JPH0622103B2 - Deflection-yoke device - Google Patents
Deflection-yoke deviceInfo
- Publication number
- JPH0622103B2 JPH0622103B2 JP61169343A JP16934386A JPH0622103B2 JP H0622103 B2 JPH0622103 B2 JP H0622103B2 JP 61169343 A JP61169343 A JP 61169343A JP 16934386 A JP16934386 A JP 16934386A JP H0622103 B2 JPH0622103 B2 JP H0622103B2
- Authority
- JP
- Japan
- Prior art keywords
- deflection
- coil
- magnetic field
- core
- coils
- 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
Links
- 230000005855 radiation Effects 0.000 description 13
- 230000002411 adverse Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 125000000391 vinyl group Chemical group [H]C([*])=C([H])[H] 0.000 description 3
- 229920002554 vinyl polymer Polymers 0.000 description 3
- 210000003298 dental enamel Anatomy 0.000 description 2
- 238000010894 electron beam technology Methods 0.000 description 2
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 2
- 230000007257 malfunction Effects 0.000 description 2
- 238000004804 winding Methods 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
- H01J29/003—Arrangements for eliminating unwanted electromagnetic effects, e.g. demagnetisation arrangements, shielding coils
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2229/00—Details of cathode ray tubes or electron beam tubes
- H01J2229/0007—Elimination of unwanted or stray electromagnetic effects
- H01J2229/0015—Preventing or cancelling fields leaving the enclosure
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
Description
【発明の詳細な説明】 <産業上の利用分野> 本発明は、例えばテレビジョン受像機、CRTディスプ
レイ装置等の陰極線管上に装着される偏向ヨーク装置の
改良に関する。TECHNICAL FIELD The present invention relates to an improvement in a deflection yoke device mounted on a cathode ray tube such as a television receiver and a CRT display device.
<従来の技術> 周知のように、テレビジョン受像機やCRTディスプレ
イ装置等の陰極線管上に装着される偏向ヨークにおいて
は、通常、水平偏向コイルに対し15.75KHz以上
で120KHz程度までの水平偏向電流を供給し、垂直
偏向コイルに対し60Hz近辺の垂直偏向電流を供給
し、各偏向コイルから発生する水平偏向磁界,垂直偏向
磁界を利用して電子ビームを所定量偏向させ、画面上に
所望の画像を得るものであり、この場合、水平偏向磁
界,垂直偏向磁界共に偏向ヨーク(コア)の外部に対し
漏れ磁界を生じるものである。そして、この外部漏れ磁
界の存在は、偏向ヨークの特性上大きな影響度はなく、
また、偏向ヨーク自体が偏向コイルからの漏れ磁界を利
用して成り立っている装置(部品)であることから、最
近まで、偏向ヨーク自体で外部漏れ磁界を低減しようと
する対策は何等講じられていないものであった。<Prior Art> As is well known, in a deflection yoke mounted on a cathode ray tube of a television receiver, a CRT display device, or the like, normally, a horizontal deflection coil of 15.75 KHz or more to 120 KHz or more is used. A vertical deflection current of about 60 Hz is supplied to the vertical deflection coil, and the electron beam is deflected by a predetermined amount by using the horizontal deflection magnetic field and the vertical deflection magnetic field generated from each deflection coil. An image is obtained. In this case, both the horizontal deflection magnetic field and the vertical deflection magnetic field generate a leakage magnetic field to the outside of the deflection yoke (core). The presence of this external leakage magnetic field does not have a great influence on the characteristics of the deflection yoke,
Further, since the deflection yoke itself is a device (component) that is formed by utilizing the leakage magnetic field from the deflection coil, until recently, no measures have been taken to reduce the external leakage magnetic field by the deflection yoke itself. It was a thing.
これに対し、近来、偏向ヨークが装着された陰極線管に
近接してコンピュータ等の高周波対応の端末機器を配置
する等、映像機器の多様化が進み、従来特に問題となら
なかった偏向ヨークの外部漏れ磁界のうち、周波数の高
い水平偏向磁界の外部漏れ磁界が不要輻射となって、端
末機器等の他機種に誤動作を生じさせる等の悪影響を及
ぼすという懸念が生じ、このため、偏向ヨーク自体で不
要輻射を低減させることが要望されるようになってき
た。On the other hand, recently, the diversification of video equipment such as arranging a high-frequency compatible terminal device such as a computer near a cathode ray tube equipped with a deflection yoke has led to an external deflection yoke which has not been a particular problem. Out of the leakage magnetic field, there is a concern that the external leakage magnetic field of the horizontal deflection magnetic field having a high frequency becomes unnecessary radiation, which may adversely affect other models such as terminal devices and cause adverse effects. There has been a demand for reducing unnecessary radiation.
従来の偏向ヨークにおいては、偏向ヨークの基本原理、
つまり、偏向ヨークは偏向コイルからの漏れ磁界を利用
して電子ビームを所定量偏向すること、の観点から、ご
く一部の偏向ヨークにおいて、偏向ヨークの外周を囲む
ように磁気シールド板を設け、磁気シールド板により不
要輻射を低減させてなるものを除いて、偏向ヨークその
ものに不要輻射を低減させるための手段を何等設けない
ものであった。In the conventional deflection yoke, the basic principle of the deflection yoke,
That is, from the viewpoint that the deflection yoke deflects the electron beam by a predetermined amount by utilizing the leakage magnetic field from the deflection coil, a magnetic shield plate is provided so as to surround the outer periphery of the deflection yoke in a small portion of the deflection yoke. The deflection yoke itself is not provided with any means for reducing the unwanted radiation, except for the one in which the unwanted radiation is reduced by the magnetic shield plate.
<発明が解決しようとする問題点> しかしながら、従来の偏向ヨークの外周を囲むようにシ
ールド板を設けるものにおいては、形状的に大型になる
という問題点があり、特性的にシールド板が不要輻射
(外部漏れ磁界)を受けて別の偏向磁界を形成し、画面
特性(ランディング,コンバージェンス,偏向歪)に悪
影響を与えるという問題点があった。一方、不要輻射の
低減させるための手段を何等有さない偏向ヨークにおい
ては、前述の如く、偏向ヨークに近接する特に高周波対
応の他機種に誤動作を生じさせたり、映像信号の乱れを
生じて正常な画像特性が得られない、等の悪影響を及ぼ
すという問題点があった。<Problems to be Solved by the Invention> However, in the conventional shield yoke that surrounds the outer circumference of the deflection yoke, there is a problem that the shield plate is large in shape, and the shield plate is characteristically unnecessary radiation. There is a problem that another deflection magnetic field is formed in response to the (external leakage magnetic field), and the screen characteristics (landing, convergence, deflection distortion) are adversely affected. On the other hand, in the case of a deflection yoke that does not have any means for reducing unnecessary radiation, as described above, other models that are close to the deflection yoke, especially those that support high frequencies, may malfunction or the video signal may be disturbed, and There is a problem that adverse image effects such as lack of excellent image characteristics are exerted.
<問題点を解決するための手段> 本発明の偏向ヨーク装置は上記問題点を解決するため、
コアと、コアの内面に沿って巻装される一対のくら型の
水平偏向コイルと、該水平偏向コイルの外側に配置され
るトロイダル型若しくはくら型の垂直偏向コイルとを備
える偏向ヨークと、水平偏向コイルに対し直列に一対の
キャンセルコイルを接続し、該キャンセルコイルを、ル
ープ状に巻回形成してコアの外部でコアおよび垂直偏向
コイルから離して配置し、また、その中心を偏向ヨーク
のY軸上若しくはY軸近傍に位置し、かつ、Y軸に対し
直交状に配置するとともに、水平偏向コイルによって発
生する水平偏向磁界のうちコアの外部に漏れる磁界と逆
の磁界を前記キャンセルコイルによって発生させてなる
ものである。<Means for Solving the Problems> The deflection yoke device of the present invention solves the above problems by
A deflection yoke including a core, a pair of hull-shaped horizontal deflection coils wound along the inner surface of the core, and a toroidal or hull-shaped vertical deflection coil arranged outside the horizontal deflection coil; A pair of canceling coils are connected in series to the deflection coil, the canceling coil is wound in a loop and is arranged outside the core away from the core and the vertical deflection coil. The cancel coil is positioned on or near the Y-axis and is arranged orthogonally to the Y-axis, and a magnetic field reverse to the magnetic field leaking to the outside of the core from the horizontal deflection magnetic field generated by the horizontal deflection coil is generated by the cancel coil. It is generated.
<作 用> 一対のキャンセルコイルに水平偏向電流を流して水平偏
向周期のキャンセル磁界を発生させる。<Operation> A horizontal deflection current is applied to a pair of cancel coils to generate a canceling magnetic field with a horizontal deflection period.
また、キャンセルコイルは、偏向ヨークのY軸方向にコ
アおよび垂直偏向コイルから離して配置し、かつ、Y軸
の位置に配置しているので、キャンセル磁界はコアから
の漏れ磁界だけでなくコアの外に出ている水平偏向コイ
ル部分からの放射磁界も低減するとともに、キャンセル
コイルの巻回数を少なく構成し、また、偏向ヨークに対
するキャンセルコイルの取付けおよび電気絶縁を容易に
する。Further, since the cancel coil is arranged apart from the core and the vertical deflection coil in the Y-axis direction of the deflection yoke and at the position of the Y-axis, the cancel magnetic field is not only the leakage magnetic field from the core but also the core. The radiated magnetic field from the horizontal deflection coil portion outside is reduced, the number of windings of the cancel coil is reduced, and the cancel coil is easily attached to and electrically insulated from the deflection yoke.
<実施例> 以下、本発明偏向ヨーク装置の一実施例を図面を用いて
詳細に説明する。第1図乃至第3図においては、1は一
対の半環状コアを接合してなる円環状のコアであり、コ
ア1には、内面に一対のくら型の水平偏向コイル2,3
が巻装され、外周に一対のトロイダル型の垂直偏向コイ
ル4,5が巻装される。6はコア1の内面に配置され水
平偏向コイル2,3と垂直偏向コイル4,5間の絶縁を
保持するコイルボビンであり、コア1,水平偏向コイル
2,3、垂直偏向コイル4,5、コイルボビン6によっ
て偏向ヨーク本体7を構成する。偏向ヨーク本体7の一
部をなす水平偏向コイル2,3には、第4図に示すよう
に、水平偏向コイル2,3に対して直列に一対のキャン
セルコイル8,9が接続される。キャンセルコイル8,
9はそれぞれ銅線の外周を絶縁材料で被覆した、例え
ば、ビニール被覆リード線やエナメル線、或は、プリン
ト配線基板等から構成される。また、キャセルコイル
8,9は、第1図および第2図に示すように、コア1お
よび垂直偏向コイル4,5の外面から離して、かつ、各
々の中心8T,9Tを偏向ヨーク(偏向ヨーク本体7)
のY軸上(垂直軸上)に位置して長方形状にループ状に
形成し、かつ、Y軸に対して直交状に位置して巻回配置
してなるもので、コイルボビン6に設けた係止部10に
係合(嵌合)した状態で、偏向ヨーク本体7に対する取
着固定がなされるものである。そして、キャンセルコイ
ル8,9により、水平偏向コイル2,3によって発生す
る水平偏向磁界のうち偏向ヨーク本体7の一部をなすコ
ア1の外部に漏れる磁界(不要輻射)と逆の磁界(キャ
ンセル磁界)をキャンセルコイル8,9の各々の両側部
8E,8F,9E,9F側で発生するものである。ここ
で、本実施例においては、キャンセルコイル8,9とし
て、ビニール被覆リード線を5ターン(図面上は簡略化
のため3ターンのみ示す)用いて巻回して構成するが、
キャンセルコイル8,9のターン数は、不要輻射の程
度、或は水平偏向コイルのインピーダンスとの関係によ
り適宜に増減ができるものである。<Example> Hereinafter, an example of the deflection yoke device of the present invention will be described in detail with reference to the drawings. 1 to 3, reference numeral 1 denotes an annular core formed by joining a pair of semi-annular cores. The core 1 has a pair of paddle-shaped horizontal deflection coils 2 and 3 on the inner surface thereof.
And a pair of toroidal vertical deflection coils 4 and 5 are wound around the outer circumference. Reference numeral 6 denotes a coil bobbin arranged on the inner surface of the core 1 for maintaining insulation between the horizontal deflection coils 2 and 3 and the vertical deflection coils 4 and 5, and includes the core 1, the horizontal deflection coils 2 and 3, the vertical deflection coils 4 and 5, and the coil bobbin. The deflection yoke body 7 is constituted by 6. As shown in FIG. 4, a pair of cancel coils 8 and 9 are connected to the horizontal deflection coils 2 and 3 forming a part of the deflection yoke body 7 in series with the horizontal deflection coils 2 and 3. Cancel coil 8,
Reference numeral 9 is composed of, for example, a vinyl-coated lead wire, an enamel wire, or a printed wiring board whose outer circumference is covered with an insulating material. Further, as shown in FIGS. 1 and 2, the casel coils 8 and 9 are separated from the outer surfaces of the core 1 and the vertical deflection coils 4 and 5, and their centers 8T and 9T are deflected by a deflection yoke (deflection yoke). Body 7)
Is formed on the Y-axis (on the vertical axis) in a rectangular loop shape, and is wound and arranged orthogonally to the Y-axis. It is attached and fixed to the deflection yoke main body 7 in a state of being engaged (fitted) with the stopper 10. Then, the cancel coils 8 and 9 cause a magnetic field (cancellation magnetic field) opposite to the magnetic field (unwanted radiation) leaking to the outside of the core 1 forming part of the deflection yoke main body 7 in the horizontal deflection magnetic fields generated by the horizontal deflection coils 2 and 3. ) Is generated on both side portions 8E, 8F, 9E, 9F of the cancel coils 8, 9. Here, in the present embodiment, the cancel coils 8 and 9 are formed by winding vinyl-coated lead wires using 5 turns (only 3 turns are shown in the drawing for simplification).
The number of turns of the cancel coils 8 and 9 can be appropriately increased or decreased depending on the degree of unnecessary radiation or the relationship with the impedance of the horizontal deflection coil.
斯かる構成の偏向ヨーク装置において、コア1の外部で
各中心8T,9Tを偏向ヨークのY軸上に位置してルー
プ状に形成し、かつ、Y軸に対して直交状に位置して巻
回配置したキャンセルコイル8,9をコア1および垂直
偏向コイル4から離して偏向ヨーク本体7に取着固定し
た状態で所定の配線接続を行なう。然る後、水平偏向コ
イル2,3、垂直偏向コイル4,5、キャンセルコイル
8,9にそれぞれ所定の電流を通電する。電流の通電に
伴い、第5図に示すように、水平偏向コイル2,3によ
って発生する水平偏向磁界HBのうち、コア1(偏向ヨ
ーク本体7)の外部に漏れる磁界、つまり不要輻射HR
に対して、コア1の外部に位置してループ状に形成した
キャンセルコイル8,9によって発生するキャンセル磁
界HCがキャンセルコイル8,9の両側部(8E,8
F、9E,9F)側で逆向きの磁界となり、この結果、
不要輻射HRはキャンセル磁界HCにより打ち消され確
実に低減がなされるものである。In the deflection yoke device having such a configuration, outside the core 1, the centers 8T and 9T are formed on the Y axis of the deflection yoke so as to form a loop, and are wound at positions orthogonal to the Y axis. Predetermined wiring connection is performed in a state where the cancel coils 8 and 9 arranged once are separated from the core 1 and the vertical deflection coil 4 and fixedly attached to the deflection yoke body 7. After that, predetermined currents are applied to the horizontal deflection coils 2 and 3, the vertical deflection coils 4 and 5, and the cancel coils 8 and 9, respectively. As shown in FIG. 5, the horizontal deflection magnetic field H B generated by the horizontal deflection coils 2 and 3 as the current is applied, leaks to the outside of the core 1 (deflection yoke body 7), that is, unnecessary radiation H R
On the other hand, the canceling magnetic field H C generated by the canceling coils 8 and 9 which are formed outside the core 1 and which are formed in a loop shape, causes the canceling magnetic fields H C to occur on both sides (8E and 8E) of the canceling coils 8 and 9.
F, 9E, 9F) side has a reverse magnetic field, and as a result,
The unnecessary radiation H R is canceled by the canceling magnetic field H C and is reliably reduced.
尚、本発明偏向ヨーク装置の一実施例においては、垂直
偏向コイルをコアに対してトロイダル型に巻回したもの
について述べたが、垂直偏向コイルをコアに対してくら
型に巻回して構成しても良いものである。また、本発明
偏向ヨーク装置の一実施例においては、第1図に示すよ
うに、キャンセルコイルをトロイダル型垂直偏向コイル
から離して管軸方向でコア外面に概略沿わせて取着固定
するものについて述べたが、第6図に示すように、キャ
ンセルコイル8,9を係止部10を介して管軸に対して
平行状に取着固定しても良く、この場合、キャンセルコ
イル8,9のコイルボビン6に対する取着固定が簡略化
されるものである。さらに、第7図に示すように、キャ
ンセルコイル8,9をコア1の外表面に沿わせて円弧状
としても良く、この場合、不要輻射に対するキャンセル
コイルの配置が効率良くなされるものである。さらにま
た、キャンセルコイル8,9の形状も実施例の長方形状
に限定されず、例えば、第8図に示すように、キャンセ
ルコイル8(9)を略台形状としてループ状に形成して
も、或は、図示しないが、円形状、長円形状としてルー
プ状に形成しても良く、コア1の外部に位置しループ状
をなし、かつ、Y軸に対して直交状に位置して巻回配置
されるものであれば適宜に変更できるものである。さら
に、本発明の一実施例においては、キャンセルコイルの
中心をY軸上に位置してループ状に形成するものについ
て述べたが、不要輻射に対して有効に作用するものであ
れば、Y軸上に限定されず、中心がY軸近傍に位置して
ループ状に形成しても良いものである。そして、本発明
偏向ヨーク装置の一実施例においては、キャンセルコイ
ルをビニール被覆リード線を用いて構成したが、既に述
べたように、エナメル線,プリント配線基板を用いても
良いものである。In the embodiment of the deflection yoke device of the present invention, the vertical deflection coil is wound around the core in a toroidal shape, but the vertical deflection coil is wound around the core in a square shape. It is also good. In one embodiment of the deflection yoke device of the present invention, as shown in FIG. 1, the cancel coil is attached and fixed so as to be separated from the toroidal type vertical deflection coil along the tube outer surface substantially along the outer surface of the core. As described above, as shown in FIG. 6, the cancel coils 8 and 9 may be attached and fixed in parallel to the tube axis via the locking portion 10. In this case, the cancel coils 8 and 9 are The attachment and fixing to the coil bobbin 6 is simplified. Further, as shown in FIG. 7, the cancel coils 8 and 9 may be formed in an arc shape along the outer surface of the core 1. In this case, the cancel coils are efficiently arranged with respect to unnecessary radiation. Furthermore, the shape of the cancel coils 8 and 9 is not limited to the rectangular shape of the embodiment. For example, as shown in FIG. 8, even if the cancel coil 8 (9) is formed in a substantially trapezoidal shape in a loop shape, Alternatively, although not shown, it may be formed in a loop shape as a circular shape or an oval shape, and is formed outside the core 1 to form a loop shape, and is wound in a shape orthogonal to the Y axis. It can be appropriately changed as long as it is arranged. Further, in the embodiment of the present invention, the center of the cancel coil is located on the Y-axis and is formed in a loop, but the Y-axis can be used as long as it effectively acts on unwanted radiation. The present invention is not limited to the above, and the center may be located in the vicinity of the Y axis to form a loop. Further, in one embodiment of the deflection yoke device of the present invention, the cancel coil is constituted by using the vinyl coated lead wire, but as described above, the enamel wire or the printed wiring board may be used.
<発明の効果> 本発明の偏向ヨーク装置は以上詳細に述べたとおりであ
り、以下に示す効果を生じるものである。(イ) キャンセ
ルコイルに水平偏向電流を流すので、コアの外部に漏れ
てくる水平偏向周期の漏れ磁界の強さに左右されること
なく、独自の磁界強度のキャンセル磁界を発生すること
ができ、コアからの漏れ磁界ばかりかコアの外に出てい
る水平偏向コイル部分から放射される磁界も確実に低減
することができる。この結果、不要輻射の低減が確実に
なされ、画面特性(ランディング,コンバージェンス,
偏向歪)に悪影響を与えることなく、偏向ヨークに近接
する他機種(コンピュータの端末装置等)に誤動作を生
じさせたり、映像信号の乱れを生じたりする懸念がなく
なるものである。(ロ) キャンセルコイルを、偏向ヨーク
のY軸方向にコア及び垂直偏向コイルから離してコアの
外部に漏れる磁界の磁界強度が少し弱くなる位置に配置
するので、キャンセルコイルの巻回数が少なくて良く、
また、コイル自体を軽量に構成できるのでキャンセルコ
イルの保持が容易になる。<Effects of the Invention> The deflection yoke device of the present invention is as described in detail above, and produces the following effects. (B) Since a horizontal deflection current is passed through the cancel coil, it is possible to generate a cancellation magnetic field with its own magnetic field strength without being influenced by the strength of the leakage magnetic field of the horizontal deflection period that leaks to the outside of the core. It is possible to surely reduce not only the leakage magnetic field from the core but also the magnetic field emitted from the horizontal deflection coil portion outside the core. As a result, the unwanted radiation is reliably reduced and the screen characteristics (landing, convergence,
It does not adversely affect the deflection distortion) and eliminates the risk of causing malfunction in other models (computer terminal devices, etc.) close to the deflection yoke, and disturbance of the video signal. (B) Since the cancel coil is arranged in the Y-axis direction of the deflection yoke away from the core and the vertical deflection coil at a position where the magnetic field strength of the magnetic field leaking to the outside of the core is slightly weakened, the number of turns of the cancel coil may be small. ,
Further, since the coil itself can be configured to be lightweight, it becomes easy to hold the cancel coil.
また、キャンセルコイルを偏向ヨークのY軸部分に配置
するので、水平偏向周期の漏れ磁界の一番多い位置にキ
ャンセルコイルを配置でき、偏向ヨークから放射する水
平偏向周期の漏れ磁界を効率よく低減することができ
る。Further, since the cancel coil is arranged in the Y-axis portion of the deflection yoke, the cancel coil can be arranged at the position where the leakage magnetic field of the horizontal deflection period is the largest, and the leakage magnetic field of the horizontal deflection period radiated from the deflection yoke can be efficiently reduced. be able to.
(ハ) キャンセルコイルを偏向ヨーク本体とは別体に別途
独立して形成することができ、かつ、偏向ヨーク本体に
対する取着固定(装着)もループ状に形成したものを直
接係止固定すれば良く極めて容易となるもので、生産
性,作業性が著しく向上し、量産性に富むものである。
このように、本発明の偏向ヨーク装置は種々の効果を有
し、特に高周波対応の映像機器用として今後益々有効と
なるものである。(C) The cancel coil can be separately formed separately from the deflection yoke body, and if the deflection coil body is attached and fixed (installed) in a loop shape, it can be directly locked and fixed. Good and extremely easy, productivity and workability are remarkably improved, and mass productivity is high.
As described above, the deflection yoke device of the present invention has various effects, and will be more and more effective in the future especially for high-frequency compatible video equipment.
第1図は本発明偏向ヨーク装置の一実施例における側面
図、第2図は第1図のII−II線断面図、第3図は本発明
偏向ヨーク装置の一実施例における要部概略上面図、第
4図は同じく水平偏向コイルとキャンセルコイルとの接
続状態を示す回路図、第5図は同じく水平偏向コイルと
キャンセルコイルによって発生する磁界の状態を示す偏
向ヨーク本体の頭部側から見た説明図、第6図は本発明
偏向ヨーク装置の他の実施例における概略側面図、第7
図は同じく更に他の実施例における要部断面図、第8図
は同じく更に他の実施例における上面(下面)図であ
る。 1……コア、2,3……水平偏向コイル、4,5……垂
直偏向コイル、8,9……キャンセルコイル、FIG. 1 is a side view of an embodiment of the deflection yoke device of the present invention, FIG. 2 is a sectional view taken along line II-II of FIG. 1, and FIG. 3 is a schematic top view of an essential part of the embodiment of the deflection yoke device of the present invention. FIG. 4 and FIG. 4 are circuit diagrams showing a connection state of the horizontal deflection coil and the cancel coil, and FIG. 5 shows a state of a magnetic field generated by the horizontal deflection coil and the cancel coil as seen from the head side of the deflection yoke body. And FIG. 6 is a schematic side view of another embodiment of the deflection yoke device of the present invention.
FIG. 8 is a sectional view of an essential part of the still another embodiment, and FIG. 8 is an upper surface (lower surface) view of the still another embodiment. 1 ... Core, 2, 3 ... Horizontal deflection coil, 4, 5 ... Vertical deflection coil, 8, 9 ... Cancellation coil,
Claims (1)
一対のくら型の水平偏向コイルと、該水平偏向コイルの
外側に配置されるトロイダル型若しくはくら型の垂直偏
向コイルとを備える偏向ヨークと、前記水平偏向コイル
に対し直列に一対のキャンセルコイルを接続し、該キャ
ンセルコイルを、ループ状に巻回形成して前記コアの外
部で前記コアおよび前記垂直偏向コイルから離して配置
し、また、その中心を前記偏向ヨークのY軸上若しくは
Y軸近傍に位置し、かつ、Y軸に対し直交状に配置する
とともに、前記水平偏向コイルによつて発生する水平偏
向磁界のうち前記コアの外部に漏れる磁界と逆の磁界を
前記キャンセルコイルから発生させることを特徴とする
偏向ヨーク装置。1. A core, a pair of saddle-shaped horizontal deflection coils wound along the inner surface of the core, and a toroidal or saddle-shaped vertical deflection coil arranged outside the horizontal deflection coil. A deflection yoke is provided, and a pair of cancel coils are connected in series to the horizontal deflection coil, and the cancel coils are wound in a loop shape and arranged outside the core and apart from the core and the vertical deflection coil. The center of the horizontal deflection magnetic field is located on or near the Y-axis of the deflection yoke and is orthogonal to the Y-axis, and the horizontal deflection magnetic field generated by the horizontal deflection coil is A deflection yoke device, wherein a magnetic field reverse to a magnetic field leaking to the outside of the core is generated from the cancel coil.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61169343A JPH0622103B2 (en) | 1986-07-18 | 1986-07-18 | Deflection-yoke device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61169343A JPH0622103B2 (en) | 1986-07-18 | 1986-07-18 | Deflection-yoke device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6326928A JPS6326928A (en) | 1988-02-04 |
| JPH0622103B2 true JPH0622103B2 (en) | 1994-03-23 |
Family
ID=15884800
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61169343A Expired - Lifetime JPH0622103B2 (en) | 1986-07-18 | 1986-07-18 | Deflection-yoke device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0622103B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0488647U (en) * | 1990-12-17 | 1992-07-31 | ||
| EP1981049B1 (en) | 2006-02-02 | 2012-08-15 | Idec Corporation | Push button switch device |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4865116U (en) * | 1971-11-24 | 1973-08-18 | ||
| JPS59197198A (en) * | 1983-04-22 | 1984-11-08 | 株式会社トーキン | Magnetic shielding device |
| JPS6264024A (en) * | 1985-09-13 | 1987-03-20 | Mitsubishi Electric Corp | Unnecessary radiation preventer |
-
1986
- 1986-07-18 JP JP61169343A patent/JPH0622103B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6326928A (en) | 1988-02-04 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |