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JPH022262B2 - - Google Patents

Info

Publication number
JPH022262B2
JPH022262B2 JP58055051A JP5505183A JPH022262B2 JP H022262 B2 JPH022262 B2 JP H022262B2 JP 58055051 A JP58055051 A JP 58055051A JP 5505183 A JP5505183 A JP 5505183A JP H022262 B2 JPH022262 B2 JP H022262B2
Authority
JP
Japan
Prior art keywords
horizontal
screen
coil
misconvergence
deflection
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
JP58055051A
Other languages
Japanese (ja)
Other versions
JPS59184439A (en
Inventor
Masao Obara
Yoshiichi Naito
Ichiro Niitsu
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 JP5505183A priority Critical patent/JPS59184439A/en
Publication of JPS59184439A publication Critical patent/JPS59184439A/en
Publication of JPH022262B2 publication Critical patent/JPH022262B2/ja
Granted 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

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明はインライン形カラー受像管に用いる偏
向ヨークに関するもので、特にインライン形カラ
ー受像管の残留ミスコンバージエンスを最適化す
る手段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 for use in an in-line color picture tube, and more particularly to means for optimizing residual misconvergence in an in-line color picture tube.

〔従来技術〕[Prior art]

従来の偏向ヨークでは、水平コイル、垂直コイ
ルの巻線分布調整のみでは画面全域における残留
ミスコンバージエンスを零にできず第2図の様な
残留ミスコンバージエンスパターンとなつてい
た。従来技術により、つまり水平コイル、垂直コ
イルの巻線分布調整により第2図における画面中
間部3Bの赤ビームと青ビームのY方向ずれ量
(横線ずれ量)を零にすると、画面周辺部3Cの
赤ビームと青ビームのY方向ずれ量(横線ずれ
量)が第8図の如くなる。又逆に画面周辺部3C
の赤ビームと青ビームのY方向ずれ量(横線ずれ
量)を零にすると、画面中間部3Bの赤ビームと
青ビームのY方向ずれ量(横線ずれ量)が第2図
の如くなる。つまり従来技術においては、水平コ
イル、垂直コイルの巻線分布調整によつてこの関
係を改善できないという欠点があつた。
In the conventional deflection yoke, the residual misconvergence over the entire screen could not be reduced to zero simply by adjusting the winding distribution of the horizontal and vertical coils, resulting in a residual misconvergence pattern as shown in FIG. By using the conventional technology, that is, by adjusting the winding distribution of the horizontal coil and the vertical coil, if the amount of deviation in the Y direction (the amount of deviation in the horizontal line) between the red beam and the blue beam in the middle part 3B of the screen in FIG. The amount of deviation in the Y direction (the amount of horizontal line deviation) between the red beam and the blue beam is as shown in FIG. On the other hand, the peripheral area of the screen 3C
When the amount of deviation in the Y direction (the amount of deviation in horizontal lines) between the red beam and the blue beam is set to zero, the amount of deviation in the Y direction (the amount of deviation in horizontal lines) between the red beam and the blue beam in the middle part 3B of the screen becomes as shown in FIG. In other words, the conventional technology has the disadvantage that this relationship cannot be improved by adjusting the winding distribution of the horizontal coil and the vertical coil.

〔発明の目的〕[Purpose of the invention]

本発明の目的はインライン形カラー受像管に用
いる偏向ヨークにおいて、インライン形カラー受
像管の画面上の全域における残留ミスコンバージ
エンスを設計的にほぼ零にし(特に画面周辺部と
画面中間部の赤ビームと青ビームの横線ずれ量を
零にする)、良質な画質のカラー受像管を提供す
る事にある。
The purpose of the present invention is to design a deflection yoke used in an in-line color picture tube to almost eliminate the residual misconvergence in the entire area on the screen of the in-line color picture tube (particularly to reduce the red beam at the periphery of the screen and the middle part of the screen). The goal is to provide a color picture tube with high image quality, which reduces the amount of horizontal line deviation of the blue beam to zero).

〔発明の概要〕[Summary of the invention]

本発明は前述した目的を達成する為偏向ヨーク
を構成する鞍形水平コイルについて、従来技術に
おいて巻線の施されていない窓部で、かつ画面側
開口部と電子銃側開口部の中間部に水平偏向軸に
対して約54゜から90゜の領域に補助水平コイルを配
置し、主水平偏向磁界と同方向の磁界を形成する
様水平偏向電流を流し、画面上下のラスター歪を
悪化させる事なく、画面の周辺部3Cと画面の中
間部3Bの赤ビームと青ビームのミスコンバージ
エンスずれをほぼ零とし、かつ画面全域にわたつ
て最良なミスコンバージエンスを得るようにした
ものである。
In order to achieve the above-mentioned object, the present invention provides a saddle-shaped horizontal coil constituting a deflection yoke in a window portion where no winding is provided in the prior art, and in an intermediate portion between an opening on the screen side and an opening on the electron gun side. An auxiliary horizontal coil is placed in the area approximately 54° to 90° with respect to the horizontal deflection axis, and a horizontal deflection current is applied to form a magnetic field in the same direction as the main horizontal deflection magnetic field, thereby worsening raster distortion at the top and bottom of the screen. In addition, the misconvergence difference between the red beam and the blue beam in the peripheral area 3C of the screen and the middle area 3B of the screen is made almost zero, and the best misconvergence is obtained over the entire screen.

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

以下本発明の一実施例を説明する。 An embodiment of the present invention will be described below.

第1図が従来の偏向ヨークで第3図が本発明に
よる偏向ヨークである。本発明による偏向ヨーク
を構成する鞍形水平コイル1,1′の画面側開口
部と電子銃側開口部の管軸方向中間部の窓部(主
水平コイル巻線が施されていない部分)には補助
水平コイル4,4′を配置してある。補助水平コ
イル4,4′の正面図を第5図に、本発明による
偏向ヨークの管軸方向断面図を第6図に示す。本
発明による補助コイル4,4′は第6図に示す如
く水平コイル1,1′垂直コイル6間の絶縁物セ
パレーター2を介してセパレーター2の小内径側
内面に係止してある。またこの補助コイル4,
4′は水平方向偏向軸x軸に対して、本実施例で
は画面開口部側で70゜、電子銃開口部側で87゜の領
域に巻線を行ない、第7図に示す如く主水平偏向
磁界発生用の水平コイル1,1′と直列に接続さ
れている。
FIG. 1 shows a conventional deflection yoke, and FIG. 3 shows a deflection yoke according to the present invention. In the window portion (portion where the main horizontal coil winding is not applied) at the center in the tube axis direction between the screen-side opening and the electron gun-side opening of the saddle-shaped horizontal coils 1, 1' constituting the deflection yoke according to the present invention. Auxiliary horizontal coils 4, 4' are arranged. FIG. 5 is a front view of the auxiliary horizontal coils 4, 4', and FIG. 6 is a sectional view of the deflection yoke according to the present invention in the tube axis direction. As shown in FIG. 6, the auxiliary coils 4, 4' according to the present invention are secured to the inner surface of the small inner diameter side of the separator 2 via the insulating separator 2 between the horizontal coils 1, 1' and the vertical coil 6. In addition, this auxiliary coil 4,
4' is a horizontal deflection axis. In this example, the winding is performed in an area of 70 degrees on the screen opening side and 87 degrees on the electron gun opening side with respect to the horizontal deflection axis x-axis, and the main horizontal deflection is as shown in FIG. It is connected in series with horizontal coils 1 and 1' for generating magnetic fields.

従来の偏向ヨークの受像管画面上でのミスコン
バージエンスパターンは第2図に示す如く画面中
間部3Bの赤ビームと青ビームとのY方向ずれ量
(横線ミスコンバージエンス)が14インチサイズ
のインライン形受像管においては約0.3から0.4mm
残留ミスコンバージエンスとして残つている。
The conventional deflection yoke's misconvergence pattern on the picture tube screen is as shown in Figure 2, where the amount of Y-direction deviation (horizontal line misconvergence) between the red beam and the blue beam at the middle part 3B of the screen is inline with a size of 14 inches. Approximately 0.3 to 0.4 mm for picture tubes
It remains as a residual misconvergence.

このミスコンバージエンスを減らすため、水平
コイルの巻線分布によるミスコンバージエンスの
動きを調べた結果、画面周辺部3Cでの赤ビーム
に対する青ビームのy方向変化量を△y3C、画面
中間部3Bでの赤ビームに対する青ビームのy方
向変化量を△y3Bとし、その変化率αをα=
△y3B/△y3Cとすると、第12図に示す如く従来の水平 コイルのように水平偏向軸x軸に対して約30゜か
ら約54゜(本実施例では45゜)の領域に水平コイル
巻線を施すと、第11図に示す如く、x軸方向離
軸距離xに対する、本水平コイル巻線によるx軸
方向磁束密度Bxは第11図の如くなつており、
この場合にはαが0.2〜0.3(本実施例では約0.25)
である。このαの値で第2図における画面中間部
3Bのy方向ずれ量(横線ミスコンバージエン
ス)を零にすれば、画面周辺部3Cで第8図の如
く約1.2〜1.6mmのミスコンバージエンスずれとな
る。ところが本実施例の補助水平コイル4,4′
を第10図に示す如く水平偏向軸x軸に対して、
約54゜から90゜(本実施例では70゜)の領域に補助水
平コイル巻線を施すと、第9図に示す如くx軸方
向離軸距離xに対する、本補助水平コイル巻線に
よるx軸方向磁束密度Bxは第11図の場合と異
なり離軸距離xが増大するに従つてx軸方向磁束
密度Bxの増加率が減少する為αが0.5〜0.9(本実
施例では約0.8)となり、第2図における画面中
間部3Bのy方向ずれ量(横線ミスコンバージエ
ンス)を零にすれば画面周辺部3Cのy方向ずれ
量(横線ミスコンバージエンス)は約0.38〜0.5
mmのミスコンバージエンスずれとなり、従来偏向
ヨークの約1/3の残留ミスコンバージエンスとな
り、大幅に改善される。本実施例においては、
14″90゜インライン形カラー受像管の場合補助水平
コイルの巻数を20ターン(主水平コイル130ター
ン)とし画面開口部側巻線角度70゜、電子銃開口
部側巻線角度87゜とし、補助水平コイル長さを22
mm(主水平コイル74.5mm)とし、鞍形水平コイル
の画面開口部側と電子銃開口部側の中間部の窓部
に配置し、主水平コイル、垂直コイルと組合せて
第4図の様なほぼミスコンバージエンスずれのな
い高画質が得られた。
In order to reduce this misconvergence, as a result of investigating the movement of misconvergence due to the winding distribution of the horizontal coil, we found that the amount of change in the y direction of the blue beam relative to the red beam at the screen periphery 3C is Δy 3C , and the amount of change in the y direction of the blue beam relative to the red beam at the screen periphery 3C is 3B The amount of change in the y direction of the blue beam relative to the red beam at is △y 3B , and the rate of change α is α=
Assuming △y 3B / △y 3C , as shown in Fig. 12, a horizontal coil is applied horizontally in an area of about 30° to about 54° (45° in this example) with respect to the horizontal deflection axis x-axis, as in the conventional horizontal coil. When the coil winding is applied, the magnetic flux density B x in the x-axis direction due to the horizontal coil winding is as shown in FIG. 11, with respect to the off-axis distance x in the x-axis direction, as shown in FIG.
In this case, α is 0.2 to 0.3 (approximately 0.25 in this example)
It is. If the y-direction shift amount (horizontal line misconvergence) of the screen middle part 3B in FIG. 2 is made zero with this value of α, the misconvergence shift of about 1.2 to 1.6 mm will occur in the screen peripheral part 3C as shown in FIG. becomes. However, the auxiliary horizontal coils 4, 4' of this embodiment
As shown in Fig. 10, with respect to the horizontal deflection axis x-axis,
When the auxiliary horizontal coil winding is applied in the area from about 54° to 90° (70° in this example), the x-axis due to the auxiliary horizontal coil winding is The directional magnetic flux density B x differs from the case in FIG. 11 because the rate of increase in the x-axis direction magnetic flux density B x decreases as the off-axis distance x increases, so α is 0.5 to 0.9 (approximately 0.8 in this example). Therefore, if the amount of deviation in the y direction (horizontal line misconvergence) of the screen middle part 3B in FIG.
The misconvergence deviation is approximately 1/3 of that of the conventional deflection yoke, which is a significant improvement. In this example,
For a 14″90° in-line color picture tube, the number of turns of the auxiliary horizontal coil is 20 turns (main horizontal coil 130 turns), the winding angle on the screen opening side is 70°, the winding angle on the electron gun opening side is 87°, and the auxiliary horizontal coil length 22
mm (main horizontal coil 74.5 mm), placed in the window between the screen opening side of the saddle-shaped horizontal coil and the electron gun opening side, and combined with the main horizontal coil and vertical coil as shown in Figure 4. High image quality with almost no misconvergence deviation was obtained.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、インライン形カラー受像管の
画面周辺部3Cに対する画面中間部3Bの赤ビー
ムと青ビームのy方向ミスコンバージエンス変化
量を増大させ、かつ補助水平コイルの巻数、形
状、及び水平コイル、垂直コイルの巻線分布を調
整する事により、画面中間部3B及び画面周辺部
3Cのy方向ずれ(横線ミスコンバージエンス)
をほぼ零にでき、かつ画面全域における残留ミス
コンバージエンスを大幅に小さくできる。故にミ
スコンバージエンス許容範囲内で受像管、偏向ヨ
ークのばらつきを吸収でき、しかもコンバージエ
ンス調整時間の短縮、製造コストの低減等多大な
効果があり、ミスコンバージエンス仕様の厳しい
デイスプレー装置への対応ができる。
According to the present invention, the amount of change in misconvergence in the y direction of the red beam and blue beam of the screen middle portion 3B relative to the screen peripheral portion 3C of an in-line color picture tube is increased, and the number of turns, shape, and horizontal direction of the auxiliary horizontal coil are increased. By adjusting the winding distribution of the coil and vertical coil, the deviation in the y direction of the screen middle part 3B and the screen peripheral part 3C (horizontal line misconvergence)
can be reduced to almost zero, and residual misconvergence over the entire screen can be significantly reduced. Therefore, variations in the picture tube and deflection yoke can be absorbed within the misconvergence tolerance range, and it has great effects such as shortening convergence adjustment time and manufacturing costs, making it suitable for display equipment with strict misconvergence specifications. Can be done.

【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画面開口部側から
見た正面図、第2図は従来の偏向ヨークとインラ
イン形カラー受像管を組み合わせた場合の画面上
のミスコンバージエンスパターン図、第3図は本
発明による偏向ヨークの画面開口部側より見た正
面図、第4図は本発明による偏向ヨークとインラ
イン形カラー受像管を組み合わせた場合の画面上
のミスコンバージエンスパターン図、第5図は本
発明による補助コイルの正面図、第6図は本発明
による偏向ヨークの管軸方向断面図、第7図は本
発明による補助コイルと水平コイルの結線図、第
8図は従来の偏向ヨークのミスコンバージエンス
パターン図、第9図は水平偏向軸に対して約70゜
の位置のみに水平コイルを配置した場合の離軸距
離に対する水平偏向軸方向磁束密度Bxとの関係
図、第10図は水平偏向軸に対して約70゜の位置
に水平コイルを配置した場合の管軸方向断面図、
第11図は水平偏向軸に対して約45゜の位置のみ
に水平コイルを配置した場合の離軸距離に対する
水平偏向軸方向磁束密度Bxとの関係図、第12
図は水平偏向軸に対して約45゜の位置に水平コイ
ルを配置した場合の管軸方向断面図である。 1,1′……主水平コイル、2……セパレータ、
3C……画面周辺部、3B……画面中間部、R…
…赤ビームラスタ、B……青ビームラスタ、4,
4′……補助水平コイル、5……コア、6……垂
直コイル。
Figure 1 is a front view of a conventional deflection yoke viewed from the screen opening side, Figure 2 is a diagram of the misconvergence pattern on the screen when a conventional deflection yoke is combined with an in-line color picture tube, and Figure 3 4 is a front view of the deflection yoke according to the present invention as seen from the screen opening side, FIG. 4 is a diagram showing the misconvergence pattern on the screen when the deflection yoke according to the present invention and an in-line color picture tube are combined, and FIG. FIG. 6 is a front view of the auxiliary coil according to the present invention, FIG. 6 is a sectional view in the tube axis direction of the deflection yoke according to the present invention, FIG. 7 is a connection diagram of the auxiliary coil and horizontal coil according to the present invention, and FIG. Misconvergence pattern diagram, Figure 9 is a diagram of the relationship between the horizontal deflection axial magnetic flux density B x and the off-axis distance when the horizontal coil is placed only at a position of about 70 degrees with respect to the horizontal deflection axis, Figure 10 is a cross-sectional view in the tube axis direction when the horizontal coil is placed at a position of approximately 70° with respect to the horizontal deflection axis.
Figure 11 is a diagram of the relationship between the horizontal deflection axial magnetic flux density B
The figure is a cross-sectional view in the tube axis direction when the horizontal coil is placed at a position of approximately 45 degrees with respect to the horizontal deflection axis. 1, 1'... Main horizontal coil, 2... Separator,
3C...peripheral area of the screen, 3B...middle area of the screen, R...
...Red beam raster, B...Blue beam raster, 4,
4'...Auxiliary horizontal coil, 5...Core, 6...Vertical coil.

Claims (1)

【特許請求の範囲】[Claims] 1 インライン形電子銃を配置したカラー受像管
に用いる鞍形水平コイルを具備している偏向ヨー
クにおいて、鞍形水平コイルの画面側開口部と電
子銃側開口部の中間部の窓部に補助水平コイルを
配置し、この補助水平コイルを、主水平コイルの
作る主磁界発生方向と同方向の偏向磁界を発生す
る様、主水平コイルと直列に接続し、かつ主水平
コイルと同方向の偏向電流を流す様にした事を特
徴とする偏向ヨーク。
1. In a deflection yoke equipped with a saddle-shaped horizontal coil used in a color picture tube with an in-line electron gun, an auxiliary horizontal The auxiliary horizontal coil is connected in series with the main horizontal coil so as to generate a deflection magnetic field in the same direction as the main magnetic field generated by the main horizontal coil, and the deflection current is in the same direction as the main horizontal coil. A deflection yoke that is characterized by being made to flow.
JP5505183A 1983-04-01 1983-04-01 Deflection yoke Granted JPS59184439A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5505183A JPS59184439A (en) 1983-04-01 1983-04-01 Deflection yoke

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5505183A JPS59184439A (en) 1983-04-01 1983-04-01 Deflection yoke

Publications (2)

Publication Number Publication Date
JPS59184439A JPS59184439A (en) 1984-10-19
JPH022262B2 true JPH022262B2 (en) 1990-01-17

Family

ID=12987871

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5505183A Granted JPS59184439A (en) 1983-04-01 1983-04-01 Deflection yoke

Country Status (1)

Country Link
JP (1) JPS59184439A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2689679A1 (en) * 1992-04-07 1993-10-08 Thomson Tubes & Displays Device for deflecting electron beams for self-converging cathode ray tubes and corrected in geometry.
TW270998B (en) * 1992-04-17 1996-02-21 Toshiba Co Ltd
KR100376994B1 (en) * 2000-06-24 2003-03-26 삼성전기주식회사 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

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6030058B2 (en) * 1978-01-17 1985-07-13 ソニー株式会社 deflection device

Also Published As

Publication number Publication date
JPS59184439A (en) 1984-10-19

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