JPH04123749A - Circular magnet for crt display apparatus - Google Patents

Circular magnet for crt display apparatus

Info

Publication number
JPH04123749A
JPH04123749A JP24507190A JP24507190A JPH04123749A JP H04123749 A JPH04123749 A JP H04123749A JP 24507190 A JP24507190 A JP 24507190A JP 24507190 A JP24507190 A JP 24507190A JP H04123749 A JPH04123749 A JP H04123749A
Authority
JP
Japan
Prior art keywords
magnetic
magnet body
parts
circular magnet
annular magnet
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
JP24507190A
Other languages
Japanese (ja)
Inventor
Hisashi Ebina
蛯名 久志
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.)
TDK Corp
Original Assignee
TDK 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 TDK Corp filed Critical TDK Corp
Priority to JP24507190A priority Critical patent/JPH04123749A/en
Publication of JPH04123749A publication Critical patent/JPH04123749A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To make the precision of magnetic joining uniform by making a step structure wherein magnetic parts in the inner circumference covering the neck region side of a television picture tube are extruded more than non- magnetic parts. CONSTITUTION:A circular magnet body 1 has a step structure in the inner circumference forming a fixing hole 2 wherein extruded parts 1a-1h for magnetic joining and non-magnetic parts 1i-1p are formed reciprocally and an extruded piece 1x for adjustment is formed in a part of the outer circumference of the circular magnet body 1. At the time of fixing magnetic yokes 10 magnetically to the circular magnet body l, each of extruded pieces 10a-10h of the magnetic yokes 10 are so put as to face to each of the parts 1a-1h for magnetic joining. With this structure. the magnetic fluxes at the time of magnetic fixing of the circular magnet body are converged into the parts for magnetic joining which correspond to the optional number of the poles, and consequently even if the magnetic resistance of the circular magnet body is not uniform, the precision of each of the parts for magnetic joining is improved.

Description

【発明の詳細な説明】 [発明の目的コ (産業上の利用分野) 本発明は、CRT(カソードレイチューブ)ディスプレ
イ装置用の環状磁石体に関し、より詳しくは、カラー用
又はモノクロ用のCRTディスプレイ装置におけるコン
バーゼンス磁石リング。
Detailed Description of the Invention [Objective of the Invention (Industrial Application Field) The present invention relates to an annular magnet body for a CRT (cathode ray tube) display device, and more particularly, to a color or monochrome CRT display device. Convergence magnet ring in the device.

センタリング磁石リング、ピンクジョン歪補正用磁石リ
ングとして用いられる環状磁石体に関する。
The present invention relates to an annular magnet used as a centering magnet ring and a pink John distortion correction magnet ring.

(従来の技術) 一般に、CRTディスプレイ装置においては、第5図に
示すように、CRT本体としての受像管20におけるネ
ック21の領域に電子銃3を内装するとともに、前記ネ
ック21の外周領域に、電子銃3から放出される電子ビ
ームを偏向するための偏向ヨーク4と、この偏向ヨーク
4の前側(蛍光面21a側)に位置するピンクジョン歪
補正用のピンクジョン歪補正用磁石リング5と、前記偏
向ヨーク4の後側(電子銃3側)に位置するコンバーゼ
ンス磁石リング6及びセンタリング磁石リング7とを取
付ける構成となっている。
(Prior Art) Generally, in a CRT display device, as shown in FIG. 5, an electron gun 3 is installed in a neck 21 area of a picture tube 20 serving as a CRT main body, and an electron gun 3 is installed in an outer peripheral area of the neck 21. A deflection yoke 4 for deflecting the electron beam emitted from the electron gun 3; a pink John distortion correction magnet ring 5 located in front of the deflection yoke 4 (on the phosphor screen 21a side); It has a configuration in which a convergence magnet ring 6 and a centering magnet ring 7 located on the rear side (electron gun 3 side) of the deflection yoke 4 are attached.

ところで、前記ピンクジョン歪補正用磁石リング5.コ
ンバーゼンス磁石リング6及びセンタリング磁石リング
7の如き磁石リング(以下「環状磁石体8」という。)
は、従来、第6図に示すように、例えば磁性粉入りの合
成樹脂材料により前記ネック2の外周に装着可能な内径
を有する段差のない円形孔9を穿設した環状に形成され
、その外周の一部に回転調整用の突出片8xを突設した
構成となっている。
By the way, the pink John distortion correction magnet ring 5. Magnet rings such as the convergence magnet ring 6 and the centering magnet ring 7 (hereinafter referred to as "annular magnet body 8")
Conventionally, as shown in FIG. 6, the neck 2 is formed into an annular shape with a step-free circular hole 9 having an inner diameter that can be attached to the outer periphery of the neck 2, made of a synthetic resin material containing magnetic powder, for example. It has a configuration in which a protruding piece 8x for rotation adjustment is provided protrudingly from a part of the holder.

この環状磁石体8に対するN、S磁極の着磁cjビンク
ツション歪補正用磁石リングとして用いられる場合は、
第6図に示すように、N、  S磁極を4個ずつ交互に
着磁した8個の突片10a乃至10hを放射状配置に有
する着磁ヨーク10により行われ、これにより、環状磁
石体8にN、  S磁極が交互に、かつ、一定間隔を隔
てつつ4個ずつ合計で8極構成となる一定間隔を有する
着磁部分8a乃至8hを形成するようになっている。
When used as a magnetic ring for compensating N and S magnetic poles of the annular magnet body 8,
As shown in FIG. 6, this is carried out by a magnetizing yoke 10 having eight protrusions 10a to 10h arranged radially, each of which has four N and four S magnetic poles alternately magnetized. The N and S magnetic poles are arranged alternately and spaced apart from each other at regular intervals to form magnetized portions 8a to 8h having regular intervals, with a total of 8 poles.

(発明が解決しようとする課題) しかしながら、上述した従来の環状磁石体8の場合、こ
の環状磁石体8に対する着磁を行う際環状磁石体8の内
周側が円形で段差部分が皆無であり、かつ、全体に亘っ
て磁気抵抗が一様でないため、着磁ヨーク10の各突片
10a、10c。
(Problems to be Solved by the Invention) However, in the case of the conventional annular magnet body 8 described above, when magnetizing the annular magnet body 8, the inner peripheral side of the annular magnet body 8 is circular and there is no stepped portion. In addition, since the magnetic resistance is not uniform throughout, each protruding piece 10a, 10c of the magnetizing yoke 10.

10e、10gから環状磁石体8の着磁部分8a8c、
8e、8gに向う磁束の流れは、環状磁石体8の磁気抵
抗の不均一さに起因して各着磁部分8a、8c、8e、
8gに対し不均一に作用し、これらのS極着磁精度にば
らつきが生じてしまうという問題がある。
From 10e and 10g, the magnetized portion 8a8c of the annular magnet body 8,
The flow of magnetic flux toward 8e, 8g is caused by the nonuniform magnetic resistance of the annular magnet body 8, and the magnetic flux flows toward each magnetized portion 8a, 8c, 8e,
There is a problem in that it acts non-uniformly on 8g, causing variations in the accuracy of these S pole magnetizations.

同様に、着磁の際に、各着磁部分8b、  8d。Similarly, during magnetization, each magnetized portion 8b, 8d.

8f、8hから突片10b、10d、10f。Projections 10b, 10d, 10f from 8f, 8h.

10hに向う磁束の流れも環状磁石体8の磁気抵抗の不
均一さに起因して不均一になり、各着磁部分8b、8d
、8f、8hのN極着磁精度にばらつきが生じてしまう
The flow of magnetic flux toward 10h also becomes non-uniform due to the non-uniform magnetic resistance of the annular magnet body 8, and each magnetized portion 8b, 8d
, 8f, and 8h, variations occur in the N-pole magnetization accuracy.

そこで、本発明は、着磁部分の形状を改良することによ
って、着磁精度の均一化を図ることができ、ひいては、
適正な電子ビームの位置補正を行うことに寄与し得るC
RTディスプレイ装置用の環状磁石体を提供することを
目的とするものである。
Therefore, the present invention can achieve uniform magnetization accuracy by improving the shape of the magnetized portion, and as a result,
C that can contribute to correcting the position of the electron beam appropriately
The object of the present invention is to provide an annular magnet for an RT display device.

[発明の構成コ (課題を解決するための手段) 本発明は、CRTディスプレイ装置の受像管のネック領
域に取付けられ、電子銃からの電子ビームの位置補正を
行う環状磁石体において、前記受像管のネック領域側を
占める内周側の任意極数に相当する着磁部分が非着磁部
分よりも突出する段差構造としたものである。
[Structure of the Invention (Means for Solving the Problems)] The present invention provides an annular magnet body that is attached to a neck region of a picture tube of a CRT display device and that corrects the position of an electron beam from an electron gun. It has a stepped structure in which magnetized portions corresponding to an arbitrary number of poles on the inner peripheral side occupying the neck region side of the magnet protrude from non-magnetized portions.

(作 用) 上述した環状磁石体によれば、受像管のネック側を占め
る内周側に、着磁部分が非着磁部分よりも突出する段構
造を設けたことにより、この環状磁石体の着磁の際の磁
束が任意極数に相当する着磁部分に絞り込まれ、これに
より、環状磁石体の磁気抵抗が不均一であっても各着磁
部分の着磁精度を向上させることができる。
(Function) According to the above-mentioned annular magnet, the step structure in which the magnetized portion protrudes more than the non-magnetized portion is provided on the inner peripheral side that occupies the neck side of the picture tube. The magnetic flux during magnetization is narrowed down to the magnetized portion corresponding to the arbitrary number of poles, and as a result, even if the magnetic resistance of the annular magnet body is uneven, the magnetization accuracy of each magnetized portion can be improved. .

(実施例) 以下に、本発明の実施例を詳細に説明する。(Example) Examples of the present invention will be described in detail below.

第1図に示す環状磁石体1は、磁性粉入すの合成樹脂材
料により所定の厚さの円形環状に形成され、略円形の装
着孔2に臨む内周側に、突出した着磁部分1a乃至1h
と非着磁部分11乃至1pとを交互に有する段差構造を
具備している。また、環状磁石体1の外周の一部には調
整用の突出片1xが設けられている。
The annular magnet body 1 shown in FIG. 1 is formed into a circular annular shape with a predetermined thickness from a synthetic resin material filled with magnetic powder, and has a protruding magnetized portion 1a on the inner circumferential side facing a substantially circular mounting hole 2. ~1h
It has a step structure having alternating portions and non-magnetized portions 11 to 1p. Moreover, a protruding piece 1x for adjustment is provided on a part of the outer periphery of the annular magnet body 1.

このような環状磁石体lに対し、既述した着磁ヨーク1
0により着磁する際には、第2図に示すように、前記装
着孔2に対し、着磁ヨークlOの各突片10a乃至10
hが前記各着磁部分1a乃至1hに各々対峙する状態と
なるように配置する。
For such an annular magnet l, the magnetizing yoke 1 described above
When magnetizing with 0, as shown in FIG.
h is arranged so as to face each of the magnetized portions 1a to 1h.

これにより、N極である各突片10a、IOC。As a result, each protruding piece 10a, which is a north pole, and the IOC.

10e、Logからの磁束が、非着磁部分1i。10e, the magnetic flux from Log is in the non-magnetized portion 1i.

lh、1m、ioに拡がらず各々対峙する着磁部分1a
、lc、4e、Igに対し絞り込まれる状態で作用し、
環状磁石体1に磁気抵抗の不均一さがあっても、各着磁
部分1a、lc、le、Igが各々均一に着磁されS極
として作用することになる。
Magnetized parts 1a facing each other without spreading to lh, 1m, and io
, lc, 4e, and Ig in a narrowed state,
Even if the annular magnet body 1 has non-uniform magnetic resistance, each magnetized portion 1a, lc, le, Ig is uniformly magnetized and acts as an S pole.

また、各着磁部分1b、ld、If、lhから、各々対
峙している突片10b、10d、10f。
Further, protrusions 10b, 10d, and 10f face each other from the magnetized portions 1b, ld, If, and lh, respectively.

10hに向う磁束も、環状磁石体1に磁気抵抗の不均一
さがあっても絞り込まれる状態となり、この際、非着磁
部分1j、11.in、ipからの磁束の回り込みもな
く、これにより、各着磁部分lb、ld、if、lhは
各々均一に着磁され各々N極として作用することになる
10h is also narrowed down even if there is non-uniform magnetic resistance in the annular magnet body 1, and at this time, the non-magnetized portions 1j, 11. There is no wraparound of the magnetic flux from in and ip, and as a result, each of the magnetized portions lb, ld, if, and lh are uniformly magnetized and act as N poles.

このようにして着磁された環状磁石体1を第3図に示す
The annular magnet body 1 magnetized in this manner is shown in FIG.

尚、前記着磁部分1aと非着磁部分11との間の段差構
造(他の部分も同様)は、第4図に示すように滑らかな
曲線をもって連続する構造とすることもできる。
Incidentally, the step structure between the magnetized portion 1a and the non-magnetized portion 11 (the same applies to other portions) may also be formed into a continuous structure with a smooth curve as shown in FIG.

以上詳述した本実施例の環状磁石体1によれば、着磁部
分1a乃至1hと非着磁部分11乃至1pを各々段差を
って連結する形状としたことにより、磁気抵抗の不均一
さが仮にあっても、各着磁部分1a乃至1hを均一に着
磁して使用に供することが可能となり、これにより、ピ
ンクジョン歪補正用、コンバーゼンス調整用、センタリ
ング調整用として適正な動作を発揮させることが可能に
なる。
According to the annular magnet body 1 of the present embodiment described in detail above, the magnetized portions 1a to 1h and the non-magnetized portions 11 to 1p are connected to each other with a step difference, thereby reducing the non-uniformity of magnetic resistance. Even if there is, it is possible to uniformly magnetize each magnetized portion 1a to 1h and use it, thereby demonstrating appropriate operation for pink John distortion correction, convergence adjustment, and centering adjustment. It becomes possible to do so.

本発明は、上述した実施例に限定されるものではなく、
その要旨の範囲内で種々の変形が可能である。
The present invention is not limited to the embodiments described above,
Various modifications are possible within the scope of the gist.

例えば、上述した実施例では8極構成の環状磁石体1に
ついて説明したが、この他、2極、4極。
For example, in the above-mentioned embodiment, the annular magnet 1 having an 8-pole configuration has been described, but other magnets include a 2-pole structure and a 4-pole structure.

6極、12極等任意極数の磁極構成としても実施可能で
ある。
It is also possible to implement a magnetic pole configuration with an arbitrary number of poles such as 6 poles or 12 poles.

[発明の効果コ 以上詳述した本発明によれば、上述した構成としたこと
により、各着磁部分の着磁精度が、磁気抵抗の不均一さ
がある場合でも均一に近いものとなり、これにより、使
用に際して、適正な電子ビームの位置補正を行うことに
寄与し得る着磁精度の良い環状磁石体を提供することが
できる。
[Effects of the Invention] According to the present invention described in detail above, due to the above-described configuration, the magnetization accuracy of each magnetized portion becomes nearly uniform even when there is non-uniformity of magnetic resistance. Accordingly, it is possible to provide an annular magnet body with high magnetization accuracy that can contribute to correcting the position of an electron beam appropriately during use.

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

第1図は本発明に係る環状磁石体の実施例を示す斜視図
、第2図は同上の着磁状態の平面図、第3図は同上の着
磁後の状態の平面図、第4図は本実施例の段差構造の変
形例を示す部分拡大平面図、第5図はCRTディスプレ
イ装置の概略側面図、第6図は従来の環状磁石体の平面
図である。 1・・・環状磁石体、1a乃至1h・・・着磁部分、1
1乃至1p・・・非着磁部分、20・・・受像管、21
・・・ネック。 第 r 図
Fig. 1 is a perspective view showing an embodiment of the annular magnet according to the present invention, Fig. 2 is a plan view of the above magnetized state, Fig. 3 is a plan view of the same after magnetization, and Fig. 4 5 is a partially enlarged plan view showing a modification of the stepped structure of this embodiment, FIG. 5 is a schematic side view of a CRT display device, and FIG. 6 is a plan view of a conventional annular magnet body. 1... Annular magnet body, 1a to 1h... Magnetized part, 1
1 to 1p...non-magnetized portion, 20... picture tube, 21
···neck. Figure r

Claims (1)

【特許請求の範囲】 CRTディスプレイ装置の受像管のネック領域に取付け
られ、電子銃からの電子ビームの位置補正を行う環状磁
石体において、 前記受像管のネック領域側を占める内周側の着磁部分が
非着磁部分よりも突出する段差構造としたことを特徴と
するCRTディスプレイ装置用の環状磁石体。
[Scope of Claims] In an annular magnet body that is attached to the neck region of a picture tube of a CRT display device and that corrects the position of an electron beam from an electron gun, magnetization is provided on the inner peripheral side that occupies the neck region side of the picture tube. 1. An annular magnet for a CRT display device, characterized by having a stepped structure in which a portion protrudes more than a non-magnetized portion.
JP24507190A 1990-09-13 1990-09-13 Circular magnet for crt display apparatus Pending JPH04123749A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24507190A JPH04123749A (en) 1990-09-13 1990-09-13 Circular magnet for crt display apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24507190A JPH04123749A (en) 1990-09-13 1990-09-13 Circular magnet for crt display apparatus

Publications (1)

Publication Number Publication Date
JPH04123749A true JPH04123749A (en) 1992-04-23

Family

ID=17128164

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24507190A Pending JPH04123749A (en) 1990-09-13 1990-09-13 Circular magnet for crt display apparatus

Country Status (1)

Country Link
JP (1) JPH04123749A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8013696B2 (en) 2008-10-14 2011-09-06 Nexteer (Beijing) Technology Co., Ltd. Magnetic apparatus and method of manufacturing the magnetic apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8013696B2 (en) 2008-10-14 2011-09-06 Nexteer (Beijing) Technology Co., Ltd. Magnetic apparatus and method of manufacturing the magnetic apparatus

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