JPS59191238A - Deflection yoke - Google Patents

Deflection yoke

Info

Publication number
JPS59191238A
JPS59191238A JP6553583A JP6553583A JPS59191238A JP S59191238 A JPS59191238 A JP S59191238A JP 6553583 A JP6553583 A JP 6553583A JP 6553583 A JP6553583 A JP 6553583A JP S59191238 A JPS59191238 A JP S59191238A
Authority
JP
Japan
Prior art keywords
deflection
vertical deflection
deflection yoke
vertical
magnetic field
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.)
Pending
Application number
JP6553583A
Other languages
Japanese (ja)
Inventor
Toshiharu Shimizu
清水 敏治
Noritaka Okuyama
宣隆 奥山
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP6553583A priority Critical patent/JPS59191238A/en
Publication of JPS59191238A publication Critical patent/JPS59191238A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/46Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
    • H01J29/70Arrangements for deflecting ray or beam
    • H01J29/72Arrangements for deflecting ray or beam along one straight line or along two perpendicular straight lines
    • H01J29/76Deflecting by magnetic fields only

Abstract

PURPOSE:To make compensation or reduction of coma aberration and G drag at a screen corner part by providing at least one pair of auxiliary coils at the electron gun side of a deflection yoke and at left and right positions inside vertical deflection coils and by allowing an electrical current to flow in the reverse direction to that of the vertical deflecting current. CONSTITUTION:At a location inside a vertical deflection coil 3 and on the electron gun side, at leat one pair of auxiliary coils 15 of a ring shape wound almost on the same curved surface or of a similar shape are provided at left and right of the deflection yoke, and are constituted so that an electrical current reverse to the vertical deflection current flowing in the vertical deflection coils may flow in these auxiliary coils. Namely, wire connection is made in such a way that the direction of magnetic field made by the vertical deflection coils inside the core and on the electron beam side may be reverse to the direction of magnetic field made by the auxiliary coils inside the core and on the electron beam side. Accordingly, both or one of misconvergence caused by coma aberration and G drag can be compensated or reduced with a single deflection yoke.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、テレビジョン受像機等のブラウン管に取付け
て使用する偏向ヨークに関し、特にコマ収差を補正する
偏向ヨークに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a deflection yoke used by being attached to a cathode ray tube of a television receiver, and more particularly to a deflection yoke for correcting coma aberration.

〔↓μ↓〕[↓μ↓]

インライン配列からなる電子銃をそなえたカラーブラウ
ン管に使用するセルフコンバーセンス偏向ヨークでは、
周知のように水平偏向コイルの作る磁界をピンクッショ
ン形磁界に、垂直偏向コイルの作る磁界をバレル形磁界
にすることでコンバーセンス補正を行なっている。上記
のうち、垂直偏向・コイルのバレル形磁界というのは、
第2図に示すように、偏向ヨークの垂直方向の中心線9
付近の巻線が両端部に比較して疎になっているため、中
心に位置1−る緑色(G)用の電子ビーム8は、両端に
位置する赤色(R)。
In the self-convergence deflection yoke used for color cathode ray tubes equipped with in-line electron guns,
As is well known, convergence correction is performed by changing the magnetic field created by the horizontal deflection coil into a pincushion-shaped magnetic field and the magnetic field created by the vertical deflection coil into a barrel-shaped magnetic field. Among the above, the barrel-shaped magnetic field of the vertical deflection coil is:
As shown in FIG. 2, the vertical centerline 9 of the deflection yoke
Since the nearby windings are sparser than those at both ends, the electron beam 8 for green (G) located at the center 1 is for red (R) located at both ends.

青色(B)用の電子ビーム8に比較して実質的に垂直方
向の偏向量が減少することになり、第3図のラスタ・パ
ターンに示すようにGのラスタ12Gは、R/Bに比較
して内側になるいわゆるコマ収差と呼ばれるミスコンバ
ーセンスヲ生シる結果となる。
The amount of vertical deflection is substantially reduced compared to the electron beam 8 for blue (B), and as shown in the raster pattern in FIG. This results in a misconvergence called so-called coma aberration, which moves to the inside.

従来、この種のコマ収差を補正する手段としては、第4
図に示すブラウン管(以下CPTという)19の電子銃
16の先端に、第5図に示すような磁界制御素子14と
呼ばれる磁性体片を配置し5.中心に位置するGの電子
銃付近に偏向磁界を集中させて、Gの偏向量をR/Hに
比較して相対的に増大させる方式が一般に使用されてい
る。
Conventionally, as means for correcting this type of coma aberration, the fourth
A magnetic piece called a magnetic field control element 14 as shown in FIG. 5 is placed at the tip of the electron gun 16 of the cathode ray tube (hereinafter referred to as CPT) 19 shown in the figure.5. A method is generally used in which the deflection magnetic field is concentrated near the G electron gun located at the center to relatively increase the amount of G deflection compared to R/H.

ところで、本方式においては、cprと偏向ヨークとの
組み合せ誤差によって、上記コマ収差が変動する要因が
あり、これは製造上のバラツキとなってあられれる。ま
た、偏向ヨークの作る磁界で偏向されるR/B電子ビー
ムと、上記した磁界制御素子14によりあらかじめ偏向
されたG電子ビームとの偏向中心が異なることに起因す
ると考えられる現象として、第6図の18に示すように
、中央のG電子ビームが画面コーナ部に偏向されるのに
従って、R/B電子ビームに比較して偏向量が減少する
ミスコンバーゼ。
By the way, in this method, there is a factor in which the above-mentioned coma aberration fluctuates due to an error in the combination of the CPR and the deflection yoke, and this may result in manufacturing variations. Furthermore, as a phenomenon that is thought to be caused by the difference in the deflection center of the R/B electron beam deflected by the magnetic field created by the deflection yoke and the G electron beam deflected in advance by the magnetic field control element 14 described above, there is a phenomenon shown in FIG. As shown in 18, as the center G electron beam is deflected to the corner of the screen, the amount of deflection decreases compared to the R/B electron beam.

ンス(以下Gダレという)が発生しており、コンバーゼ
ンス品位の悪化につながっている。
convergence (hereinafter referred to as G-sag), which leads to deterioration of convergence quality.

さて、上記コマ収差0本例では上下方向)を調整する手
段としては、第7図に示すように。
Now, as a means for adjusting the above-mentioned coma aberration (in the vertical direction in this example), as shown in FIG.

偏向ヨーク1の後端部の上下位置に磁性体片20を配置
する方法が公知であるが、この方法では偏向ヨークの作
る垂直偏向磁界を弱める作用しの偏向量を増大させるこ
とはできない。また、上記したように上下方向のコマ収
差は、垂直偏向コイルの中央部、付近の偏向量が小さい
ことに起因するものであるから、この部分に巻線を集中
させればよいわけであるが、このようにすると垂直偏向
コイルの作る磁界全体がピンクッション形磁界の傾向に
変化するため、εスコンノ(−ゼンスを極度に悪化させ
るという欠点が存在する。
Although a method of arranging magnetic pieces 20 above and below the rear end of the deflection yoke 1 is known, this method cannot increase the amount of deflection that weakens the vertical deflection magnetic field produced by the deflection yoke. Furthermore, as mentioned above, the vertical coma aberration is caused by the small amount of deflection in and around the center of the vertical deflection coil, so it would be better to concentrate the windings in this area. If this is done, the entire magnetic field created by the vertical deflection coil changes to a pincushion-shaped magnetic field, which has the disadvantage of extremely worsening the .epsilon.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、上記した従来技術の欠点をなくすため
に、コマ収差を偏向ヨーク単体で補正するか低減すると
ともに、画面コーナ部のGダレについても補正するか低
減する偏向ヨークを実現するための手段を提供すること
にある。
An object of the present invention is to realize a deflection yoke that corrects or reduces coma aberration with the deflection yoke alone, and also corrects or reduces G sag at the corners of the screen, in order to eliminate the drawbacks of the prior art described above. The goal is to provide a means for

〔発明の概要〕[Summary of the invention]

上記目的達成のため1本発明による偏向ヨークは、その
電子銃側で、垂直偏向コイルより内側の左右方向の位置
に、少なくとも1対の補助コイルを設け、これに垂直偏
向電流と逆方向の電流を流すように構成したもので、こ
れにより両端に位置するR/B電子ビームの偏向量を低
減し、相対的に中心に位置するG li、子ビームとの
コ、々収差を補正し、これとともにGダレについても補
正する機能をもたせたものである。
In order to achieve the above object, the deflection yoke according to the present invention is provided with at least one pair of auxiliary coils on the electron gun side at a position in the left and right direction inside the vertical deflection coil, and a current in the direction opposite to the vertical deflection current is applied to the deflection yoke. This reduces the amount of deflection of the R/B electron beams located at both ends, corrects aberrations between the G li and the child beam located relatively at the center, and It also has a function to correct G sag.

〔発明の実施例〕[Embodiments of the invention]

以下1本発明を図に示すセミトロイダル型の偏向ヨーク
(水平偏向コイルはくら型、垂直偏向コイルはトロイダ
ル型)による実施例について説明する。従来の偏向ヨー
ク1の外観は、第1図に示す通りであり、本発明の実施
例による偏向ヨークを第8図に、本発明の要部を示す垂
直偏向コイルの補助コイルの外観を第9図に示す。また
、本発明による偏向ヨークの構成図を第10図に示す。
An embodiment of the present invention using a semi-toroidal type deflection yoke (horizontal deflection coil is hollow type, vertical deflection coil is toroidal type) shown in the drawings will be described below. The appearance of the conventional deflection yoke 1 is as shown in FIG. 1, the deflection yoke according to the embodiment of the present invention is shown in FIG. As shown in the figure. Further, a configuration diagram of the deflection yoke according to the present invention is shown in FIG.

本発明による偏向ヨークの構成は、第10図に示すよう
に、垂直偏向コイル5(コア4)の内側で電子銃側の位
置に略同−曲面内に巻装されたリング形状もしくはこれ
に準する形状の補助−イル15を、偏向ヨークの左右方
向で少なくとも1対設けるもので、これらの補助コイル
は、同図の垂直偏向コイルに流す垂直偏向電流と逆方向
の電流を流すように構成したものである。
As shown in FIG. 10, the deflection yoke according to the present invention has a ring shape or a ring shape wound around the vertical deflection coil 5 (core 4) at a position on the electron gun side within the substantially same curved surface. At least one pair of auxiliary coils 15 each having a shape such as It is something.

すなわち、垂直偏向コイルによってコア内側の電子ビー
ム側に作られる磁界の方向と、補助コイルによってコア
の内側の電子ビーム側に作られる磁界の方向とが、互に
逆向きになるように結線した偏向ヨークである。
In other words, deflection wires are connected so that the direction of the magnetic field created by the vertical deflection coil on the electron beam side inside the core and the direction of the magnetic field created on the electron beam side inside the core by the auxiliary coil are opposite to each other. It's York.

次に、これによる補正原理について説明するよ、。Next, I will explain the principle behind this correction.

まず、本発明による偏向ヨークの断面につ(て、第11
図(但し、垂直偏向コイル部分のみを図示)VCもとす
いて考える。本発明にかかわる。
First, regarding the cross section of the deflection yoke according to the present invention (11th
Figure (however, only the vertical deflection coil portion is shown) VC is also considered. Pertains to the present invention.

補助コイル15は、第11図に示すように垂直偏向コイ
ルの内側に、垂直偏向コイル巻線の両端部の磁界に作用
する位置に設けられる。この補助コイル15は、主偏向
の垂直偏向コイルと逆方向に電流を流すように接続され
ており、その効果としては第11図の偏向力10で示す
ように、垂直偏向コイルによる電子ビーム偏向方向(同
図中のeで表示)と逆方向(同図中のeで表示)に電子
ビームを移動させる効力を有す条。
As shown in FIG. 11, the auxiliary coil 15 is provided inside the vertical deflection coil at a position where it acts on the magnetic field at both ends of the vertical deflection coil winding. This auxiliary coil 15 is connected so that a current flows in the opposite direction to the vertical deflection coil of the main deflection, and its effect is as shown by the deflection force 10 in FIG. A strip that has the effect of moving the electron beam in the opposite direction (indicated by e in the figure) and in the opposite direction (indicated by e in the figure).

そして、この補助コイルは主偏向゛の垂直偏向コイルの
作る偏向磁界に対して、そのコイル両端部付近(すなわ
ち、R/B電子ビーム軌道に影響を与える範曲)で部分
的に作用するように構成しであるから、第11図および
第12図に示すように、補助コイル15の存在する近傍
を通過するR/B電子ビームの偏向量を低減させる働き
を有する。
This auxiliary coil acts partially on the deflection magnetic field created by the main deflection vertical deflection coil near both ends of the coil (in other words, in the range that affects the R/B electron beam trajectory). As shown in FIGS. 11 and 12, this structure has the function of reducing the amount of deflection of the R/B electron beam passing near the auxiliary coil 15.

また、この補助コイル15によるR/B電子ビームの偏
向量を低減させる力は、偏向コイルに電子ビームが接近
するに従って、そのローレンツ力が増加することになる
ので、画面コーナ部に電子ビームが偏向されるに従い、
R/B電子ビームの偏向量はさらに低下する傾向となる
In addition, the Lorentz force of the force that reduces the amount of deflection of the R/B electron beam by the auxiliary coil 15 increases as the electron beam approaches the deflection coil, so the electron beam is deflected toward the corner of the screen. As it is done,
The amount of deflection of the R/B electron beam tends to further decrease.

このため、本発明にかかわる補助コイル15を設けるこ
とにより、第12図に示すように相対的fG電子ビーム
がR/B電子ビームに対して偏向量が増加してコマ収差
17が補正される結果になることと、画面コーナ部にお
いても、R/B電子ビームによるラスタと、G電子ビー
ム(Cよるラスタの差によるGダレ18に関するミスコ
ンバーゼンスが補正される結果になる。(なお、場合に
よっては上記効果により、画面上にバレル形状の偏向歪
が生じることもあるが、これは1、偏向コイルの巻線分
布、マグネット付加などの従来技術により補正可能であ
ることは周知である。) 以上のことから、本発明を実施することにより、第15
図に示すようにコマ収差およびGダレに起因−「るミス
コンバーゼンスの両者もしくは一方を、偏向ヨーク単体
で補正するかあるいは軽減された良好なラスタを得るこ
とができるので、笑用効果の大きい技術手段である。
Therefore, by providing the auxiliary coil 15 according to the present invention, the amount of deflection of the relative fG electron beam with respect to the R/B electron beam increases as shown in FIG. 12, and the coma aberration 17 is corrected. In addition, misconvergence related to G sag 18 due to the difference between the raster caused by the R/B electron beam and the raster caused by the G electron beam (C) is corrected even in the corner areas of the screen. Due to the above effect, barrel-shaped deflection distortion may occur on the screen, but it is well known that this can be corrected by conventional techniques such as 1. winding distribution of the deflection coil and addition of magnets.) Therefore, by implementing the present invention, the 15th
As shown in the figure, the deflection yoke alone can correct or reduce misconvergence caused by comatic aberration and G sag, or both, resulting in a good raster image. It is a means.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、CPT側でのコマ収差補正用の磁界制
御素子を不要化もしくは簡略化するとともに、Gダレお
よびCPTと偏向ヨークとの組合せ誤差によるコマ収差
変化などに起因するミスコンバーゼンスを低減化するこ
とができるので、実用上有効な手段となり得る。
According to the present invention, the magnetic field control element for coma aberration correction on the CPT side is not required or simplified, and misconvergence caused by changes in coma aberration due to G sag and combination errors between the CPT and the deflection yoke is reduced. It can be a practically effective means.

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

第1図は、従来の偏向ヨークの斜視図、第2図は、垂直
偏向コイルの断面図、第3図は、コマ収差を表わす説明
図、第4図は、偏向ヨークと電子銃の位置関係を示す説
明図、第5図は、従来の(、’ F T電子銃付近に設
ける磁界制御素子を示す説明図、第6図は、磁界制御素
子によるコマ収差補正後のミスコンバーゼンスのパター
ン図、第70図は、従来のコマ収差謂整機能をもつ偏向
ヨークの斜視図、第8図(alは、本発明による偏向ヨ
ークの平面図、第8図(blは、(α)の偏向ヨークの
正面図、第9図は、本発明の要部である補助コイルの斜
視図、第10図は、本発明による偏向ヨークの構成展開
図、第11図は、第8図の垂直偏向コイルと補助コイル
の背面図、第12図は1本発明の補助コイルによる横線
ラスタの変化を示すパターン図、第13図は、本発明を
実施した場合のミスコンバーゼンスのパターン図である
。 1!偏向ヨーク、2:水平偏向コイル、31垂直偏向コ
イル、4+コア、5Iセパレータ(モールド品)、6ト
クリツプ、7;垂直偏向の磁力線、8:電子ビーム、9
:垂直方向の中心線(Y軸)、 10 +偏向力、11
iC’7’Tの画面、12゜IR,G、B横線ラスタ、
151を子銃本体、14:磁界制御素子、15;補助コ
イル、16を水平方向17)中心線(X軸)、17sコ
−r収差、181Gダレ成分、19:CPT、20+磁
性体片、21:偏向ヨークの中心線。 手  1  図 斗  2 図    羊 3 図 4−4図   羊5図 早 8 図 羊 /θ 図 手  〃  図
Figure 1 is a perspective view of a conventional deflection yoke, Figure 2 is a sectional view of a vertical deflection coil, Figure 3 is an explanatory diagram showing coma aberration, and Figure 4 is the positional relationship between the deflection yoke and the electron gun. FIG. 5 is an explanatory diagram showing a magnetic field control element provided near the conventional (, F T electron gun), FIG. 6 is a pattern diagram of misconvergence after coma aberration correction by the magnetic field control element, FIG. 70 is a perspective view of a conventional deflection yoke having a coma aberration adjustment function, FIG. 8 (al is a plan view of the deflection yoke according to the present invention, and FIG. 9 is a perspective view of the auxiliary coil, which is the main part of the present invention, FIG. 10 is a developed view of the structure of the deflection yoke according to the present invention, and FIG. 11 is the vertical deflection coil of FIG. 8 and the auxiliary coil. FIG. 12 is a rear view of the coil, FIG. 12 is a pattern diagram showing changes in the horizontal line raster due to the auxiliary coil of the present invention, and FIG. 13 is a pattern diagram of misconvergence when the present invention is implemented. 1! Deflection yoke, 2: Horizontal deflection coil, 31 Vertical deflection coil, 4+ core, 5I separator (molded product), 6 Toclip, 7; Vertical deflection magnetic field line, 8: Electron beam, 9
: Vertical center line (Y axis), 10 + deflection force, 11
iC'7'T screen, 12°IR, G, B horizontal line raster,
151 is the secondary gun body, 14: magnetic field control element, 15; auxiliary coil, 16 is the horizontal direction 17) center line (X axis), 17s Co-r aberration, 181G sagging component, 19: CPT, 20 + magnetic piece, 21 : Center line of deflection yoke. Hand 1 Figure 2 Figure Sheep 3 Figure 4-4 Figure Sheep 5 Figure Haya 8 Figure Sheep /θ Figure Hand 〃 Figure

Claims (1)

【特許請求の範囲】[Claims] 1、 偏向ヨークの電子銃側で、垂直偏向コイルより内
側の左右方向の位置に、垂直偏向コイルの導体とほぼ平
行に巻線された部分をもつリング形状もしくはこれに準
する形状を有する補助コイルを少なくとも1対設け、こ
れに垂直偏向電流と逆方向の電流を流すように構成した
ことを特徴とする偏向ヨーク。
1. On the electron gun side of the deflection yoke, an auxiliary coil having a ring shape or a similar shape with a portion wound approximately parallel to the conductor of the vertical deflection coil at a position in the left and right direction inside the vertical deflection coil. 1. A deflection yoke characterized in that at least one pair of yoke are provided, and a current in a direction opposite to the vertical deflection current is passed through the yoke.
JP6553583A 1983-04-15 1983-04-15 Deflection yoke Pending JPS59191238A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6553583A JPS59191238A (en) 1983-04-15 1983-04-15 Deflection yoke

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6553583A JPS59191238A (en) 1983-04-15 1983-04-15 Deflection yoke

Publications (1)

Publication Number Publication Date
JPS59191238A true JPS59191238A (en) 1984-10-30

Family

ID=13289802

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6553583A Pending JPS59191238A (en) 1983-04-15 1983-04-15 Deflection yoke

Country Status (1)

Country Link
JP (1) JPS59191238A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4943753A (en) * 1987-08-13 1990-07-24 International Business Machines Corporation Magnetic shunt for deflection yokes
KR20030018195A (en) * 2001-08-27 2003-03-06 (주)올링스미디어 deflection yoke device for a color cathode ray tube with an improved definition and a constant brightness characteristics in a screen corner
KR20030071121A (en) * 2002-02-27 2003-09-03 엘지.필립스디스플레이(주) Deflection York for C-CRT
KR100393388B1 (en) * 1994-07-01 2003-10-17 톰슨 튜브 앤드 디스플레이 에스. 에이. Secondary Coil Fasteners in Deflection Yoke

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4943753A (en) * 1987-08-13 1990-07-24 International Business Machines Corporation Magnetic shunt for deflection yokes
KR100393388B1 (en) * 1994-07-01 2003-10-17 톰슨 튜브 앤드 디스플레이 에스. 에이. Secondary Coil Fasteners in Deflection Yoke
KR20030018195A (en) * 2001-08-27 2003-03-06 (주)올링스미디어 deflection yoke device for a color cathode ray tube with an improved definition and a constant brightness characteristics in a screen corner
KR20030071121A (en) * 2002-02-27 2003-09-03 엘지.필립스디스플레이(주) Deflection York for C-CRT

Similar Documents

Publication Publication Date Title
JP2993957B2 (en) Device for correcting deflection yoke misconvergence and geometric distortion
US4041428A (en) Deflection yoke for use with in-line cathode ray tubes
US4882521A (en) Deflection yoke for a color cathode ray tube
JPS59191238A (en) Deflection yoke
JPS6039742A (en) Deflection yoke
JPS6029183B2 (en) deflection yoke
US4933596A (en) Deflection yoke with compensation for misconvergence by the horizontal center raster
JP3390761B2 (en) Deflection device
JPS5933153Y2 (en) deflection yoke
JPH0723405A (en) Electromagnetic deflection yoke for color cathode ray tube
JPS59171437A (en) Deflection yoke
JP2656591B2 (en) Deflection device and deflection yoke constituting the same
JPH035079Y2 (en)
JP2001101983A (en) Color picture tube device
JPS59184439A (en) Deflection yoke
JPH0359931A (en) Deflection yoke for color television picture tube
JP3500163B2 (en) Deflection device for color picture tube
JPS6223422B2 (en)
JPH0138353B2 (en)
JPS6028036Y2 (en) deflection yoke
JPS61230244A (en) Convergence correction device
JPS6318836B2 (en)
KR810001808B1 (en) Deflection yoke device for use in color television reciever sets
JPS59171435A (en) Deflection yoke
JPH02267840A (en) Deflection yoke structure