JPS59173932A - Production method of crt - Google Patents
Production method of crtInfo
- Publication number
- JPS59173932A JPS59173932A JP4817883A JP4817883A JPS59173932A JP S59173932 A JPS59173932 A JP S59173932A JP 4817883 A JP4817883 A JP 4817883A JP 4817883 A JP4817883 A JP 4817883A JP S59173932 A JPS59173932 A JP S59173932A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- generating member
- field generating
- magnetic field
- pole
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J9/00—Apparatus or processes specially adapted for the manufacture, installation, removal, maintenance of electric discharge tubes, discharge lamps, or parts thereof; Recovery of material from discharge tubes or lamps
- H01J9/44—Factory adjustment of completed discharge tubes or lamps to comply with desired tolerances
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は電子ビームの軌道を修正するための陰極線管
の製造方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of manufacturing a cathode ray tube for correcting the trajectory of an electron beam.
従来の陰極線管装置を示す第1図において、(1)はカ
ラー陰極線管装置し、パネル部(1a)の内面に形成さ
れた螢光スクリーン(2)と、シャドウマスク(3)お
よび螢光スクリーン(2)ニ対向してネック部(1に+
) K配置された市子銃(4)とを内蔵して形成さねて
いる。(6)は陰極線管(1)のファンネル部(1c)
外周に取付けられた偏向ヨークで、鴫子銃(4)によっ
て形成さ7″した鑵子ビームを水平および垂直方向に偏
向させる。(6)はゴム状に形成されたフェライト磁石
全陰極@菅tNのネック部(1b)外周に巻きつけて構
成された磁界発生部材で、螢光スクリーン(2)ニおけ
るストライプ幅中心と゛電子ビームの幅中心とを一致き
せるだめの補正磁界を電子ビームに与えるものである。In FIG. 1 showing a conventional cathode ray tube device, (1) is a color cathode ray tube device, which includes a fluorescent screen (2) formed on the inner surface of a panel portion (1a), a shadow mask (3), and a fluorescent screen. (2) Neck part facing 2 (+ to 1)
) It is formed with a built-in Ichiko gun (4) arranged in K. (6) is the funnel part (1c) of the cathode ray tube (1)
A deflection yoke attached to the outer periphery deflects the 7" beam formed by the scoop gun (4) horizontally and vertically. (6) is a ferrite magnet all cathode @ SugatN made of rubber. A magnetic field generating member wrapped around the outer periphery of the neck portion (1b), which provides the electron beam with a corrective magnetic field that allows the center of the stripe width on the fluorescent screen (2) to coincide with the center of the width of the electron beam. be.
この補正磁界は第2図に示すように一対の近接した磁極
からなる着磁ヘッド(7)全磁界発生部材(6)の外周
VC密着させながら回動させ、S極あるい1−jN極に
順次磁化させることによって形成さねている。As shown in Fig. 2, this correction magnetic field is applied by rotating the magnetizing head (7), which consists of a pair of adjacent magnetic poles, while bringing the entire magnetic field generating member (6) into close contact with the outer circumference VC, and applying it to the S pole or 1-j N pole. It is formed by sequential magnetization.
ところで、磁界発生部材fi+の磁化容易軸は陰極線管
用の管軸に直交する方向に形成さねており、第2図に示
すよう′fx看磁着磁を用いると、磁束が磁化容易軸と
直交する方向に発生することになるため着磁効率が極め
て悪く、また、大きな磁束ぞ度を必要とすることから、
゛嘔力消黄も大きなものとなっていた。By the way, the axis of easy magnetization of the magnetic field generating member fi+ is formed in a direction perpendicular to the tube axis of the cathode ray tube, and when using 'fx magnetization as shown in Figure 2, the magnetic flux is perpendicular to the axis of easy magnetization. Since the magnetic flux is generated in the direction of
``Nausea and yellowing were also a major problem.
この発明ぼ上述のL12な欠点を解消するためなされた
もので、着磁効率を向上させた陰極、I!!管の製造方
法を提供するものである。This invention was made to eliminate the above-mentioned drawbacks of L12, and is a cathode with improved magnetization efficiency. ! A method for manufacturing a tube is provided.
以下、この発明を一実施例である第3図、第4図につい
て説明する。Hereinafter, this invention will be explained with reference to FIGS. 3 and 4, which are one embodiment.
第3図なこの発明による着磁装置を示すもので、E字状
に形成されたコア(8)と、このコア(8)の中心磁極
(8a)に蓚き付けられたコイル(9)と、コア(8)
の両側磁極(8b)に対して摺動可能に取付けられた円
弧状の磁性体(10)とから形成されている。すなわち
、磁極(8a)と磁性体(+01とVCLり異なる磁束
密度の着磁ヘッドが形成されることになる。Figure 3 shows a magnetizing device according to the present invention, which includes a core (8) formed in an E-shape, and a coil (9) attached to the central magnetic pole (8a) of this core (8). , core (8)
It is formed from an arcuate magnetic body (10) slidably attached to the magnetic poles (8b) on both sides of the magnetic body. That is, a magnetized head having different magnetic flux densities is formed between the magnetic pole (8a) and the magnetic body (+01 and VCL).
このような着磁装置を用い、まず、陰極線管+1+にお
けるネック部(1b) f磁極(8a)と磁性体(lO
)との間に挿入して磁性体(lO)を上方に移動させ、
第4図に示すように磁界発生部材(6)の外周を挾むよ
うに配置する。次いで、コイル(9)に電流ケ流すと、
磁極(8a)の先端から磁性体(101K向って磁力線
が発生することになり、このとき、磁極(8a)の先端
部分が最大の磁束密度となる。捷だ、磁極(8a)と磁
性体(lO)の距離を管軸を通る位置において最も短か
くなるように磁性体f101 k形成することによって
磁極(8a)の先端に対応する磁界発生部材(6)には
磁力線が肉厚方向すなわち磁化容易軸と同一方向vc全
発生ることになり、効果的vc4磁させることが可能と
なる。その後、パルスモータに工って着磁装装置f 1
/200のピッチで回動するとともに磁極(8a) f
N極またばS極(て切替えることにエリ、磁界発生部材
(6)?順次着磁して工程を完了する。Using such a magnetizing device, first, the neck part (1b), the f magnetic pole (8a) and the magnetic body (lO
) to move the magnetic material (lO) upward,
As shown in FIG. 4, they are arranged so as to sandwich the outer periphery of the magnetic field generating member (6). Next, when a current is passed through the coil (9),
Lines of magnetic force are generated from the tip of the magnetic pole (8a) toward the magnetic body (101K, and at this time, the tip of the magnetic pole (8a) has the maximum magnetic flux density. By forming the magnetic material f101k so that the distance of lO) is the shortest at the position passing through the tube axis, the magnetic field generating member (6) corresponding to the tip of the magnetic pole (8a) has lines of magnetic force in the thickness direction, that is, easy to magnetize. All VC will be generated in the same direction as the axis, making it possible to effectively magnetize VC4.After that, a pulse motor will be used to create a magnetizing device f1.
It rotates at a pitch of /200 and the magnetic pole (8a) f
The magnetic field generating member (6) may be switched between the N pole and the S pole (6).The process is completed by sequentially magnetizing the magnetic field generating member (6).
なお、着磁磁界および強度は囃子ビームと螢光体発光部
と9相対的なずれを検出し、こね全補正するために必要
な磁界全算出させることによって決定さねる。丑1こ、
磁4(8a)の幅WH磁界発生部材(6)の肉厚に対し
て2倍程度が必軛とさね、磁界発生t$材(6)の肉厚
全0.’i’6mm七すると、1.5mmに形成する必
要がある。さらに、磁極(8a)の肉厚tは約5rnm
Vc影形成れている。Note that the magnetizing magnetic field and strength are determined by detecting the relative deviation between the musical accompaniment beam and the fluorescent light emitting section, and calculating the total magnetic field required to fully correct the kneading. 1 ox,
The width of the magnet 4 (8a) WH must be about twice the thickness of the magnetic field generating member (6), and the total thickness of the magnetic field generating member (6) is 0. If 'i' is 6mm, then it needs to be formed to 1.5mm. Furthermore, the wall thickness t of the magnetic pole (8a) is approximately 5 rnm.
Vc shadow is formed.
このように形成することによって、磁界発生部材+61
VCおける宣磁磁界幅を狭く、かつ強力な着磁が可能
となり、囃子ビームの軌道補正の精度全向上させること
ができる。By forming in this way, the magnetic field generating member +61
It becomes possible to narrow the width of the magnetic field in the VC and to achieve strong magnetization, thereby making it possible to completely improve the accuracy of the trajectory correction of the accompaniment beam.
なお、上述の実施例においては、コアt81’ThK字
状に形成し、両IJlll磁極(8b) l+’jに磁
性体(lO)を架設するように構成したが、コ字状とし
て磁性体(10)の一方を遊端としてもよく、また、磁
界発生部材(6)ヲ陰極線−#(1)のネック部(lb
)内に配置してもよい。In the above-mentioned embodiment, the core t81'ThK-shape was formed, and the magnetic material (lO) was installed on both IJllll magnetic poles (8b) l+'j. 10) may be used as a free end, and the magnetic field generating member (6) may be connected to the neck portion (lb) of the cathode ray #(1).
) may be placed within.
ざらに、着磁装置を固定とし、陰極線管(1)を回動す
るように構成してもよい。Alternatively, the magnetizing device may be fixed and the cathode ray tube (1) may be configured to rotate.
以上、説明したように、この発明によれば磁界発生部材
の看磁効率を向上させることが可能となり、この発明の
実用価値は太である。As described above, according to the present invention, it is possible to improve the viewing efficiency of the magnetic field generating member, and the practical value of the present invention is great.
第1図はカラー陰極線管の構成?示す概要図、第2図は
従来の着磁方法を示す概要図、第3図けこの発明vc…
いられる着磁装置?尽す概要図、第4図なこの発1力の
一実施例である看破方法を示す概要図である。
図中、(1)は陰極線管、(1b)はネック部、(6)
け磁界発生部材、(8)はコア、(9)はコイル、(1
o)は磁性体である。
なお、図中、同一符号な同一あるいけ相当する部分を示
すものとする。
第1図
第2図Figure 1 shows the configuration of a color cathode ray tube? Fig. 2 is a schematic diagram showing the conventional magnetization method, Fig. 3 is a schematic diagram showing the conventional magnetization method, and Fig. 3 is a schematic diagram showing the conventional magnetization method.
A magnetizing device that can be used? FIG. 4 is a schematic diagram showing a detection method which is an embodiment of this power. In the figure, (1) is the cathode ray tube, (1b) is the neck, (6)
magnetic field generating member, (8) is the core, (9) is the coil, (1
o) is a magnetic material. In the figures, the same reference numerals indicate corresponding parts. Figure 1 Figure 2
Claims (1)
着磁する手段として、異なる磁束密度全発生する一対の
磁極間に上記磁界発生部材を配置させ、上記磁極またげ
陰極線管全回動じて着磁するようにしたことを特徴とす
る陰極線管の製造方法。As a means of magnetizing the annular magnetic field generating member provided at the neck of the cathode ray tube, the magnetic field generating member is placed between a pair of magnetic poles that generate different magnetic flux densities, and the cathode ray tube is completely rotated across the magnetic poles. A method for manufacturing a cathode ray tube, characterized in that the cathode ray tube is magnetized by the following steps.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4817883A JPS59173932A (en) | 1983-03-22 | 1983-03-22 | Production method of crt |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4817883A JPS59173932A (en) | 1983-03-22 | 1983-03-22 | Production method of crt |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59173932A true JPS59173932A (en) | 1984-10-02 |
JPH022259B2 JPH022259B2 (en) | 1990-01-17 |
Family
ID=12796128
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4817883A Granted JPS59173932A (en) | 1983-03-22 | 1983-03-22 | Production method of crt |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59173932A (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51122322A (en) * | 1975-04-01 | 1976-10-26 | Philips Nv | Method of producing magnetic convergence device and color display tube having magnetic convergence device |
JPS5576554A (en) * | 1978-11-30 | 1980-06-09 | Mitsubishi Electric Corp | Color braun tube |
-
1983
- 1983-03-22 JP JP4817883A patent/JPS59173932A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51122322A (en) * | 1975-04-01 | 1976-10-26 | Philips Nv | Method of producing magnetic convergence device and color display tube having magnetic convergence device |
JPS5576554A (en) * | 1978-11-30 | 1980-06-09 | Mitsubishi Electric Corp | Color braun tube |
Also Published As
Publication number | Publication date |
---|---|
JPH022259B2 (en) | 1990-01-17 |
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