JPH0735289Y2 - High frequency deflection yoke - Google Patents

High frequency deflection yoke

Info

Publication number
JPH0735289Y2
JPH0735289Y2 JP1986032494U JP3249486U JPH0735289Y2 JP H0735289 Y2 JPH0735289 Y2 JP H0735289Y2 JP 1986032494 U JP1986032494 U JP 1986032494U JP 3249486 U JP3249486 U JP 3249486U JP H0735289 Y2 JPH0735289 Y2 JP H0735289Y2
Authority
JP
Japan
Prior art keywords
deflection
core
circumferential direction
horizontal
coil
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
JP1986032494U
Other languages
Japanese (ja)
Other versions
JPS62144053U (en
Inventor
浩二 中村
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 JP1986032494U priority Critical patent/JPH0735289Y2/en
Publication of JPS62144053U publication Critical patent/JPS62144053U/ja
Application granted granted Critical
Publication of JPH0735289Y2 publication Critical patent/JPH0735289Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】 [産業上の利用分野] この考案は、例えば130KHzのような高い水平偏向周波数
で作動する高密度、高解像度モニタ用の偏向ヨークに関
する。
DETAILED DESCRIPTION OF THE INVENTION Industrial Field This invention relates to deflection yokes for high density, high resolution monitors operating at high horizontal deflection frequencies such as 130 KHz.

[従来の技術] 第4図は従来の高周波用偏向ヨークの正面図、第5図は
その磁気コアの正面図、第6図はその斜視図である。図
において、(1)は磁気コア(以下、「コア」とい
う。)で、その内面(1a)には複数の溝(2)が前縁
(1b)から後縁(1c)まで、中心軸Zに沿う方向に、か
つ、周方向に一定のピツチでもつて軸対称に形成されて
いる。(3)は溝(2)の間の凸部、(4a)は水平偏向
コイル、(4b)は垂直偏向コイル、(5),(6)はコ
ア(1)の前縁(1b)および後縁(1c)にそれぞれ溝
(2)につづいて形成されているガイド溝で、水平・垂
直偏向コイル(4a),(4b)は、それぞれ溝(2)およ
びガイド溝(5),(6)でもつて位置決めされ、か
つ、コア(1)の内面(1a)では、溝(2)内に収容さ
れるように巻装されている。
[Prior Art] FIG. 4 is a front view of a conventional high-frequency deflection yoke, FIG. 5 is a front view of a magnetic core thereof, and FIG. 6 is a perspective view thereof. In the figure, (1) is a magnetic core (hereinafter referred to as "core"), and a plurality of grooves (2) are formed on its inner surface (1a) from the front edge (1b) to the rear edge (1c) of the central axis Z. It is formed axially symmetrically with a constant pitch in the circumferential direction and along the circumferential direction. (3) is a convex portion between the grooves (2), (4a) is a horizontal deflection coil, (4b) is a vertical deflection coil, (5) and (6) are the leading edge (1b) and the rear of the core (1). Guide grooves formed on the edge (1c) following the groove (2). The horizontal and vertical deflection coils (4a) and (4b) are the groove (2) and the guide grooves (5) and (6), respectively. The inner surface (1a) of the core (1) is wound so as to be housed in the groove (2).

このように、水平・垂直偏向コイル(4a),(4b)を、
それぞれ溝(2)内に収めた構成にすると、高周波水平
偏向磁界によつて水平・垂直偏向コイル(4a),(4b)
に生じるうず電流が減少し、ジユール損失が減少するの
で発熱量が減少するとともに、溝(2)の間の凸部
(3)の面が陰極線管のネツクに近づくので偏向感度が
高まり、駆動電力の低減が図れる。
In this way, the horizontal and vertical deflection coils (4a), (4b)
When each of them is housed in the groove (2), horizontal and vertical deflection coils (4a) and (4b) are generated by the high frequency horizontal deflection magnetic field.
The eddy current that occurs in the cathode decreases and the amount of heat generated decreases because the amount of heat generated decreases, and since the surface of the convex portion (3) between the grooves (2) approaches the neck of the cathode ray tube, the deflection sensitivity is increased and the driving power is reduced. Can be reduced.

[考案が解決しようとする問題点] しかし、この従来の偏向ヨークは、溝(2)がコア
(1)の内面(1a)の周方向に、一定のピツチでもつ
て、後縁(1c)から前縁(1b)にわたつて軸対称に形成
されているため、陰極線管に装着したとき、ネツク側と
なる後縁(1c)に近い部分(以下、「ネツク側」とい
う)と、フアンネル側となる前縁(1b)に近い部分(以
下、「フアンネル側」という)の円周方向の角度θに関
する巻線分布関数をあまり変えることができない。この
ため、偏向ヨークのネツク側とフアンネル側の偏向磁界
分布形を、それぞれ所望の分布形に調整することが困難
となり、陰極線管のスクリーン上での色ずれ(ミスコン
バージエンス)が大きくなるとともに、スクリーン上の
ラスタ歪みを方形に修正することが難しいという問題点
があつた。
[Problems to be solved by the invention] However, in this conventional deflection yoke, the groove (2) is held in the circumferential direction of the inner surface (1a) of the core (1) with a constant pitch from the trailing edge (1c). Since it is formed axially symmetrically across the front edge (1b), when it is attached to the cathode ray tube, the portion near the rear edge (1c), which is the neck side (hereinafter referred to as the "neck side"), and the funnel side. The winding distribution function with respect to the angle θ in the circumferential direction of the portion close to the leading edge (1b) (hereinafter, referred to as “funnel side”) cannot be changed so much. For this reason, it becomes difficult to adjust the deflection magnetic field distribution shapes on the neck side and the funnel side of the deflection yoke to the desired distribution shapes, and the color misregistration (misconvergence) on the screen of the cathode ray tube increases. There is a problem that it is difficult to correct the raster distortion on the screen into a square.

この考案は上記のような従来の問題点を解消するために
なされたもので、発熱量の増加及び偏向感度の低下を十
分に抑制しつつ、ファンネル側の巻線分布を所望のもの
にして、色ずれおよびラスタ歪の発生をなくすることが
できる高周波用偏向ヨークを提供することを目的として
いる。
The present invention has been made to solve the above-mentioned conventional problems, and makes it possible to obtain a desired winding distribution on the funnel side while sufficiently suppressing an increase in heat generation amount and a decrease in deflection sensitivity. An object of the present invention is to provide a high-frequency deflection yoke capable of eliminating color misregistration and raster distortion.

[問題点を解決するための手段] この考案に係る高周波用偏向ヨークは、一端が小径をな
し、他端が大径をなすラッパ形状で、上記小径側内面の
周方向に所定のピッチで軸方向に延在する複数の溝を形
成するとともに、上記大径側内面を平坦面に成形した磁
気コア、この磁気コアに巻装されている水平・垂直偏向
コイルとを備え、上記両偏向コイルの上記小径側のコイ
ル辺は上記溝内に埋め込まれて保持され、かつ、上記両
偏向コイルの上記大径側のコイル辺は、それぞれ円周方
向に広げられて所望の巻線分布となるように巻装されて
いることを特徴とするものである。
[Means for Solving the Problems] A high-frequency deflection yoke according to the present invention has a trumpet shape in which one end has a small diameter and the other end has a large diameter, and a shaft is provided at a predetermined pitch in the circumferential direction of the inner surface on the small diameter side. A magnetic core having a plurality of grooves extending in the same direction and having the inner surface on the large diameter side formed into a flat surface, and horizontal and vertical deflection coils wound around the magnetic core. The coil side on the small diameter side is embedded and held in the groove, and the coil sides on the large diameter side of both the deflection coils are expanded in the circumferential direction to have a desired winding distribution. It is characterized by being wrapped.

[作用] この考案によれば、水平・垂直偏向コイルの小径側(ネ
ック側)は、コアの内面に形成されている溝内に収容さ
れて位置決めされており、それら各コイルの周方向の巻
線分布が規制されるのに対して、大径側(ファンネル
側)は、規制がなくて、円周方向に広げて自由に変位さ
せることが可能である。したがって、大径側の巻線分布
を所望の偏向磁界分布形にすることで、色ずれが少な
く、かつ、ラスタ歪のない偏向ヨークが得られる。ま
た、磁界が強く、ジュール損失が多く発生するネック側
の偏向コイル部分は、コア内面に形成した溝内に収容さ
れて位置決めされているので、もともとジュール損失の
少ないファンネル側のコイルは、コア面上に巻装して
も、ジュール損失の増加が少なく、偏向ヨークの発熱対
策として、何らの問題を生じることがない。
[Operation] According to the present invention, the small-diameter side (neck side) of the horizontal / vertical deflection coils is housed and positioned in the groove formed on the inner surface of the core, and the coils are wound in the circumferential direction. While the line distribution is regulated, the large diameter side (funnel side) is not regulated, and it is possible to spread it in the circumferential direction and freely displace it. Therefore, by setting the winding distribution on the large diameter side to a desired deflection magnetic field distribution type, it is possible to obtain a deflection yoke with less color misregistration and raster distortion. In addition, the deflection coil part on the neck side, where the magnetic field is strong and a large amount of Joule loss occurs, is positioned and accommodated in the groove formed on the inner surface of the core. Even if it is wound on the upper side, the increase in Joule loss is small and no problem occurs as a measure against heat generation of the deflection yoke.

[考案の実施例] 第1図はこの考案の一実施例の正面図で、垂直偏向コイ
ルを取り除いて示している。第2図はそのコアの正面
図、第3図は第2図III-III線矢視断面図である。図に
おいて、(7)はコア(1)の後縁(1c)から前縁(1
b)に向う中間部までの内径の小さい範囲Rの内面(1
a)に、周方向に所定ピツチでもつて形成した凸部、
(8)は凸部(5)の間に形成される溝で、コア(1)
の前縁(1b)は、平滑面に形成されている。水平偏向コ
イル(4a)は第1図に示すように、ネツク側の内側の各
コイル辺の部分が、溝(8)内に収容されて位置決めさ
れるとともに、各コイル辺のフアンネル側は図示のよう
に、凸部(7)を出たところで円周方向に広げられて所
望の巻線分布となるようにコア(1)に巻装されてい
る。
[Embodiment of the Invention] FIG. 1 is a front view of an embodiment of the present invention in which a vertical deflection coil is removed. FIG. 2 is a front view of the core, and FIG. 3 is a sectional view taken along the line III-III in FIG. In the figure, (7) is from the trailing edge (1c) to the leading edge (1) of the core (1).
Inner surface (1) in the range R of small inner diameter toward the middle part toward b)
In a), a convex portion formed by holding a predetermined pitch in the circumferential direction,
Reference numeral (8) is a groove formed between the convex portions (5), which is the core (1).
The front edge (1b) of is formed as a smooth surface. As shown in FIG. 1, the horizontal deflection coil (4a) is positioned such that the inner coil sides of the neck side are housed and positioned in the grooves (8), and the funnel side of each coil side is shown in the figure. As described above, the wire is wound around the core (1) so as to be expanded in the circumferential direction at the exit of the convex portion (7) and to have a desired winding distribution.

なお、垂直偏向コイル(4b)も、水平偏向コイル(4a)
と同様に、所望の巻線分布となるにコア(1)に巻装さ
れている。
The vertical deflection coil (4b) is also the horizontal deflection coil (4a).
Similarly, the core (1) is wound so as to have a desired winding distribution.

このように、水平・垂直偏向コイル(4a),(4b)の位
置を規制する凸部(7)をコア(1)の内径が小さい範
囲R内にだけ設けたので、両偏向コイル(4a),(4b)
のネツク側の巻線分布を、それぞれ規制することができ
るとともに、フアンネル側の巻線分布を、自由に設定す
ることができる。
In this way, since the convex portion (7) for regulating the positions of the horizontal / vertical deflection coils (4a) and (4b) is provided only within the range R where the inner diameter of the core (1) is small, both deflection coils (4a) , (4b)
It is possible to restrict the winding distribution on the net side of each of the above and to freely set the winding distribution on the funnel side.

このように、水平・垂直偏向コイル(4a),(4b)をコ
ア(1)に巻装すると、ネツク側の巻線分布は、凸部
(7)を形成した配置でもつて規制でき、他方、フアン
ネル側は、所望の巻線分布に形成することができるの
で、ネツク側およびフアンネル側の偏向磁界分布を、そ
れぞれ所望の分布形にすることができ、色ずれがなく、
かつ、ラスタ歪みのない偏向ヨークが得られる。
When the horizontal / vertical deflection coils (4a) and (4b) are wound around the core (1) in this way, the winding distribution on the neck side can be restricted by the arrangement in which the convex portion (7) is formed, while Since the funnel side can be formed to have a desired winding distribution, the deflection magnetic field distributions on the neck side and the funnel side can be made into desired distribution shapes, respectively, and there is no color shift.
Moreover, a deflection yoke without raster distortion can be obtained.

なお、コア(1)の内面(1a)の内径の大きい範囲F
に、凸部を形成せず、水平偏向コイル(4a)をコア材の
中に埋め込ないことによる偏向ヨークの偏向感度の低下
は小さい。これは、内径の小さい範囲Rにおける偏向磁
界強度より、内径の大きい範囲Fにおける偏向磁界強度
の方が弱く、したがつて、凸部を設けないために生じる
磁界強度の減少は僅かで、偏向ヨークの偏向感度に及ぼ
す影響は小さいからである。
In addition, the range F where the inner diameter of the inner surface (1a) of the core (1) is large
In addition, the decrease in the deflection sensitivity of the deflection yoke due to the fact that the horizontal deflection coil (4a) is not embedded in the core material without forming the convex portion is small. This is because the deflection magnetic field strength in the large inner diameter range F is weaker than the deflection magnetic field strength in the smaller inner diameter range R, and therefore, the decrease in the magnetic field strength caused by not providing the convex portion is slight, and the deflection yoke is small. This has a small effect on the deflection sensitivity of.

また、同様の理由で、水平偏向コイル(4a)のフアンネ
ル側におけるジユール損失も小さいので、凸部の間にコ
イル辺を埋め込まないことによるジユール損失の増加も
僅かで、格別の発熱対策は必要でない。
Also, for the same reason, since the jule loss on the funnel side of the horizontal deflection coil (4a) is also small, the jule loss increase by not embedding the coil side between the convex parts is also small, and no special heat generation measures are required. .

[考案の効果] 以上のように、この考案によれば、一端が小径をなし、
他端が大径をなすラッパ形状で、上記小径側内面の周方
向に所定のピッチで軸方向に延在する複数の溝を形成す
るとともに、上記大径側内面を平坦面に成形した磁気コ
ア、この磁気コアに巻装されている水平・垂直偏向コイ
ルとを備え、上記両偏向コイルの上記小径側のコイル辺
は上記溝内に埋め込まれて保持され、かつ、上記両偏向
コイルの上記大径側のコイル辺は、それぞれ円周方向に
広げられて所望の巻線分布となるように巻装したので、
偏向感度の低下および発熱量の増加を十分に抑制しつ
つ、大径側の巻線分布の調整に自由性があって、色ずれ
およびラスタ歪の生じない良好な高周波用偏向ヨークを
得ることができる。
[Advantage of Invention] As described above, according to this invention, one end has a small diameter,
A magnetic core having a trumpet shape in which the other end has a large diameter, and forming a plurality of grooves axially extending at a predetermined pitch in the circumferential direction of the inner surface of the small diameter side, and molding the inner surface of the large diameter side into a flat surface. And a horizontal / vertical deflection coil wound around the magnetic core, the coil sides of the deflection coils on the small diameter side are embedded and retained in the groove, and the deflection coils of the deflection coil have the large size. Since the coil sides on the radial side are each wound in a circumferential direction to have a desired winding distribution,
It is possible to obtain a good high-frequency deflection yoke that is free from adjustment of winding distribution on the large diameter side and does not cause color misregistration and raster distortion while sufficiently suppressing reduction in deflection sensitivity and increase in heat generation. it can.

【図面の簡単な説明】 第1図ないし第3図はこの一実施例を示す図で、第1図
は垂直偏向コイルを除いた正面図、第2図はその磁気コ
アの正面図、第3図は第2図III-III線矢視断面図、第
4図は従来の高周波用偏向ヨークの正面図、第5図はそ
の磁気コアの正面図、第6図は同じくその斜視図であ
る。 (1)……磁気コア、(1a)……内面、(1b)……前
縁、(1c)……後縁、(4a)……水平偏向コイル、(4
b)……垂直偏向コイル、(7)……凸部、(8)……
溝。 なお、図中、同一符号はそれぞれ同一、または相当部分
を示す。
BRIEF DESCRIPTION OF THE DRAWINGS FIGS. 1 to 3 are views showing this embodiment, FIG. 1 is a front view without a vertical deflection coil, FIG. 2 is a front view of a magnetic core thereof, and FIG. 2 is a sectional view taken along the line III-III in FIG. 2, FIG. 4 is a front view of a conventional high-frequency deflection yoke, FIG. 5 is a front view of its magnetic core, and FIG. 6 is a perspective view thereof. (1) ... magnetic core, (1a) ... inner surface, (1b) ... leading edge, (1c) ... trailing edge, (4a) ... horizontal deflection coil, (4
b) …… Vertical deflection coil, (7) …… Convex part, (8) ……
groove. In the drawings, the same reference numerals indicate the same or corresponding portions.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】一端が小径をなし、他端が大径をなすラッ
パ形状で、上記小径側内面の周方向に所定のピッチで軸
方向に延在する複数の溝を形成するとともに、上記大径
側内面を平坦面に成形した磁気コア、この磁気コアに巻
装されている水平・垂直偏向コイルとを備え、上記両偏
向コイルの上記小径側のコイル辺は上記溝内に埋め込ま
れて保持され、かつ、上記両偏向コイルの上記大径側の
コイル辺は、それぞれ円周方向に広げられて所望の巻線
分布となるように巻装されていることを特徴とする高周
波偏向ヨーク。
1. A trumpet shape in which one end has a small diameter and the other end has a large diameter, and a plurality of grooves extending in the axial direction at a predetermined pitch in the circumferential direction of the inner surface on the small diameter side are formed, and the large diameter is formed. It has a magnetic core whose inner surface on the radial side is formed into a flat surface, and horizontal and vertical deflection coils wound around this magnetic core, and the coil sides on the small diameter side of both deflection coils are embedded and held in the groove. The high-frequency deflection yoke is characterized in that the coil sides on the large diameter side of the both deflection coils are respectively wound in a circumferential direction to have a desired winding distribution.
JP1986032494U 1986-03-06 1986-03-06 High frequency deflection yoke Expired - Lifetime JPH0735289Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1986032494U JPH0735289Y2 (en) 1986-03-06 1986-03-06 High frequency deflection yoke

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1986032494U JPH0735289Y2 (en) 1986-03-06 1986-03-06 High frequency deflection yoke

Publications (2)

Publication Number Publication Date
JPS62144053U JPS62144053U (en) 1987-09-11
JPH0735289Y2 true JPH0735289Y2 (en) 1995-08-09

Family

ID=30839220

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1986032494U Expired - Lifetime JPH0735289Y2 (en) 1986-03-06 1986-03-06 High frequency deflection yoke

Country Status (1)

Country Link
JP (1) JPH0735289Y2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100377285C (en) * 2002-06-07 2008-03-26 松下电器产业株式会社 Deflection yoke and crt device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5183227U (en) * 1974-12-25 1976-07-03

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100377285C (en) * 2002-06-07 2008-03-26 松下电器产业株式会社 Deflection yoke and crt device

Also Published As

Publication number Publication date
JPS62144053U (en) 1987-09-11

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