小さくなることにより、磁気的な効率の向上も
図れることとなる。その結果、θ1を70度としたもの
は、θ1を65度としたものに比べ高い磁気的引力が得
られるので、より低電流による駆動が可能となる。
Further, in the embodiment of the present invention, when the truncated cone taper angle θ1 is set to 70 degrees, the magnetic attractive force is 48 N on average between 1 mm and 7 mm of the stroke, and the maximum fluctuation range is 1. At 9 N, the variation ratio is about ± 2%, which is a stable value similar to θ1 = 65 degrees, and it can be seen that the average value is about 10% larger. That is, when the mover 5 is closest to the fixed iron core 4, the facing part is formed at a position where the starting points of the facing parts are substantially coincident with each other in the axial direction. In the flow of current, the magnetic flux
The concave facing portion 4c and the truncated cone-shaped facing portion 5b are dispersed between the facing portions and generated substantially evenly, and the magnetic resistance between the facing portions is reduced, so that the magnetic efficiency can be improved. Becomes As a result, when θ1 is set to 70 degrees, a higher magnetic attractive force is obtained compared to when θ1 is set to 65 degrees, so that driving with a lower current becomes possible.

【0025】なお、実施形態におけるθ1=70度のも
のにおいて、その各対向部を、可動子5が固定鉄心4に
最も近接したとき、その起点を軸方向において略一致す
る位置に形成したが、これは異なる位置としても磁気的
な効率は低下するものの、磁気的引力の安定化に対する
影響は僅かで何ら問題とはならない。また、固定鉄心4
の凹状のテーパ角度θ2を60度とし、可動子5の円錐
台状のテーパ角度θ1をパラメータとして最大70度ま
でについての実測データを示したが、このテーパ角度θ
2及びθ1は、可動子5及び固定鉄心4の磁性金属材料
の条件、あるいは可動子が固定鉄心に最も近接したとき
の軸方向と直交方向における各対向部間の距離の設定に
おいて設定されるべきもので、何ら限定するものではな
い。
In the embodiment of θ1 = 70 degrees, the respective facing portions are formed so that their starting points are substantially aligned in the axial direction when the mover 5 is closest to the fixed iron core 4. Even if the position is different, the magnetic efficiency is reduced, but the influence on the stabilization of the magnetic attractive force is small and does not pose any problem. In addition, the fixed iron core 4
The concave taper angle θ2 of 60 is set to 60 degrees, and the actual measurement data is shown up to 70 degrees using the truncated cone taper angle θ1 of the mover 5 as a parameter.
2 and θ1 should be set in the condition of the magnetic metal material of the mover 5 and the fixed iron core 4, or in the setting of the distance between the facing parts in the direction orthogonal to the axial direction when the mover is closest to the fixed iron core. But not limiting.

【0026】[0026]

【発明の効果】請求項1記載の電磁ソレノイドは、可動
子の変位するストローク全域にて磁気的引力の変化を小
さくできるので、操作を行うストローク全域に渡って励
磁電流による比例操作が可能となる。
In the electromagnetic solenoid according to the first aspect of the present invention, since the change in the magnetic attractive force can be reduced in the entire stroke of displacement of the mover, proportional operation can be performed by the exciting current over the entire stroke of operation. .

【0027】また、請求項2記載の電磁ソレノイドは、
請求項1記載の効果に加え、可動子の変位するストロー
ク全域にて高い磁気的引力が得られるので、低電流によ
る駆動が可能となる。
The electromagnetic solenoid according to claim 2 is
In addition to the effect of the first aspect, a high magnetic attractive force can be obtained over the entire stroke of displacement of the mover, so that driving with a low current becomes possible.

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

【図1】本発明の実施形態の正面断面図である。FIG. 1 is a front sectional view of an embodiment of the present invention.

【図2】その要部である対向部の部分拡大図である。FIG. 2 is a partially enlarged view of a facing portion that is a main portion thereof.

【図3】そのストローク−磁気的引力特性の特性図であ
る。
FIG. 3 is a characteristic diagram of its stroke-magnetic attraction characteristic.

【符号の説明】[Explanation of symbols]

2 電磁コイル 3 継鉄 4 固定鉄心 5 可動子 6 軸 7 スプリング 8 第1軸受け 9 第2軸受け 10 ポジションセンサ 11 ケーシング 2 Electromagnetic coil 3 Yoke 4 Fixed iron core 5 Mover 6 Shaft 7 Spring 8 1st bearing 9 2nd bearing 10 Position sensor 11 Casing

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 電磁コイルと、電磁コイルに流れる励磁
電流により磁化制御される継鉄及び固定鉄心と、固定鉄
心より磁気的引力を受けてその同軸上を移動し得るよう
配設される可動子と、固定鉄心と可動子との間の磁気的
引力に対抗するスプリングを具備し、固定鉄心と可動子
の互いに対向する各対向部は、可動子の方を円錐台状
に、固定鉄心の方をそれに略対応する凹状とした電磁ソ
レノイドにおいて、 軸方向と直交方向における各対向部間の距離を、前記可
動子が固定鉄心に最も近接したとき、可動子の先端側に
いくに従い大きくなるよう形成してなることを特徴とす
る電磁ソレノイド。
1. An electromagnetic coil, a yoke and a fixed iron core whose magnetization is controlled by an exciting current flowing through the electromagnetic coil, and a mover arranged so as to be movable coaxially by receiving a magnetic attractive force from the fixed iron core. And a spring that opposes the magnetic attraction between the fixed iron core and the mover, and the facing portions of the fixed iron core and the mover that face each other have a frustoconical shape for the mover and a fixed iron core for the opposite direction. In the electromagnetic solenoid with a concave shape that substantially corresponds to that, the distance between the facing parts in the direction orthogonal to the axial direction is formed so as to increase toward the tip side of the mover when the mover is closest to the fixed iron core. An electromagnetic solenoid characterized by being formed.
【請求項2】 前記各対向部は、前記可動子が固定鉄心
に最も近接したとき、その起点が軸方向において略一致
する位置に形成されてなることを特徴とする請求項1記
載の電磁ソレノイド。
2. The electromagnetic solenoid according to claim 1, wherein each of the facing portions is formed at a position where a starting point thereof substantially coincides with an axial direction when the mover is closest to the fixed iron core. .
JP22294695A 1995-08-31 1995-08-31 Electromagnetic solenoid Expired - Fee Related JP3473208B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22294695A JP3473208B2 (en) 1995-08-31 1995-08-31 Electromagnetic solenoid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22294695A JP3473208B2 (en) 1995-08-31 1995-08-31 Electromagnetic solenoid

Publications (2)

Publication Number Publication Date
JPH0969432A true JPH0969432A (en) 1997-03-11
JP3473208B2 JP3473208B2 (en) 2003-12-02

Family

ID=16790358

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22294695A Expired - Fee Related JP3473208B2 (en) 1995-08-31 1995-08-31 Electromagnetic solenoid

Country Status (1)

Country Link
JP (1) JP3473208B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012188977A (en) * 2011-03-10 2012-10-04 Hitachi Automotive Systems Ltd Fuel injection device
JP2014134207A (en) * 2014-04-23 2014-07-24 Hitachi Automotive Systems Ltd Fuel injection device

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012188977A (en) * 2011-03-10 2012-10-04 Hitachi Automotive Systems Ltd Fuel injection device
US11067045B2 (en) 2011-03-10 2021-07-20 Hitachi Automotive Systems, Ltd. Fuel injection device
US11703021B2 (en) 2011-03-10 2023-07-18 Hitachi Astemo, Ltd. Fuel injection device
JP2014134207A (en) * 2014-04-23 2014-07-24 Hitachi Automotive Systems Ltd Fuel injection device

Also Published As

Publication number Publication date
JP3473208B2 (en) 2003-12-02

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