JPS5897809A - Magnetic saturated variable inductor - Google Patents

Magnetic saturated variable inductor

Info

Publication number
JPS5897809A
JPS5897809A JP56198091A JP19809181A JPS5897809A JP S5897809 A JPS5897809 A JP S5897809A JP 56198091 A JP56198091 A JP 56198091A JP 19809181 A JP19809181 A JP 19809181A JP S5897809 A JPS5897809 A JP S5897809A
Authority
JP
Japan
Prior art keywords
drum
magnetic
coil
shaped core
permanent magnet
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
JP56198091A
Other languages
Japanese (ja)
Other versions
JPH0449241B2 (en
Inventor
Koichi Yasuma
安間 康一
Hiroshi Otake
大嶽 博志
Saburo Koresawa
是沢 三郎
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 Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP56198091A priority Critical patent/JPS5897809A/en
Publication of JPS5897809A publication Critical patent/JPS5897809A/en
Publication of JPH0449241B2 publication Critical patent/JPH0449241B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F21/00Variable inductances or transformers of the signal type
    • H01F21/02Variable inductances or transformers of the signal type continuously variable, e.g. variometers
    • H01F21/08Variable inductances or transformers of the signal type continuously variable, e.g. variometers by varying the permeability of the core, e.g. by varying magnetic bias

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Coils Or Transformers For Communication (AREA)

Abstract

PURPOSE:To vary the magnetic bias and amplitude characteristic (saturation curve) and greatly improve the linearity characteristic, by moving a magnetized magnetic substance provided on the outer periphery of a drum core. CONSTITUTION:A coil 8 is wound up around the drum core 7 having flanges 7a, 7b at both end parts and mounted by fixing the flange 7b side of a terminal base 9 having terminal pins 9a. At one open end of the cylindrical magnetic substance 11 wherein a screw part 11a screwed into the screw part 10a of a case 10 is provided on the outer peripheral surface and the both ends are opened, a permanent magnet 12 is fixed so as to block this open end, and this magnetic substance 11 is provided on the outer peripheral part of the drum core 7. The permanent magnet 12 is magnetized N pole and S pole in a thickness direction.

Description

【発明の詳細な説明】 本発明はテレビジョン受像機などの水平直線性の改善に
利用される磁気飽和性可変インダクターに関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetically saturable variable inductor used for improving the horizontal linearity of television receivers and the like.

最近、テレビジョン受像機の高品質化により、特にコン
ピュータの端末器のモニター用テレビジョン受像機に使
用する場合、従来のりニアリティ特性を大幅に向上させ
る必要が生じてきた。すなわち、偏向ヨークのばらつき
、偏向電流のばらつきなどにより、画面の水平方向の左
右に歪が生じるため、個々のテレビジョン受像機に合せ
て、最良のりニアリティ特性が得られるように調整可能
なりニアリテイコイルが要望されている。
Recently, as the quality of television receivers has increased, it has become necessary to significantly improve the linearity characteristics of conventional television receivers, especially when used as monitors for computer terminals. In other words, distortion occurs horizontally on the left and right sides of the screen due to variations in the deflection yoke and deflection current. A coil is requested.

このような要望に応えるだめの従来のりニアリティコイ
ルは、第1図に示すような構造であり、すなわちコイル
1を巻装したドラム型コア2の鍔の外側面に、厚み方向
に磁極を持つ永久磁石3を接着によシ固定した構造であ
る。
The conventional linearity coil that meets these demands has a structure as shown in Figure 1, in which the outer surface of the collar of the drum-shaped core 2 around which the coil 1 is wound has magnetic poles in the thickness direction. It has a structure in which a permanent magnet 3 is fixed by adhesive.

ところが、この第1図に示す従来のりニアリティコイル
の場合、ドラム型コア2および永久磁石3のばらつきに
より、第2図に示す偏向電流IDCとインダクタンスL
との関係の特性(電流重畳特性)が曲線a、bのように
大きくばらつき、直線性補正が悪くなり、十分に要望に
応えることができなかった。なお、第2図において、実
線による特性は中心値を示している。
However, in the case of the conventional linearity coil shown in FIG. 1, due to variations in the drum core 2 and permanent magnet 3, the deflection current IDC and inductance L shown in FIG.
The characteristics (current superimposition characteristics) of the relationship between the current and current values varied greatly as shown by curves a and b, resulting in poor linearity correction, and it was not possible to fully meet the demands. In addition, in FIG. 2, the characteristic indicated by the solid line indicates the central value.

そこで、このような問題点を解決するために、第3図に
示すような構造のものが考えられていた。
In order to solve these problems, a structure as shown in FIG. 3 has been considered.

この第3図に示す従来のりニアリテイコイルは、コイル
4を巻装したドラム型コア6の外周部に、そのドラム型
コア6の両端の鍔と鍔との間を橋渡しするように鍔と対
応する位置に磁極を持つ永久磁石6を並べて配置し、そ
の永久磁石6を回転させて磁気バイアス量を変化するよ
うにしたものである。
In the conventional linearity coil shown in FIG. 3, a coil 4 is wound around a drum-shaped core 6, and the outer periphery of the drum-shaped core 6 is provided with flanges that bridge the gap between the flanges at both ends of the drum-shaped core 6. Permanent magnets 6 having magnetic poles are arranged side by side at the positions where the magnets rotate, and the amount of magnetic bias is changed by rotating the permanent magnets 6.

ところが、この第3図に示すリニアリティコイルの場合
、電流重畳特性が第4図の曲線0.dのように、磁気バ
イアス点の移動のみであるため、十分な直線性補正を行
うことができなかった。
However, in the case of the linearity coil shown in FIG. 3, the current superposition characteristic is as shown in the curve 0.0 in FIG. As shown in d, sufficient linearity correction could not be performed because only the magnetic bias point was moved.

本発明はこのような従来の欠点を解決するもので、リニ
アリティ特性を大幅に改善することを目的とするもので
ある。
The present invention aims to solve these conventional drawbacks and to significantly improve linearity characteristics.

このような目的を達成するために本発明においては、コ
イルを巻装したドラム型コアの外周部に、このドラム型
コアの高さ方向に移動可能な両端が開放した筒状の磁性
体を配設し、かつその磁性体の一方の開放端にこの開放
端を塞ぐように永久磁石を固着したものであシ、従来の
ように永久磁石を移動させて磁気バイアス点を変えるの
ではなく、ドラム型コアの外周部に配設した着磁された
磁性体を移動させることにより、磁気バイアスおよび振
幅特性(飽和曲線)を変化させるものである。
In order to achieve such an object, in the present invention, a cylindrical magnetic body with both ends open and movable in the height direction of the drum-shaped core is disposed around the outer periphery of the drum-shaped core around which the coil is wound. A permanent magnet is fixed to one open end of the magnetic material so as to close this open end. The magnetic bias and amplitude characteristics (saturation curve) are changed by moving a magnetized magnetic body disposed around the outer periphery of the mold core.

以下、本発明の一実施例を示す第6図および第6図の図
面を用いて説明する。
Hereinafter, an embodiment of the present invention will be explained using FIGS. 6 and 6, which show an embodiment of the present invention.

第6図に本発明の一実施例による磁気飽和性可変インダ
クターを示しており、第6図において7は両端部に鍔7
a、7bを有する・+°ラム型ココアあり、このドラム
型コア7にはコイル8が巻装されている。このドラム型
コア7は、端子ビン9aを有する端子台9に一方の鍔T
b側を固定することによシ取付けられている。
FIG. 6 shows a magnetically saturable variable inductor according to an embodiment of the present invention, and in FIG.
There is a +° ram type cocoa having a and 7b, and a coil 8 is wound around this drum type core 7. This drum-shaped core 7 has one flange T on a terminal block 9 having a terminal bin 9a.
It is attached by fixing the b side.

10はドラム型コア7が収納される円筒状のケースであ
り、このケース10の内周面には、ねじ部10&が設け
られている。
Reference numeral 10 denotes a cylindrical case in which the drum-shaped core 7 is housed, and the inner peripheral surface of this case 10 is provided with a threaded portion 10&.

11はこのケース1oのねじ部101Lに螺合するねじ
部11aを外周面に設けた両端が開放した筒状の磁性体
であシ、この磁性体11の一方の開放端にはこの開放端
を塞ぐように永久磁石12が固着され、またこの磁性体
11は前記ドラム型コア7の外周部に配設されている。
Reference numeral 11 denotes a cylindrical magnetic body with both ends open, the outer peripheral surface of which is provided with a threaded portion 11a that is screwed into the threaded portion 101L of the case 1o. A permanent magnet 12 is fixed to cover the drum-shaped core 7, and the magnetic body 11 is disposed around the outer periphery of the drum-shaped core 7.

また永久磁石12は厚み方向にN極、S極に着磁された
ものである。
Further, the permanent magnet 12 is magnetized with N pole and S pole in the thickness direction.

すなわち、この実施例による磁気飽和性可変インダクタ
ーにおいては、コイル8が巻装されたドラム型コア7の
外周部に配設した筒状の磁性体11をドラム型コア7の
高さ方向に上下動させることにより、電流重畳特性を調
整するようにしたものである。
That is, in the magnetically saturable variable inductor according to this embodiment, the cylindrical magnetic body 11 disposed on the outer periphery of the drum-shaped core 7 around which the coil 8 is wound is moved up and down in the height direction of the drum-shaped core 7. By doing so, the current superimposition characteristics are adjusted.

そして、この実施例において、磁性体11を移動させて
、ドラム型コア7に巻装したコイル8に接近させると、
磁路が閉磁路になるため、電流による飽和性は早く変化
し、飽和曲線の傾斜が立ち、Lかも永久磁石12の影響
を受けやすくなるので、バイアス点も変化し、第6図の
曲線Eの特性となる。逆に、磁性体11をドラム型コア
7よシ遠ざけると、磁路が開磁路となるため、電流によ
る飽和特性は遅く変化し、飽和曲線の傾斜、が第6図の
曲線Fとなる。
In this embodiment, when the magnetic body 11 is moved to approach the coil 8 wound around the drum-shaped core 7,
Since the magnetic path becomes a closed magnetic path, the saturation due to the current changes quickly, the saturation curve becomes steeper, and L becomes more susceptible to the influence of the permanent magnet 12, so the bias point also changes, resulting in curve E in Figure 6. It is a characteristic of Conversely, when the magnetic body 11 is moved away from the drum-shaped core 7, the magnetic path becomes an open magnetic path, so the saturation characteristics due to current change slowly, and the slope of the saturation curve becomes curve F in FIG. 6.

以上のように本発明の磁気飽和性可変インダクターによ
れば、ドラム型コアの形状9着磁量のばらつきが磁性体
を移動させることにより吸収され、安定した電流重畳特
性を得るこ、とができる。また、磁性体の高さ方向の形
状を変えることにより、磁気構造に与える磁束の量が変
わるため、電流重畳特性を任意に設定することができ、
しかもドラム型コアの外周部に磁性体が配置されている
ため、漏洩磁束が少なくなシ、テレビジョン受像機の画
面に及ぼす影響も少ないという効果が得られる。
As described above, according to the variable magnetic saturation inductor of the present invention, variations in the amount of magnetization of the drum-shaped core can be absorbed by moving the magnetic body, and stable current superimposition characteristics can be obtained. . In addition, by changing the shape of the magnetic body in the height direction, the amount of magnetic flux applied to the magnetic structure changes, so the current superimposition characteristics can be set arbitrarily.
Furthermore, since the magnetic material is arranged around the outer periphery of the drum-shaped core, it is possible to obtain the effect that there is less leakage magnetic flux and less influence on the screen of the television receiver.

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

第1図嬬従来の17 ニアリティコイルの概略構成を示
す断面図、第2図は同コイルの電流重畳特性図、第3図
は他の従来のりニアリティコイルの概略構成を示す断面
図、第4図は同コイルの電流重畳特性図、第6図は本発
明の一実施例による磁気飽和性可変インダクターの概略
構成を示す断面図、第6図は同可変イ/ダクターの電流
重畳特性図である。 7・・・・・・ドラム型コア、8・・・・・・コイル、
11・・・・・・磁性体、12・・・・・・永久磁石。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名11
s 2 m 第4ffil 第3図中 115図 にa 第6図 −Ipe   ’   +Ivc
Fig. 1 is a sectional view showing the schematic structure of a conventional 17 linearity coil, Fig. 2 is a current superimposition characteristic diagram of the coil, and Fig. 3 is a sectional view showing the schematic structure of another conventional linearity coil. Fig. 4 is a current superimposition characteristic diagram of the same coil, Fig. 6 is a sectional view showing a schematic configuration of a magnetically saturable variable inductor according to an embodiment of the present invention, and Fig. 6 is a current superimposition characteristic diagram of the same variable inductor. be. 7...Drum-shaped core, 8...Coil,
11...Magnetic material, 12...Permanent magnet. Name of agent: Patent attorney Toshio Nakao and 1 other person11
s 2 m 4th ffil a in Figure 115 in Figure 3 Figure 6 - Ipe' + Ivc

Claims (1)

【特許請求の範囲】[Claims] コイルを巻装したドラム型コアの外周部に、このドラム
型コアの高さ方向に移動可能な両端が開放した筒状の磁
性体を配設し、かつその磁性体の一方の開放端にこの開
放端を塞ぐように永久磁石を固着した磁気飽和性可変イ
ンダクター。
A cylindrical magnetic body with both ends open and movable in the height direction of the drum-shaped core is arranged on the outer circumference of the drum-shaped core around which the coil is wound, and this magnetic body is attached to one open end of the magnetic body. A magnetically saturable variable inductor with a permanent magnet fixed so as to close the open end.
JP56198091A 1981-12-08 1981-12-08 Magnetic saturated variable inductor Granted JPS5897809A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56198091A JPS5897809A (en) 1981-12-08 1981-12-08 Magnetic saturated variable inductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56198091A JPS5897809A (en) 1981-12-08 1981-12-08 Magnetic saturated variable inductor

Publications (2)

Publication Number Publication Date
JPS5897809A true JPS5897809A (en) 1983-06-10
JPH0449241B2 JPH0449241B2 (en) 1992-08-11

Family

ID=16385343

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56198091A Granted JPS5897809A (en) 1981-12-08 1981-12-08 Magnetic saturated variable inductor

Country Status (1)

Country Link
JP (1) JPS5897809A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3534451A1 (en) * 1985-09-27 1987-04-02 Vogt Electronic Ag ADJUSTABLE LINEARITY COIL

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103824675A (en) * 2013-12-31 2014-05-28 芜湖国睿兆伏电子有限公司 Adjustable inductor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3534451A1 (en) * 1985-09-27 1987-04-02 Vogt Electronic Ag ADJUSTABLE LINEARITY COIL

Also Published As

Publication number Publication date
JPH0449241B2 (en) 1992-08-11

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