JPH01255136A - Convergence correcting device of cathode-ray tube - Google Patents

Convergence correcting device of cathode-ray tube

Info

Publication number
JPH01255136A
JPH01255136A JP8267388A JP8267388A JPH01255136A JP H01255136 A JPH01255136 A JP H01255136A JP 8267388 A JP8267388 A JP 8267388A JP 8267388 A JP8267388 A JP 8267388A JP H01255136 A JPH01255136 A JP H01255136A
Authority
JP
Japan
Prior art keywords
ring
magnet
magnetic substance
fitting
correction
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
JP8267388A
Other languages
Japanese (ja)
Inventor
Fumio Abe
阿部 文夫
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP8267388A priority Critical patent/JPH01255136A/en
Publication of JPH01255136A publication Critical patent/JPH01255136A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To provide effective correction of a deflecting mag. field and enhance the working easiness in fitting and removal of a magnetic substance ring by fitting the magnetic substance ring in a ring shaped groove provided at the surface of a stop ring on a CP magnet. CONSTITUTION:A ring-shaped groove 24 is furnished to fit a magnetic substance ring 23 at the surface of stop rings 15a, 15b of a CP magnet 10 for convergence adjustment of a convergence correcting device. The inner dia. RA of this ring- shaped groove 24 is identical the inner dia. RA of the magnetic substance ring 23, while the outside dia. RB of the former 24 is greater than the outside dia. RC of the latter 23. When the ring 23 is to be mounted, therefore, fixation is attained without eccentricity from the center of the CP magnet 10. It is not required at this time to remove once the stop ring 15a and conceal in the CP magnet for performing fitting, but direct fitting can be made to the surface of the stop ring 15a. Accordingly the vertically deflecting mag. field 22 with the deflection yoke 9 varied is free from asymmetrical correction, and correction to the normal vertical deflecting mag. filed 20 is possible, and further installation at the time of correction becomes easy.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、カラーブラウン管のネック部に設けられる
コンバーゼンス補正装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a convergence correction device provided in the neck of a color cathode ray tube.

〔従来の技術〕[Conventional technology]

第2図に従来のカラーブラウン管の構成図を示す。図に
おいて、1は陰極線管となるカラーブラウン管で、内面
に蛍光体膜2を有する。3はブラウン管のパネル、4は
このパネル3に接続された漏斗状のファンネル、5(よ
ネック部である。6は複数本の電子線を発生する電子銃
で、ネック部5内に配置されている。7は電子銃6を動
作させるための電圧を供給するベース、8は電子銃6か
ら発射する電子ビームを蛍光体膜2を形成する各色に発
光する蛍光体に選択的に衝突させるシャドウマスク、9
は電子ビームを必要部分に偏向させる偏向ヨークである
。10はコンバーゼンス調整用磁石(以下CP磁石とい
う)であり、電子銃6を取囲むようにネック部5に装着
されている。
FIG. 2 shows a configuration diagram of a conventional color cathode ray tube. In the figure, numeral 1 is a color cathode ray tube, which is a cathode ray tube, and has a phosphor film 2 on its inner surface. 3 is a panel of a cathode ray tube, 4 is a funnel-shaped funnel connected to this panel 3, and 5 is a neck part. 6 is an electron gun that generates multiple electron beams, which is placed inside the neck part 5. 7 is a base that supplies voltage to operate the electron gun 6, and 8 is a shadow mask that selectively causes the electron beam emitted from the electron gun 6 to collide with the phosphors that emit light in each color forming the phosphor film 2. ,9
is a deflection yoke that deflects the electron beam to the required part. Reference numeral 10 denotes a convergence adjustment magnet (hereinafter referred to as a CP magnet), which is attached to the neck portion 5 so as to surround the electron gun 6.

第3図はCP磁石10の拡大図を示し、ila。FIG. 3 shows an enlarged view of the CP magnet 10, ila.

11bは2極磁石、12 a、  12 bは4極磁石
、13n、13bは6攪磁石である。14a〜14dは
磁石相互間に介在したスペーサで、止めリング15a、
15bで両端を締付けることにより、各磁石の回転を防
止している。16はCP磁石10をネック部5に固定す
るためのねじである。
11b is a two-pole magnet, 12a and 12b are four-pole magnets, and 13n and 13b are six-stirring magnets. 14a to 14d are spacers interposed between the magnets, and retaining rings 15a,
Rotation of each magnet is prevented by tightening both ends with 15b. 16 is a screw for fixing the CP magnet 10 to the neck portion 5.

次にa作について説明する。パネル3」二で画像を出す
ためには電子銃6から発射した電子ビームを偏向ヨーク
9で偏向させ、シャドウマスク8の孔を通して定められ
た蛍光体膜2上の蛍光体に正しく当てなければならない
。上3aQ向ヨーク9は第4図に示すように水平偏向コ
イル17と垂直偏向コイル18とからなり、垂直偏向コ
イル18はコア19を伴ったトロイダル状に形成されて
いる。
Next, work a will be explained. In order to produce an image on the panel 3'', the electron beam emitted from the electron gun 6 must be deflected by a deflection yoke 9, and must pass through the hole in the shadow mask 8 and correctly hit the phosphor on the phosphor film 2. . The upper 3aQ direction yoke 9 is composed of a horizontal deflection coil 17 and a vertical deflection coil 18, as shown in FIG. 4, and the vertical deflection coil 18 is formed in a toroidal shape with a core 19.

また垂直偏向コイル18はその構造上、電子ビームを垂
直に偏向させるための磁界以外にも偏向ヨーク9の外部
にも漏れ磁界を発生し、かつ外部の環境からも影響を受
けやすい。この−例としては第4図に示すように通常の
垂直偏向磁界20が外部からの影響を受け、変化した垂
直偏向磁界22となる。これによって、電子ビームは蛍
光体膜2上の蛍光体に正しく当たらない。
Further, due to its structure, the vertical deflection coil 18 generates a leakage magnetic field outside the deflection yoke 9 in addition to the magnetic field for vertically deflecting the electron beam, and is easily influenced by the external environment. As an example of this, as shown in FIG. 4, a normal vertical deflection magnetic field 20 is influenced by an external source, resulting in a changed vertical deflection magnetic field 22. As a result, the electron beam does not correctly hit the phosphor on the phosphor film 2.

また、第4図の変化した垂直偏向磁界22を通常の偏向
磁界20に補正する手段の1つとして、第5図に示すよ
うな磁性体のリング23を第3図に示すCP磁石10の
止めリング15aとスペーサ14aまたはスペーサ14
aと2極磁石11aの間、あるいは止めリング15a、
15b1スペーサ14 a 〜14 d、 241磁石
11a、llb。
Furthermore, as one means for correcting the changed vertical deflection magnetic field 22 shown in FIG. 4 to the normal deflection magnetic field 20, a magnetic ring 23 as shown in FIG. Ring 15a and spacer 14a or spacer 14
a and the two-pole magnet 11a, or the retaining ring 15a,
15b1 spacers 14a to 14d, 241 magnets 11a, llb.

4極磁石12 a、  12 b、 64%磁石13a
、13bのいずれかの間に押入し、止めリング15a、
15bで締付は固定する方法がある。
4-pole magnet 12a, 12b, 64% magnet 13a
, 13b, a retaining ring 15a,
There is a method of fixing the tightening with 15b.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来のコンバーゼンス補正装置によれば、例えば第7図
に示すようにCPli1石10内に磁性体リング23が
隠れて固定されるので、その取付は状態が傷心し、垂直
偏向磁界に非対称性が生じたり、磁性体リング23を取
付ける際に一度止めリング15aを外して再び固定する
など組立て作業性に問題があった。
According to the conventional convergence correction device, for example, as shown in FIG. 7, the magnetic ring 23 is hidden and fixed within the CPli 1 stone 10, so the installation is unstable and asymmetry occurs in the vertical deflection magnetic field. Also, when attaching the magnetic ring 23, the retaining ring 15a must be removed once and then fixed again, resulting in problems in assembly workability.

この発明は上記のような課題を解消するためになされた
もので、カラーブラウン管の偏向磁界を有効に補正する
ことのできろコンバーゼンス補正装置を得ることを目的
とする。
The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide a convergence correction device that can effectively correct the deflection magnetic field of a color cathode ray tube.

〔課題を解決するための手段〕[Means to solve the problem]

この発明に係るコンバーゼンス補正装置は、CPPb0
止めリングの表面に磁性体リングを装着するための環状
溝を形成したものである。
The convergence correction device according to the present invention has CPPb0
An annular groove for mounting a magnetic ring is formed on the surface of the retaining ring.

〔作 用〕[For production]

この発明においては、止めリングに形成した環状溝に磁
性体リングを装着するようにしたので、偏向磁界を補正
する際、非対称な補正を防止できると共に、磁性体リン
グの環状溝に対する着脱作業が容易に行なえろ。
In this invention, since the magnetic ring is attached to the annular groove formed in the retaining ring, it is possible to prevent asymmetric correction when correcting the deflection magnetic field, and it is easy to attach and detach the magnetic ring to and from the annular groove. Go to.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明する。第1
図はこの発明によるコンバーゼンス補正装置の斜視図を
示し、10はCPPb0あって、24は止めリング15
aの表面に形成した環状溝で、この環状溝24に磁性体
リング23を装着したものである。ここで、環状溝24
の内径RAは磁性体リング23の内径RAと一致し、し
かも環状溝24の外径RBは磁性体リング23の外径R
cより大きくし、その大きさは限定しない。
An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure shows a perspective view of the convergence correction device according to the invention, in which 10 is a CPPb0, 24 is a retaining ring 15
This is an annular groove formed on the surface of a, and a magnetic ring 23 is attached to this annular groove 24. Here, the annular groove 24
The inner diameter RA of the annular groove 24 matches the inner diameter RA of the magnetic ring 23, and the outer diameter RB of the annular groove 24 matches the outer diameter R of the magnetic ring 23.
c, and its size is not limited.

この発明においては、磁性体リング23の内径RAと環
状溝24の内径RAは一致するため、リング23の取付
けの際はCP磁石10の中心から偏心することな(固定
できる。また、リング23を取付ける際は例又は止めリ
ング15aを一度取外し、CP磁石10の内部に隠して
装入する必要はなく、止めリング15aの表面に直接装
入できる。
In this invention, since the inner diameter RA of the magnetic ring 23 and the inner diameter RA of the annular groove 24 match, when the ring 23 is attached, it can be fixed without being eccentric from the center of the CP magnet 10. When installing, there is no need to remove the retaining ring 15a and insert it hidden inside the CP magnet 10, but it can be inserted directly onto the surface of the retaining ring 15a.

上記のように構成したことで、第4図に示すように偏向
ヨーク9の変化した垂直偏向磁界22は、非対称な補正
がされずに通常の垂直偏向磁界2゜に補正が可能であり
、しかも補正の際の取付けが容易である。
With the above configuration, as shown in FIG. 4, the vertical deflection magnetic field 22 of the deflection yoke 9 that has changed can be corrected to the normal vertical deflection magnetic field of 2° without being asymmetrically corrected. Easy to install for correction.

〔発明の効果〕〔Effect of the invention〕

以上説明したようにこの発明によれば、CPPb0止め
リング表面に形成した環状溝に磁性体リングを装着する
ようにしたので、偏向磁界を有効に補正することができ
る。また、磁性体リングの着脱の作業性を向上できる。
As explained above, according to the present invention, since the magnetic ring is attached to the annular groove formed on the surface of the CPPb0 retaining ring, the deflection magnetic field can be effectively corrected. Further, the workability of attaching and detaching the magnetic ring can be improved.

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

1第1図はこの発明の一実施例によるコンバーゼンス補
正装置の斜視図、第2図は従来のカラーブラウン管の構
成図、第3図はCPPb0拡大側面図、第4図は偏向ヨ
ークの斜視図、第5図は外部から影響を受けた偏向ヨー
クの垂直磁界の説明図、第6図は磁性体リングの正面図
、第7図はCP磁石へ磁性体リングの従来の取付は状態
の正面図である。 5・・・ネック部、10−CP磁石、lla、1lb−
2li磁石、12 a、  12 b−4i磁石、13
a。 13 b−6極磁石、15a、15b−止めリング、2
3・−・磁性体リング、24・・・環状溝。 なお、図中同一符号は同−又は相当部分を示す。
1. FIG. 1 is a perspective view of a convergence correction device according to an embodiment of the present invention, FIG. 2 is a configuration diagram of a conventional color cathode ray tube, FIG. 3 is an enlarged side view of CPPb0, and FIG. 4 is a perspective view of a deflection yoke. Figure 5 is an explanatory diagram of the vertical magnetic field of the deflection yoke influenced by the outside, Figure 6 is a front view of the magnetic ring, and Figure 7 is a front view of the conventional installation of the magnetic ring to the CP magnet. be. 5...Neck part, 10-CP magnet, lla, 1lb-
2li magnet, 12 a, 12 b-4i magnet, 13
a. 13 b - 6-pole magnet, 15a, 15b - retaining ring, 2
3... Magnetic ring, 24... Annular groove. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 陰極線管のネック部に装着され、偏向磁界を補正するた
めのコンバーゼンス補正装置において、コンバーゼンス
調整用磁石を構成する外側の止めリングの中心表面に環
状溝を形成し、この環状溝に磁性体リングを装着したこ
とを特徴とする陰極線管のコンバーゼンス補正装置。
In a convergence correction device that is attached to the neck of a cathode ray tube to correct the deflection magnetic field, an annular groove is formed on the center surface of the outer retaining ring that constitutes the convergence adjustment magnet, and a magnetic ring is inserted into this annular groove. A convergence correction device for a cathode ray tube, which is characterized by being installed.
JP8267388A 1988-04-04 1988-04-04 Convergence correcting device of cathode-ray tube Pending JPH01255136A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8267388A JPH01255136A (en) 1988-04-04 1988-04-04 Convergence correcting device of cathode-ray tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8267388A JPH01255136A (en) 1988-04-04 1988-04-04 Convergence correcting device of cathode-ray tube

Publications (1)

Publication Number Publication Date
JPH01255136A true JPH01255136A (en) 1989-10-12

Family

ID=13780943

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8267388A Pending JPH01255136A (en) 1988-04-04 1988-04-04 Convergence correcting device of cathode-ray tube

Country Status (1)

Country Link
JP (1) JPH01255136A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5708323A (en) * 1993-09-14 1998-01-13 Kabushiki Kaisha Toshiba Color cathode ray tube

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5708323A (en) * 1993-09-14 1998-01-13 Kabushiki Kaisha Toshiba Color cathode ray tube

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