JPH01209639A - Magnet composition for convergence correction - Google Patents

Magnet composition for convergence correction

Info

Publication number
JPH01209639A
JPH01209639A JP3322388A JP3322388A JPH01209639A JP H01209639 A JPH01209639 A JP H01209639A JP 3322388 A JP3322388 A JP 3322388A JP 3322388 A JP3322388 A JP 3322388A JP H01209639 A JPH01209639 A JP H01209639A
Authority
JP
Japan
Prior art keywords
ring
spacer
shaped
convergence correction
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
JP3322388A
Other languages
Japanese (ja)
Inventor
Katsumi Muta
牟田 克巳
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 JP3322388A priority Critical patent/JPH01209639A/en
Publication of JPH01209639A publication Critical patent/JPH01209639A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce the cost by forming projections or ring-form grooves which are geared to the pushing-out parts of ring-form magnets and maintained rotatable coaxially to the tube axis, at the contact surfaces of a holding member and a spacer to the ring-form magnets. CONSTITUTION:In this convergence correction magnet composition 11, the inner diameter of ring-form magnets 52, 62, and 72 is formed a little larger than the outer diameter of the neck 2 of a cathode-ray tube, and pushing-out parts 52b, 62b, and 72b, which are coaxial to the central axis, are formed. Projections 12d, 13d, and 14d, or ringform grooves 12a, 13a, and 14a, to gear with the pushing-out parts 52b, 62b, and 72b being maintained coaxial, at the surfaces where a holding member 14 arranged at both ends and a spacer 13 arranged at the middle are contacted to the ring-form magnets 52, 62, and 72, are formed. Furthermore, the magnet composition 11 is contacted elastically to tubes 12b, and 14b of the holding member 14 and to the outer wall surface of the neck 2.

Description

【発明の詳細な説明】 [産業上の利用分野] この発明はインライン形電子銃を有するカラー陰極線管
のビユリティおよびスタティックφコンバーゼンスの補
正に用いられるコンバーゼンス補正用磁石構体に関する
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a convergence correction magnet structure used to correct the utility and static φ convergence of a color cathode ray tube having an in-line electron gun.

[従来の技術] 第7図は特公昭51−45936号公報に示されている
スタティック・コンバーゼンス補正用磁石構体をカラー
陰極線管に装着した状態で示す一部破断側面図である。
[Prior Art] FIG. 7 is a partially cutaway side view showing the static convergence correction magnet assembly disclosed in Japanese Patent Publication No. 45936/1983, which is attached to a color cathode ray tube.

図において、(1)はカラー陰極線管のファンネル部、
(2)はネック部、(3)は偏向ヨーク、(5)は一対
の薄いリング状磁石(51)および(52)で構成され
た第1の可変磁界発生装置、(8)は同じく一対のリン
グ状磁石(81)および(82)で構成された第2の可
変磁界発生装置、(7)は同じく一対のリング状磁石(
71)および(72)で構成された第3の可変磁界発生
装置で、第1の可変磁界発生装置(5)はピュリ補正用
の2極磁界を発生し、第2および第3の可変磁界発生装
置(8)および(7)はスタテイック−コンバーゼンス
補正用の4極および6極磁界を発生する。(0はネック
部(2)に挿入される合成樹脂材などの非磁性材で形成
された筒状支持体、(8)は筒状支持体(4)に嵌めら
れて固定されている合成樹脂材等の非磁性材で形成され
たリング状の位置決め部材で1位置決め部材(8)の間
にはリング状磁石(51)および(52) 。
In the figure, (1) is the funnel part of the color cathode ray tube;
(2) is a neck portion, (3) is a deflection yoke, (5) is a first variable magnetic field generator composed of a pair of thin ring-shaped magnets (51) and (52), and (8) is a first variable magnetic field generator composed of a pair of thin ring-shaped magnets (51) and (52). The second variable magnetic field generator is composed of ring-shaped magnets (81) and (82), and (7) is also composed of a pair of ring-shaped magnets (
71) and (72), the first variable magnetic field generator (5) generates a bipolar magnetic field for Pury correction, and the second and third variable magnetic field generators Devices (8) and (7) generate 4-pole and 6-pole magnetic fields for static-convergence correction. (0 is a cylindrical support made of a non-magnetic material such as a synthetic resin material that is inserted into the neck part (2), and (8) is a synthetic resin that is fitted and fixed to the cylindrical support (4). There are ring-shaped positioning members (51) and (52) between each positioning member (8).

(61)および(1112) 、 (71)および(7
2)がそれぞれ摩擦低減用の薄いワッシャ(8)を挾ん
で密着し、かつ回転可能に挾持された状態でもって保持
されている。 (10)は筒状支持体(4)の一端をネ
ック部(2)に締め付けて固定する締付バンド、(10
a)はその締付用のネジで、筒状支持体(4)〜締結バ
ンド(lO)でコンバーゼンス補正用磁石構体(11)
を構成している。
(61) and (1112), (71) and (7
2) are held in close contact with each other by sandwiching a thin washer (8) for reducing friction, and are rotatably held in the sandwiched state. (10) is a tightening band that tightens and fixes one end of the cylindrical support (4) to the neck (2);
a) is a screw for tightening the convergence correction magnet structure (11) between the cylindrical support (4) and the fastening band (lO).
It consists of

第8図は第7図■−■線矢視断面図で、(72a)はリ
ング状磁石(72)に形成されている回転位置調整用の
突出タブで、他のリング状磁石にもそれぞれ設けられて
いる0図中、R,G、Bは図示していないインライン形
電子銃から発射された3木の電子ビームで中央の電子ビ
ームGが管軸Zを通るように構成されている。
Fig. 8 is a sectional view taken along the line ■-■ in Fig. 7, and (72a) is a protruding tab for adjusting the rotational position formed on the ring-shaped magnet (72), which is also provided on the other ring-shaped magnets. In the figure, R, G, and B are three electron beams emitted from an in-line electron gun (not shown), and the center electron beam G is configured to pass through the tube axis Z.

このように構成されたコンバーゼンス補正用磁石構体(
11)は、カラー陰極線管を作動させたとき、各リング
状磁石(51)〜(72)の回転位置を調節することに
よりピユリティ補正およびスタティック・コンバーゼン
スの補正を行うことができる。
The convergence correction magnet structure configured in this way (
11), when the color cathode ray tube is operated, the purity correction and static convergence correction can be performed by adjusting the rotational position of each of the ring-shaped magnets (51) to (72).

[発明が解決しようとする課題] 従来のコンバーゼンス補正用磁石構体(11)は、構成
部品点数が多く、また、筒状支持体(4)にリング磁石
(51)〜(72)が嵌められた状態で組み立てられて
いるので、筒状支持体(4)の厚さだけリング状磁石の
内径が大きくなり、その分だけ電子ビームに作用する磁
界が弱くなるため、強い磁界を発生するリング磁石が必
要になり、コスト高となる。
[Problems to be Solved by the Invention] The conventional convergence correction magnet structure (11) has a large number of component parts, and the ring magnets (51) to (72) are fitted into the cylindrical support (4). Since the inner diameter of the ring-shaped magnet increases by the thickness of the cylindrical support (4), the magnetic field that acts on the electron beam becomes weaker by that much, so the ring magnet that generates a strong magnetic field becomes necessary, and the cost is high.

この発明は構成部品点数が少なく、また、弱い磁界を発
生するリング状磁石で足りるコストの安い補正用磁石構
体を得ることを目的とする。
It is an object of the present invention to provide a low-cost correction magnet assembly that has a small number of component parts and that requires only a ring-shaped magnet that generates a weak magnetic field.

[課題を解決するための手段] この発明に係るコンバーゼンス補正用磁石構体は、各リ
ング状磁石の内径をネック部の外径より僅かに大きい寸
法に形成するとともに、互いに嵌り合う管軸と同志に形
成されている環状の押出部を形成して重ね合わせ、この
重ね合わせた各一対のリング状磁石を位置決めして保持
するスペーサおよび支持部材の当接面にそれぞれ上記環
状の押出部に係合して管軸に対して同志に保持する環状
の突起部および溝部をそれぞれ設けてなることを特徴と
する。
[Means for Solving the Problems] In the convergence correction magnet structure according to the present invention, the inner diameter of each ring-shaped magnet is formed to be slightly larger than the outer diameter of the neck portion, and the inner diameter of each ring-shaped magnet is formed to be slightly larger than the outer diameter of the neck portion, and the structure is arranged so that the inner diameter of each ring-shaped magnet is slightly larger than the outer diameter of the neck portion. The annular extruded portions are formed and overlapped, and the contact surfaces of a spacer and a support member that position and hold each pair of overlapping ring-shaped magnets are respectively engaged with the annular extruded portions. It is characterized in that it is provided with an annular protrusion and a groove that are held together with respect to the tube axis.

[作用] リング状磁石の内径をネック部の外径より僅かに大きい
寸法に形成したので、リング状磁石を電子ビームに近づ
けることができ、したがって、リング状磁石に弱い磁石
を用いることができる。
[Function] Since the inner diameter of the ring-shaped magnet is formed to be slightly larger than the outer diameter of the neck portion, the ring-shaped magnet can be brought close to the electron beam, and therefore a weak magnet can be used as the ring-shaped magnet.

また、従来装置における筒状支持体および締付バンドを
要しないので、構成部品点数が少なくなる。
Further, since the cylindrical support and the tightening band in the conventional device are not required, the number of component parts is reduced.

[発明の実施例] 第1図はこの発明の一実施例の一部破断側面図である。[Embodiments of the invention] FIG. 1 is a partially cutaway side view of an embodiment of the present invention.

図において、(12)、(14)はコンバーゼンス補正
用磁石構体(1りの両端に配設されたリング状の支持部
材で、その内径はネック部(2)の外形より僅かに大き
く、スリン) (12a)、(14a)が設けられた筒
部(12b) 、(tab)の先端は僅かに小径に形成
されて弾性力でもってネック部(2)の外壁に当接し。
In the figure, (12) and (14) are ring-shaped support members disposed at both ends of the convergence correction magnet structure (1), the inner diameter of which is slightly larger than the outer diameter of the neck (2). The tips of the cylindrical portions (12b) and (tab) provided with the cylindrical portions (12a) and (14a) are formed to have a slightly small diameter and abut against the outer wall of the neck portion (2) with elastic force.

ff擦力でもって配置された位置を保つように構成され
、フランジ部の内面には、それぞれ第2図および第5図
に示すように、突起部(12d)、および環状の溝部(
14d)が中心軸Oと同軸形成されている。リング状磁
石(51) 、(81) 、(71)には、それぞれ第
3図に示すように、円弧状の押出部(51b)、(81
b)、(71b)が中心軸0と同軸に形成されており、
その開き角度θは、この例では90’である。また、リ
ング状磁石(52)、(62) 、(72)には、それ
ぞれ第4図に示すように、環状の押出部(52b)、(
82b)。
ff It is configured to maintain the arranged position by frictional force, and the inner surface of the flange part has a protrusion (12d) and an annular groove (12d), as shown in FIGS. 2 and 5, respectively.
14d) is formed coaxially with the central axis O. As shown in FIG. 3, the ring-shaped magnets (51), (81), and (71) have arc-shaped extruded portions (51b) and (81), respectively.
b), (71b) are formed coaxially with the central axis 0,
The opening angle θ is 90' in this example. Further, as shown in FIG. 4, the ring-shaped magnets (52), (62), and (72) have annular extruded portions (52b), (
82b).

(72b)が中心軸0と同軸に形成されている。リング
状のスペーサ(13)の一方の当接面には環状の溝部(
13a)が、また反対側の当接面には突起部(13b)
が形成されており、支持部材(12)、リング状磁石(
51) 、ワッシャ(9)、リング状磁石(52) 。
(72b) is formed coaxially with the central axis 0. The ring-shaped spacer (13) has an annular groove (
13a), and there is also a protrusion (13b) on the contact surface on the opposite side.
is formed, a supporting member (12), a ring-shaped magnet (
51), washer (9), ring-shaped magnet (52).

スペーサ(13) 、リング状の磁石(61)、・・・
支持部材(14)の図示の順に重ねられて、突起部(1
2d)、(13d)と円弧状の押出部(51b) 、(
Ellb) 、(72b)とが係合し、また円弧状の押
出部(51b) 、(81b) 、(71b)と環状の
押出部(52b) 、 (82b) 、 (72b)と
が係合し、さらに円弧状の押出部(52b) 、([1
2b) 、(72b)と環状の溝部(13a) 、 (
14d)とが係合して管軸Zと同軸に各構成部材が支持
部材(12)、(14)によって両端から挾持された状
態でもってネック部(2)に挿入された状態でもって保
持され、支持部材(12)、(14)の筒部(12b)
 、(14b)に形成されている凹部(12c)、(1
4c)の部分で接着剤(15)によりネック部(2)に
固定され、各リング状磁石(51)、(52)、(81
)、(62)、(71)、(72)はネック部(2)に
当接することなく、角度θの範囲内で自由に回転位置が
調節できるように構成されている。
Spacer (13), ring-shaped magnet (61),...
The support members (14) are stacked in the order shown, and the protrusions (1
2d), (13d) and the arc-shaped extrusion part (51b), (
Ellb), (72b) are engaged, and the arcuate extrusion parts (51b), (81b), (71b) are engaged with the annular extrusion parts (52b), (82b), (72b). , and further an arcuate extrusion part (52b), ([1
2b), (72b) and the annular groove (13a), (
14d) are engaged with each other so that each component is held coaxially with the tube axis Z while being inserted into the neck portion (2) while being held from both ends by the supporting members (12) and (14). , the cylindrical portion (12b) of the support members (12), (14)
, (14b) are formed in the recesses (12c), (1
4c) is fixed to the neck part (2) with adhesive (15), and each ring-shaped magnet (51), (52), (81
), (62), (71), and (72) are configured so that their rotational positions can be freely adjusted within the range of angle θ without coming into contact with the neck portion (2).

第6図はこの発明の他の実施例の一部破断側面図で、各
リング状磁石の内径部分を同一方向に押し出した円錐状
の押出部(51c) 、(52c) 、(etc) 、
(E12c)、(71c)、(72c)を形成するとと
もに、支持部材(12)、(14)およびスペーサ(1
3)にそれぞれこの押出部に係合する円錐面を形成した
もので、第1図に示した実施例と同様に、リング状磁石
(51)、(52) 、(81)、(82) 、(71
)、(72)を回転自由に保持してネック部(2)に取
り付けることができる。
FIG. 6 is a partially cutaway side view of another embodiment of the present invention, in which the inner diameter portions of each ring-shaped magnet are pushed out in the same direction with conical extrusion parts (51c), (52c), (etc),
(E12c), (71c), (72c), supporting members (12), (14) and spacer (1
3) are each formed with a conical surface that engages with this extruded portion, and similarly to the embodiment shown in FIG. 1, ring-shaped magnets (51), (52), (81), (82), (71
), (72) can be rotatably held and attached to the neck (2).

なお、この発明に係る補正用磁石構体(11)を装着す
る場合、順次各構成部材をネック部(2)に挿入してゆ
き、筒部(12b) 、(14b)の弾性力でもって一
体に組立てて位置決めしたのち接着剤(15)で固定す
るが、作業性を高めるため、第1図中に一点鎖線で示し
たように非磁性材で形成した締結部材(16)を支持部
材(12)、(14)間に複数水掛は渡して一体に組立
てた状態としたものをネック部(2)に挿入するように
してもよい。
In addition, when installing the correction magnet structure (11) according to the present invention, each component is sequentially inserted into the neck part (2), and the elastic force of the cylindrical parts (12b) and (14b) is used to unite them. After assembly and positioning, it is fixed with adhesive (15), but in order to improve workability, a fastening member (16) made of non-magnetic material is attached to the support member (12) as shown by the dashed line in Fig. 1. , (14) A plurality of water hooks may be passed between them, assembled into one body, and then inserted into the neck portion (2).

なお、支持部材、スペーサおよびリング状磁石を、管軸
Zと同軸に回転可能に係合させるための構成は、上記実
施例のほか、種々な変形が可能である0例えば、突起部
(12d) 、(13a)をそれぞれ環状の突起部に形
成し、円弧状の押出部(51b) 、(Blb)、(7
1b)はそれぞれ環状の押出部に形成してもよく、この
ように構成すればリング状磁石は同一形のものとするこ
とができる。
The configuration for rotatably engaging the support member, spacer, and ring-shaped magnet coaxially with the tube axis Z can be modified in various ways in addition to the above embodiment. , (13a) are respectively formed into annular projections, and arcuate extrusion parts (51b), (Blb), (7
1b) may each be formed into an annular extruded portion, and with this configuration, the ring-shaped magnets can have the same shape.

さらに、両端の支持部材(12)、(14)を同一形状
のものを用い、リング状磁石(71)、(72)の押出
部の向きを反対にしてスペーサ(13)の突起部(13
b)を環状の溝部に変更すれば、簡単な形状のスペーサ
(13)を2種類用意するだけで、複雑な形状の支持部
材を1種類にすることができる。
Further, the supporting members (12) and (14) at both ends are of the same shape, and the direction of the extruded parts of the ring-shaped magnets (71) and (72) is reversed so that the protruding part (13) of the spacer (13)
By changing b) to an annular groove, only one type of support member with a complicated shape can be used by simply preparing two types of spacers (13) with a simple shape.

[発明の効果] この発明に係るコンバーゼンス補正用磁石構体は、リン
グ状磁石の内径を陰極線管のネック部の外形より僅かに
大きい寸法に形成するとともに中心軸と同軸の押出部を
形成し、両端に配設される支持部材および間に配置され
るスペーサの当該リング状磁石に当接する面に上記押出
部に係合して同軸に保持する突起部もしくは環状の溝部
を形成し、かつ当該支持部材の筒部を上記ネック部の外
壁面に弾性力でもって当接する構成としたものであるか
ら、リング状磁石の小径化が図れるとともに構成部品点
数を少なくでき、安価なコンバーゼンス補正用磁石構体
が得られる効果がある。
[Effects of the Invention] In the convergence correction magnet structure according to the present invention, the inner diameter of the ring-shaped magnet is slightly larger than the outer diameter of the neck portion of the cathode ray tube, and an extruded portion coaxial with the central axis is formed. A protrusion or annular groove that engages with and coaxially holds the extruded portion is formed on the surface of the support member disposed on the support member and the spacer disposed therebetween that abuts the ring-shaped magnet, and the support member Since the cylindrical portion is configured to abut elastically against the outer wall surface of the neck portion, the diameter of the ring-shaped magnet can be reduced, the number of component parts can be reduced, and an inexpensive convergence correction magnet structure can be obtained. It has the effect of

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

第1図はこの発明の一実施例の一部破断側面図、第2図
はこの実施例の一方の支持部材を示す図、第3図はこの
実施例の一方のリング磁石を示す平面図、第4図はこの
実施例の他方のリング磁石を示す平面図、第5図はこの
実施例の他方の支持部材を示す平面図、第6図はこの発
明の他の実施例を示す一部破断側面図、第7図は従来の
補正用磁石構体を示す一部破断側面図、第8図は第7図
の■−■線矢視断面図である。 (5)、(fl)、(?)・・・可変磁界発生装置、(
11)・・・コンバーゼンス補正用磁石構体、(12)
 、 (14)・・・支持部材、(12b) ・・・筒
状部、(12d)、(13a) −・突起部。 (13)・・・スペーサ、(13b) 、(tad)・
・・環状の溝部、(51)、(52)、(θ1)、 (
lli2) 、(71)、(72)・・・リング状磁石
、(51b) 、(Blb) 、(71b)・・・円弧
状の押出部、(52b) 、(82b) 、(72b)
・・・環状の押出部。 なお、各図中、同一符号は同一、または相当部分を示す
FIG. 1 is a partially cutaway side view of one embodiment of the present invention, FIG. 2 is a diagram showing one support member of this embodiment, and FIG. 3 is a plan view showing one ring magnet of this embodiment. FIG. 4 is a plan view showing the other ring magnet of this embodiment, FIG. 5 is a plan view showing the other support member of this embodiment, and FIG. 6 is a partially broken view showing another embodiment of the present invention. 7 is a partially cutaway side view showing a conventional correction magnet structure, and FIG. 8 is a cross-sectional view taken along the line ■--■ in FIG. 7. (5), (fl), (?)...Variable magnetic field generator, (
11) ... Convergence correction magnet structure, (12)
, (14)...Supporting member, (12b)...Cylindrical part, (12d), (13a)--Protrusion part. (13)...Spacer, (13b), (tad).
...Annular groove, (51), (52), (θ1), (
lli2) , (71), (72)...Ring magnet, (51b), (Blb), (71b)...Circular extrusion part, (52b), (82b), (72b)
...An annular extrusion part. In each figure, the same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] (1)カラー陰極線管のネック部の外径より僅かに大き
い内径に形成されかつ中心軸と同軸の円弧状もしくは環
状の押出部が形成されて回動可能に重ね合わされるとと
もに上記ネック部に挿入されてコンバーゼンス補正用の
磁界を発生する少なくとも一対のリング状磁石と、一対
のリング状磁石と他の一対のリング状磁石との間に介挿
されるスペーサおよび両端部に配置されて上記ネック部
に固着されかつ間に挿入された各一対のリング状磁石お
よびスペーサを挾持する支持部材とを備え、上記支持部
材およびスペーサの上記リング状磁石との当接面に当該
リング状磁石の押出部に係合して管軸に対して同軸に回
転可能に保持する突起部もしくは環状の溝部を形成して
なることを特徴とするコンバーゼンス補正用磁石構体。
(1) An arcuate or annular extruded part is formed with an inner diameter slightly larger than the outer diameter of the neck part of the color cathode ray tube and is coaxial with the central axis, and is rotatably overlapped and inserted into the neck part. at least one pair of ring-shaped magnets that generate a magnetic field for convergence correction, a spacer inserted between one pair of ring-shaped magnets and another pair of ring-shaped magnets, and a spacer disposed at both ends of the neck part. A support member is provided which clamps each pair of ring-shaped magnets and a spacer that are fixedly inserted between each other, and the support member and the spacer have contact surfaces with the ring-shaped magnet that are engaged with the extruded portions of the ring-shaped magnets. 1. A convergence correction magnet structure comprising a protrusion or an annular groove that is rotatably held coaxially with respect to a tube axis.
JP3322388A 1988-02-15 1988-02-15 Magnet composition for convergence correction Pending JPH01209639A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3322388A JPH01209639A (en) 1988-02-15 1988-02-15 Magnet composition for convergence correction

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3322388A JPH01209639A (en) 1988-02-15 1988-02-15 Magnet composition for convergence correction

Publications (1)

Publication Number Publication Date
JPH01209639A true JPH01209639A (en) 1989-08-23

Family

ID=12380450

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3322388A Pending JPH01209639A (en) 1988-02-15 1988-02-15 Magnet composition for convergence correction

Country Status (1)

Country Link
JP (1) JPH01209639A (en)

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