JP3479555B2 - Deflection yoke - Google Patents

Deflection yoke

Info

Publication number
JP3479555B2
JP3479555B2 JP14316594A JP14316594A JP3479555B2 JP 3479555 B2 JP3479555 B2 JP 3479555B2 JP 14316594 A JP14316594 A JP 14316594A JP 14316594 A JP14316594 A JP 14316594A JP 3479555 B2 JP3479555 B2 JP 3479555B2
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic
deflection yoke
bar
shaped permanent
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 - Fee Related
Application number
JP14316594A
Other languages
Japanese (ja)
Other versions
JPH087788A (en
Inventor
伸一郎 福宿
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 Corp
Panasonic Holdings Corp
Original Assignee
Panasonic Corp
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 Panasonic Corp, Matsushita Electric Industrial Co Ltd filed Critical Panasonic Corp
Priority to JP14316594A priority Critical patent/JP3479555B2/en
Publication of JPH087788A publication Critical patent/JPH087788A/en
Application granted granted Critical
Publication of JP3479555B2 publication Critical patent/JP3479555B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 【0001】 【産業上の利用分野】本発明はテレビジョン受像機等に
用いられる偏向ヨークに関する。 【0002】 【従来の技術】テレビジョン受像機に使用される偏向ヨ
ークシステムは、上下糸巻歪フリー方式となっており、
その対策として偏向ヨークの開口部上下に棒状永久磁石
を使用している。図5は従来の偏向ヨークの一例を示す
もので、7は絶縁枠で、コア8を取付けている。偏向ヨ
ークは電子ビームを偏向するための水平偏向コイル、垂
直偏向コイル及びフロント側上下に一対の棒状永久磁石
9、9を備えている。 【0003】上記偏向ヨークにおいて、陰極線管(CR
T)の電子銃から発射された電子ビームは、一方の棒状
永久磁石9により上へ偏向され、他方の棒状永久磁石9
により下へ偏向され上下の糸巻歪が補正される。このよ
うに上下の棒状永久磁石により上下の糸巻歪を補正し、
その補正量は永久磁石の大きさや配置を検討することで
調整するようにしていた。 【0004】 【発明が解決しようとする課題】しかしながら、上記従
来の偏向ヨークでは、棒状永久磁石が弱いと上下の糸巻
歪の補正は図6の点線で示す様に小さくなり、逆に棒状
永久磁石が強いと図7の点線で示す様に中央部分だけ引
っ張られ直線性を失ってしまう。従って、上下の糸巻歪
を補正するにはその補正量に合わせて棒状磁石の大きさ
や形状、配置を充分に検討しなければならず、補正量が
大きくなると永久磁石を大きくしなければならず、他の
特性に不具合が生じるという問題点があった。 【0005】本発明の目的は上記問題点を解消し、永久
磁石の磁界を効率的に電子ビームに作用させることで他
の特性への不具合を低減させつつ永久磁石の大きさ、形
状、取付位置等の検討を容易にする偏向ヨークを提供し
ようとするものである。 【0006】 【課題を解決するための手段】上記目的を達成するため
に本発明は、陰極線管の電子ビームを偏向するための偏
向磁界を発生しフロント側の上下に一対の棒状永久磁石
を有する偏向ヨークにおいて、前記棒状永久磁石の各々
の両端に略L字状の磁性片を配置し、この磁性片は前記
棒状永久磁石の長手方向端部の磁極を形成する面に対向
する磁界収拾(放出)部と偏向ヨーク開口部の曲率と同
曲率に弯曲して延びた磁界放出(収拾)部とからなる偏
向ヨークとした。 【0007】 【作用】本発明は、上記のように棒状永久磁石の両端に
略L字状の磁性片を配置し、この磁性片は前記棒状永久
磁石の長手方向端部の磁極を形成する面に対向する磁界
収拾(放出)部と、偏向ヨーク開口部の曲率と同曲率に
弯曲して延びた磁界放出(収拾)部とを有するので、電
子ビームに対して、棒状永久磁石と磁性片とが同距離に
配置することとなり、磁界の範囲を広げ、磁界を有効利
用できるようになった。従って、上下の糸巻歪は棒状永
久磁石と磁性片の形状を変えることにより調整される。 【0008】 【実施例】以下、本発明の偏向ヨークの一実施例を図1
〜図4を参照して説明する。図1において、1は絶縁
枠、2はコアであり、電子ビームを偏向するための水平
偏向コイル、垂直偏向コイルを備えて偏向ヨークを構成
している。3、3は一対の棒状永久磁石で、偏向ヨーク
のフロント側上下に位置するよう絶縁枠1の周縁に設け
ている。4、4は磁性片で、棒状永久磁石3、3の両端
にそれぞれ配置されている。 【0009】図2は磁性片4を示す拡大斜視図で、4a
は磁界収拾(放出)部、4bは磁界放出(収拾)部であ
る。磁界放出(収拾)部4bは偏向ヨークの開口部の曲
率と同曲率で弯曲し延びた形状をとっている。また、図
3は磁性片4、4を棒状永久磁石3の両端に配置した時
の磁界の説明図である。磁性片4、4の磁界収拾(放
出)部4aはそれぞれ棒状永久磁石3の端部と対向して
おり、磁界放出(収拾)部4bは偏向ヨーク開口部の曲
率と同曲率で弯曲して延びている。このため磁性片4、
4及び棒状永久磁石3は、電子ビームから同距離に位置
している。 【0010】上記のように配置された磁性片及び棒状永
久磁石において、棒状永久磁石3のN極から出た磁束
は、矢印で示す様に磁性片4の磁界収拾部4aを通り、
磁界放出部4bから磁束を放出する。そして磁性片4の
磁界収拾部4bで磁束を収拾し、磁界放出部4aを通っ
て棒状磁石3のS極へ入る。この様に磁性片4、4の磁
界収拾部と放出部とはその役割が変化する。 【0011】上記棒状永久磁石3だけであれば電子ビー
ムに与える影響は図3中、Xの範囲であるが、本実施例
のように磁性片4、4を使用すると電子ビームに与える
影響は図3中、Yの範囲となり、上下の糸巻歪の補正範
囲を大きくすることができた。従って、図4で示した様
に補正前の電子ビーム5の歪を補正後の電子ビーム6に
改善することが可能となった。この様に磁性片の大き
さ、形状、配置等を考慮することで上下の糸巻歪を容易
に改善することができるようになった。 【0012】 【発明の効果】本発明は、上記のように磁性片の形状と
大きさにより棒状永久磁石の磁界を効率よく電子ビーム
に与えることができるようになった。従って、上下の糸
巻歪を改善するため、従来のように永久磁石を大きくす
ることなく磁性片の形状、大きさを変えることでその補
正範囲を大きくして対応することができ、他の特性への
不具合も低減できるようになった。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a deflection yoke used for a television receiver or the like. 2. Description of the Related Art A deflection yoke system used for a television receiver is of an upper and lower pincushion distortion free type.
As a countermeasure, bar-shaped permanent magnets are used above and below the opening of the deflection yoke. FIG. 5 shows an example of a conventional deflection yoke. Reference numeral 7 denotes an insulating frame to which a core 8 is attached. The deflection yoke includes a horizontal deflection coil for deflecting the electron beam, a vertical deflection coil, and a pair of bar-shaped permanent magnets 9 on the front side and below. In the above deflection yoke, a cathode ray tube (CR)
The electron beam emitted from the electron gun T) is deflected upward by one of the rod-shaped permanent magnets 9, and is deflected by the other.
And the upper and lower pincushion distortions are corrected. The upper and lower pincushion distortion is corrected by the upper and lower bar-shaped permanent magnets,
The correction amount was adjusted by examining the size and arrangement of the permanent magnet. However, in the above-described conventional deflection yoke, when the bar-shaped permanent magnet is weak, the correction of the upper and lower pincushion distortions is reduced as shown by the dotted line in FIG. Is strong, only the central portion is pulled as shown by the dotted line in FIG. 7, and the linearity is lost. Therefore, in order to correct the upper and lower pincushion distortions, the size, shape, and arrangement of the bar-shaped magnet must be sufficiently considered in accordance with the correction amount, and if the correction amount is large, the permanent magnet must be increased. There has been a problem that other characteristics are disadvantageous. SUMMARY OF THE INVENTION It is an object of the present invention to solve the above-mentioned problems, and to efficiently apply a magnetic field of a permanent magnet to an electron beam, thereby reducing inconvenience to other characteristics while reducing the size, shape, and mounting position of the permanent magnet. It is an object of the present invention to provide a deflection yoke that facilitates the study of the above. In order to achieve the above object, the present invention provides a deflection magnetic field for deflecting an electron beam of a cathode ray tube and has a pair of bar-shaped permanent magnets on the upper and lower sides of a front side. In the deflection yoke, substantially L-shaped magnetic pieces are arranged at both ends of the rod-shaped permanent magnet, and the magnetic pieces are arranged to collect a magnetic field (discharge) facing a surface forming a magnetic pole at a longitudinal end of the rod-shaped permanent magnet. ) And a curvature of the opening of the deflection yoke, and a magnetic field emitting (collecting) portion which is curved and extended to the same curvature. According to the present invention, as described above, both ends of a bar-shaped permanent magnet are provided.
A substantially L-shaped magnetic piece is disposed, and the magnetic piece has a magnetic field pickup (emission) portion facing a surface forming a magnetic pole at a longitudinal end of the bar-shaped permanent magnet, and a curvature equal to a curvature of a deflection yoke opening. Since it has a magnetic field emitting (collecting) portion that extends in a curved manner, the bar-shaped permanent magnet and the magnetic piece are arranged at the same distance from the electron beam, so that the range of the magnetic field can be expanded and the magnetic field can be used effectively. It became so. Therefore, the upper and lower pincushion distortions are adjusted by changing the shapes of the bar-shaped permanent magnet and the magnetic piece. FIG. 1 shows an embodiment of a deflection yoke according to the present invention.
This will be described with reference to FIGS. In FIG. 1, reference numeral 1 denotes an insulating frame, and 2 denotes a core, which comprises a horizontal deflection coil and a vertical deflection coil for deflecting an electron beam to constitute a deflection yoke. Reference numerals 3 and 3 denote a pair of bar-shaped permanent magnets, which are provided on the periphery of the insulating frame 1 so as to be positioned above and below the front side of the deflection yoke. Reference numerals 4 and 4 denote magnetic pieces, which are arranged at both ends of the bar-shaped permanent magnets 3 and 3, respectively. FIG. 2 is an enlarged perspective view showing the magnetic piece 4.
Is a magnetic field collecting (emitting) section, and 4b is a magnetic field emitting (collecting) section. The magnetic field emission (collection) section 4b has a shape that is curved and extended at the same curvature as the curvature of the opening of the deflection yoke. FIG. 3 is an explanatory diagram of a magnetic field when the magnetic pieces 4 and 4 are arranged at both ends of the bar-shaped permanent magnet 3. The magnetic field collecting (emitting) portions 4a of the magnetic pieces 4, 4 face the ends of the bar-shaped permanent magnet 3, respectively, and the magnetic field emitting (collecting) portion 4b is curved and extends at the same curvature as the curvature of the deflection yoke opening. ing. Therefore, the magnetic piece 4,
4 and the bar-shaped permanent magnet 3 are located at the same distance from the electron beam. In the magnetic piece and the bar-shaped permanent magnet arranged as described above, the magnetic flux coming out of the N pole of the bar-shaped permanent magnet 3 passes through the magnetic field collecting portion 4a of the magnetic piece 4 as shown by the arrow.
The magnetic flux is emitted from the magnetic field emission part 4b. Then, the magnetic flux is collected by the magnetic field collection part 4b of the magnetic piece 4 and enters the S pole of the rod-shaped magnet 3 through the magnetic field emission part 4a. In this way, the roles of the magnetic field collection and emission portions of the magnetic pieces 4, 4 change. If only the rod-shaped permanent magnet 3 is used, the effect on the electron beam is in the range of X in FIG. 3, but when the magnetic pieces 4 and 4 are used as in this embodiment, the effect on the electron beam is not shown. 3, the range was Y, and the upper and lower pincushion distortion correction ranges could be increased. Therefore, as shown in FIG. 4, the distortion of the electron beam 5 before correction can be improved to the electron beam 6 after correction. As described above, the upper and lower pincushion distortions can be easily improved by considering the size, shape, arrangement, and the like of the magnetic pieces. According to the present invention, the magnetic field of the bar-shaped permanent magnet can be efficiently applied to the electron beam by the shape and size of the magnetic piece as described above. Therefore, in order to improve the upper and lower pincushion distortion, the shape and size of the magnetic piece can be changed without increasing the size of the permanent magnet as in the prior art, thereby increasing the correction range and responding to other characteristics. Problems can also be reduced.

【図面の簡単な説明】 【図1】本発明の一実施例として示した偏向ヨークの側
面図 【図2】磁性片の拡大斜視図 【図3】磁性片を棒状永久磁石の両端に配置した時の磁
界の説明図 【図4】本発明による電子ビームの補正の前後を示した
説明図 【図5】従来の偏向ヨークの側面図 【図6】従来の偏向ヨークによる電子ビームの補正を示
した説明図 【図7】電子ビームの補正を示した説明図 【符号の説明】 3 棒状永久磁石 4 磁性片 4a 磁界収拾(放出)部 4b 磁界放出(収拾)部
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a side view of a deflection yoke shown as one embodiment of the present invention. FIG. 2 is an enlarged perspective view of a magnetic piece. FIG. FIG. 4 is an explanatory view showing before and after correction of an electron beam according to the present invention. FIG. 5 is a side view of a conventional deflection yoke. FIG. 6 shows correction of an electron beam by a conventional deflection yoke. FIG. 7 is an explanatory view showing correction of an electron beam. [Description of References] 3 Bar-shaped permanent magnet 4 Magnetic piece 4a Magnetic field collecting (emitting) section 4b Magnetic field emitting (collecting) section

Claims (1)

(57)【特許請求の範囲】 【請求項1】 陰極線管の電子ビームを偏向するための
偏向磁界を発生しフロント側の上下に一対の棒状永久磁
石を有する偏向ヨークにおいて、前記棒状永久磁石の各
々の両端に略L字状の磁性片を配置し、この磁性片は前
記棒状永久磁石の長手方向端部の磁極を形成する面に
向する磁界収拾(放出)部と偏向ヨーク開口部の曲率と
同曲率に弯曲して延びた磁界放出(収拾)部とからなる
ことを特徴とする偏向ヨーク。
(57) Claims 1. In a deflection yoke having a pair of bar-shaped permanent magnets on the front side and above and below, which generates a deflection magnetic field for deflecting an electron beam of a cathode ray tube, A substantially L-shaped magnetic piece is disposed at each of both ends, and the magnetic piece is provided with a magnetic field pickup (emission) part and a deflection part facing a surface forming a magnetic pole at a longitudinal end of the bar-shaped permanent magnet. A deflection yoke, comprising: a curvature of a yoke opening; and a magnetic field emission (collection) portion that is curved and extended to the same curvature.
JP14316594A 1994-06-24 1994-06-24 Deflection yoke Expired - Fee Related JP3479555B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14316594A JP3479555B2 (en) 1994-06-24 1994-06-24 Deflection yoke

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14316594A JP3479555B2 (en) 1994-06-24 1994-06-24 Deflection yoke

Publications (2)

Publication Number Publication Date
JPH087788A JPH087788A (en) 1996-01-12
JP3479555B2 true JP3479555B2 (en) 2003-12-15

Family

ID=15332432

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14316594A Expired - Fee Related JP3479555B2 (en) 1994-06-24 1994-06-24 Deflection yoke

Country Status (1)

Country Link
JP (1) JP3479555B2 (en)

Also Published As

Publication number Publication date
JPH087788A (en) 1996-01-12

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