JPH01154442A - Cathode-ray tube display device - Google Patents

Cathode-ray tube display device

Info

Publication number
JPH01154442A
JPH01154442A JP31212087A JP31212087A JPH01154442A JP H01154442 A JPH01154442 A JP H01154442A JP 31212087 A JP31212087 A JP 31212087A JP 31212087 A JP31212087 A JP 31212087A JP H01154442 A JPH01154442 A JP H01154442A
Authority
JP
Japan
Prior art keywords
ray tube
coil
horizontal
coils
magnetic flux
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
JP31212087A
Other languages
Japanese (ja)
Inventor
Manabu Tamura
学 田村
Akiyoshi Matsunaga
松永 明義
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 JP31212087A priority Critical patent/JPH01154442A/en
Publication of JPH01154442A publication Critical patent/JPH01154442A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To prevent a reduction in life and an increase in weight due to an increase in temperature in internal electronic circuits by winding a cancel coil along the circumferential direction of a magnetic shield member provided along the openly diffusing surface of a funnel section. CONSTITUTION:A device is equipped with a cathode-ray tube 1 provided with a magnetic shield 8 on the openly diffusing surface of a funnel section 16, with a circular coil approximately in a cylindrical form to be fixed on the narrow section of the aforesaid cathode-ray tube 1, with horizontal coils 3 and 4 provided along the inner circumferential surface of the circular core 2, with a vertical coil wound by the circular core 2, and with cancel coils 21 and 22 wound along the circumferential direction of the magnetic shield member 8. And horizontal deflection current or its high frequency current is applied to the concel coils 21 and 22 in such a way that a magnetic field induced from the front side of the horizontal coil is concelled or reduced. This constitution thereby can prevent a reduction in life and an increase in weight due to an increase in temperature in internal electronic circuits.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は陰極線管(以下CRTという)において高エ
ネルギーの電子ビームを用いる場合に、この電子ビーム
を電磁的に偏向させる陰極線管表示装置の改良に関する
ものである。
[Detailed Description of the Invention] [Field of Industrial Application] This invention is an improvement of a cathode ray tube display device that electromagnetically deflects a high-energy electron beam when a cathode ray tube (hereinafter referred to as CRT) uses a high-energy electron beam. It is related to.

〔従来の技術〕[Conventional technology]

第4図は例えばrNHKカラーテレビ受信技術」P19
4 (日本放送協会昭和62年4月10日発行)に示さ
れた従来の陰極線管表示装置の一例を示す側面図であり
、図において、■はCRT、2はCRTIの細径部1a
(電子銃近傍)部分に取り付けられる略円筒形の環状コ
ア(トロイダルコア)、3.4は上記環状コア2の内周
面に沿って略水平方向に対向して配置された水平コイル
、5゜6は上記環状コア2に巻回されて上記水平コイル
3.4の磁束と直交する方向の磁束を生じさせる垂直コ
イルで、これら水平コイル3,4と垂直コイル5.6と
により偏向ヨーク7を構成する。8はCRTIのファン
ネル部1bの拡開面に沿って設けられた磁気シールド部
材である。なお、第5図においては6011□付近の周
波数で駆動される垂直コイル5.6は西独の電磁波不要
輻射規制規格VDEO871の磁束領域(Magnet
ic fieldnoise )で規制する範囲がl0
KH2からであり、その高調波もレベルが限度に及ばな
いので、説明を簡単にするために省略する。
Figure 4 shows, for example, "rNHK color television reception technology" P19
4 (published by Japan Broadcasting Corporation on April 10, 1986) is a side view showing an example of a conventional cathode ray tube display device, in which ■ is a CRT, and 2 is a narrow diameter portion 1a of a CRTI.
(near the electron gun) a substantially cylindrical annular core (toroidal core); 3.4 is a horizontal coil disposed substantially horizontally facing each other along the inner peripheral surface of the annular core 2; A vertical coil 6 is wound around the annular core 2 and generates a magnetic flux in a direction perpendicular to the magnetic flux of the horizontal coil 3.4.The horizontal coils 3, 4 and the vertical coil 5.6 form a deflection yoke 7. Configure. 8 is a magnetic shielding member provided along the expanded surface of the funnel portion 1b of the CRTI. In addition, in Fig. 5, the vertical coil 5.6 driven at a frequency around 6011□ is in the magnetic flux region (Magnet
ic field noise) is regulated by 10
KH2, and the level of its harmonics does not reach the limit, so they will be omitted to simplify the explanation.

次に動作について説明する。Next, the operation will be explained.

原理的には水平コイル3,4は水平磁束を発生し、垂直
コイル5.6は垂直磁束を発生する。このため、この2
方向の磁束を有する磁界が環状コア2の中心に形成され
る。また、上記水平磁束と垂直磁束とは水平コイル3,
4および垂直コイル5.6に流れる電流量により磁界の
強さが変化する。そして、この磁界により上記環状コア
2の中央部分を挿通したCRTIの細径部la内を通過
する電子ビームが偏向されてCRTIに画像を形成する
ことになる。すなわち、第5図において、偏向ヨーク7
の水平コイル3.4に符号9,10で示すような電流が
流れると、実線矢印で示すような水平磁束11が発生し
、符号11で示すように偏向する。
In principle, the horizontal coils 3, 4 generate a horizontal magnetic flux, and the vertical coils 5.6 generate a vertical magnetic flux. For this reason, these two
A magnetic field with directional magnetic flux is formed at the center of the annular core 2. In addition, the horizontal magnetic flux and vertical magnetic flux mentioned above are the horizontal coil 3,
The strength of the magnetic field changes depending on the amount of current flowing through the vertical coils 4 and 5.6. This magnetic field deflects the electron beam passing through the narrow diameter portion la of the CRTI that has passed through the central portion of the annular core 2, thereby forming an image on the CRTI. That is, in FIG. 5, the deflection yoke 7
When currents as shown by symbols 9 and 10 flow through the horizontal coils 3.4, a horizontal magnetic flux 11 as shown by the solid arrow is generated and deflected as shown by the symbol 11.

ところで、水平コイル3.4の前端3a、4aおよび後
端3b、4bの符号9,10で示す電流方向が変化する
場所ではそれぞれ磁束12,13゜14.15が発生す
ると共に、これらの磁界発生メカニズムにより電子ビー
ムの偏向には特に寄与しない不要輻射磁束16.17が
発生する。この不要輻射磁束16.17のレヘルは偏向
ヨーク7の前部側が大きく開口しているためと、(磁束
12゜13の線路長が磁束14.15に較べ長いために
不要輻射磁束17が大きくなっている。この従来の偏向
ヨーク装置を内蔵したデイスプレィモニタまたはテレビ
ジョンを西独の不要輻射規制規格■DEO877の測定
方法で測定したときの磁束を第6図に示すと、偏向ヨー
ク7の前側磁束18゜19.20は地面の透磁率が空気
中より大きいため地面でループしている。なお、第6図
中DMはデイスプレィモニタ、EMIは不要輻射測定用
ループアンテナである。
By the way, magnetic fluxes of 12, 13° and 14.15 degrees are generated at the locations where the current directions shown by the symbols 9 and 10 at the front ends 3a, 4a and rear ends 3b, 4b of the horizontal coil 3.4 change, respectively, and these magnetic fields are generated. This mechanism generates unnecessary radiated magnetic flux 16,17 that does not particularly contribute to the deflection of the electron beam. The level of this unnecessary radiated magnetic flux 16.17 is due to the large opening on the front side of the deflection yoke 7, and (because the line length of the magnetic flux 12°13 is longer than that of the magnetic flux 14.15), the unnecessary radiated magnetic flux 17 becomes large. Figure 6 shows the magnetic flux when a display monitor or television equipped with this conventional deflection yoke device is measured using the measurement method of the West German unnecessary radiation control standard DEO877.The front magnetic flux of the deflection yoke 7 is 18°19.20 is a loop on the ground because the magnetic permeability of the ground is greater than that of air.In addition, in Fig. 6, DM is a display monitor, and EMI is a loop antenna for measuring unnecessary radiation.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来の陰極線管表示装置は以上のように構成されている
ので、偏向ヨーク7から発生する不要輻射磁束16の影
害を与えないようにするために、鉄板やパーマロイなど
の透磁率の高い材料で磁路をショートループさせなげれ
ばならず、電子回路を含めCRTlや偏向ヨーク7を鉄
板で囲んだりするため、内部電子回路の温度上昇による
寿命低下や重量増を招いたりしてサービスの悪化を招く
するという問題点があった。
Since the conventional cathode ray tube display device is constructed as described above, in order to prevent the influence of the unnecessary radiation magnetic flux 16 generated from the deflection yoke 7, it is made of a material with high magnetic permeability such as an iron plate or permalloy. The magnetic path must be made into a short loop, and the CRTl and deflection yoke 7, including the electronic circuits, are surrounded by iron plates, which reduces the service life and increases weight due to the temperature rise of the internal electronic circuits, resulting in deterioration of service. There was a problem with inviting people.

この発明は上記のような問題点を解消するためになされ
たもので、内部電子回路の温度上昇による寿命の低下や
重量増を招かないようにした陰極線管表示装置を得るこ
とを目的とする。
The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide a cathode ray tube display device that does not cause a decrease in life or an increase in weight due to a rise in temperature of internal electronic circuits.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る陰極線管表示装置はファンネル部の拡開
面に磁気シールド部材を施した陰極線管と、この陰極線
管の細径部分に取り付けられる略円筒形の環状コアと、
この環状コアの内周面に沿って設けられる水平コイルと
、上記環状コアに巻回される垂直コイルと、上記磁気シ
ールド部材の周囲方向に沿って巻回したキャンセルコイ
ルとを備えたものである。
A cathode ray tube display device according to the present invention includes: a cathode ray tube in which a magnetic shielding member is provided on the expanded surface of the funnel portion; a substantially cylindrical annular core attached to a narrow diameter portion of the cathode ray tube;
A horizontal coil provided along the inner peripheral surface of the annular core, a vertical coil wound around the annular core, and a canceling coil wound along the circumferential direction of the magnetic shielding member. .

〔作用〕[Effect]

この発明における陰極線管表示装置はファンネル部の拡
開面に沿って設けられる磁気シールド部材の周囲方向に
沿って巻回させたキャンセルコイルに水平偏向電流また
はその高調波電流を流すことで水平コイルの前側から発
生する磁界をキャンセルまた°は減少させるようにした
ものである。
The cathode ray tube display device according to the present invention has a horizontal deflection current or its harmonic current flowing through a canceling coil wound along the circumferential direction of a magnetic shielding member provided along an expanded surface of a funnel portion. It is designed to cancel or reduce the magnetic field generated from the front side.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明する。第1
図はこの発明の一実施例を示す断面図であって、第1図
において第4図と同一または均等部分には同一符号を付
して重複説明を省略する。
An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure is a sectional view showing one embodiment of the present invention, and the same or equivalent parts in FIG. 1 as in FIG. 4 are given the same reference numerals, and redundant explanation will be omitted.

第1図において、21.22はファンネル部tbの拡開
面外側に沿って設けられた磁気シールド部材8の周囲方
向に沿って巻回されるキャンセルコイルで、このキャン
セルコイル2L22は偏向ヨーク7の上側水平コイル3
の前側から発生する不要輻射磁束16を弯曲させるため
のものである。
In FIG. 1, reference numerals 21 and 22 denote cancel coils wound along the circumferential direction of the magnetic shielding member 8 provided along the outside of the expanded surface of the funnel portion tb, and this cancel coil 2L22 is attached to the deflection yoke 7. Upper horizontal coil 3
This is for bending unnecessary radiant magnetic flux 16 generated from the front side.

また、キャンセルコイル21.22には水平コイル3,
4に流す水平偏向電流またはその高調波電流、但し高調
波周波数はn倍(nは1〜5程度)、の電流を流す。
In addition, the horizontal coil 3,
4 or its harmonic current, where the harmonic frequency is n times (n is about 1 to 5).

次の動作について説明する。The following operation will be explained.

第2図において、偏向ヨーク7の水平コイル3゜4に符
号9.10で示すような電流を流すと、実線矢印で示す
ような水平磁束Hが発生ずる。また、キャンセルコイル
21.22に水平偏向電流またはその高調波電流を流し
た場合、磁束23.24が発生する。よって、水平コイ
ル3.4の前端3a、4aの符号9.10で示す電流方
向が変化する場所に発生するそれぞれの磁束25.26
はキャンセルコイル21.22の磁束23.24の影響
を受けて、磁束25は減磁し、また磁束26は増磁する
ので、これらの磁界発生メカニズムにより電子ビームの
偏向には特に寄与しない不要幅磁束17は第2図に示す
ように弯曲する。
In FIG. 2, when a current as indicated by reference numeral 9.10 is passed through the horizontal coil 3.4 of the deflection yoke 7, a horizontal magnetic flux H as indicated by the solid arrow is generated. Furthermore, when a horizontal deflection current or its harmonic current is passed through the canceling coils 21 and 22, magnetic fluxes 23 and 24 are generated. Therefore, each magnetic flux 25.26 generated at the front end 3a, 4a of the horizontal coil 3.4 at the location where the current direction indicated by reference numeral 9.10 changes.
is influenced by the magnetic fluxes 23 and 24 of the canceling coils 21 and 22, and the magnetic flux 25 is demagnetized and the magnetic flux 26 is magnetized, so these magnetic field generation mechanisms create an unnecessary width that does not particularly contribute to the deflection of the electron beam. The magnetic flux 17 is curved as shown in FIG.

したがって、磁気シールド部材8にキャンセルコイル2
1.22が施されたデイスプレィモニタDMまたはテレ
ビジョンなどの陰極線管表示装置を西独の不要輻射規制
規格VDEO877の測定方法で測定したときの磁界を
第3図に示すと、偏向ヨーク7の前側磁束18,19.
20は強く地面側に弯曲し、不要輻射測定用ループアン
テナEMIでは検出されなくなる。また、偏向ヨーク7
の後側磁束は空中側に弯曲するもののもともと小さな磁
束であるために妨害源とはならない。
Therefore, the canceling coil 2 is attached to the magnetic shielding member 8.
Figure 3 shows the magnetic field when measuring a cathode ray tube display device such as a display monitor DM or television equipped with 1.22 using the measurement method of the West German unnecessary radiation control standard VDEO877. Magnetic flux 18, 19.
20 is strongly curved toward the ground and is no longer detected by the loop antenna EMI for measuring unnecessary radiation. In addition, the deflection yoke 7
Although the magnetic flux on the rear side curves toward the air, it is originally a small magnetic flux and does not become a source of interference.

なお、上記実施例ではキャンセルコイル21゜22に水
平偏向電流を流すように説明したが、水平偏向電流のn
倍の周波数の高調波電流を流した場合はn倍の不要輻射
成分を強く打ち消すことができる。
In the above embodiment, the horizontal deflection current is passed through the canceling coils 21 and 22, but the horizontal deflection current n
When a harmonic current with twice the frequency is passed, it is possible to strongly cancel n times as many unnecessary radiation components.

〔発明の効果〕〔Effect of the invention〕

以上のようにこの発明によれば陰極線管表示装置をファ
ンネル部の拡開面に沿って設けられた磁気シールド部材
の周囲方向に沿ってキャンセルコイルを巻回させて構成
したので、水平コイルの前側不要輻射磁束を対地側に弯
曲させることができ、特に磁気シールドさせる材料を用
いることなく、不要輻射対策が行え、内部電子回路の温
度上昇に伴う寿命の低下や重量増を招かないようにした
安価な装置が得られる効果がある。
As described above, according to the present invention, the cathode ray tube display device is constructed by winding the canceling coil along the circumferential direction of the magnetic shielding member provided along the expanded surface of the funnel portion. The unnecessary radiation magnetic flux can be curved toward the ground side, and unnecessary radiation measures can be taken without using any special magnetic shielding materials.It is an inexpensive product that does not reduce the lifespan or increase the weight due to the temperature rise of the internal electronic circuit. This has the effect of providing a suitable device.

【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による陰極線管表示装置を
示す断面図、第2図は第、1図の動作を説明するための
陰極線管表示装置の概念図、第3図はこの発明の陰極線
管表示装置を用いて不要輻射磁束を測定した場合の磁束
分布を示す側面図、第4図は従来の陰極線管表示装置の
一例を示す一部切欠側面図、第5図は第4図の動作を説
明するための陰極線管表示装置の概念図、第6図は従来
の陰極線管表示装置を用いて不要輻射磁束を測定した場
合の磁束分布を示す側面図である。 ■は陰極線管(CRT) 、1 bはファンネル部、2
は環状コア、3,4は水平コイル、5,6は垂直コイル
、8は磁気シールド部材、21.22はキャンセルコイ
ル。 なお、図中同一符号は同一または相当部分を示す。 (外2名) 第 2 因 第3図 第 4 空 5.6:叡直コイ1し 第 52 第6フ
FIG. 1 is a sectional view showing a cathode ray tube display device according to an embodiment of the present invention, FIG. 2 is a conceptual diagram of the cathode ray tube display device for explaining the operations of FIGS. A side view showing the magnetic flux distribution when unnecessary radiated magnetic flux is measured using a cathode ray tube display device, FIG. 4 is a partially cutaway side view showing an example of a conventional cathode ray tube display device, and FIG. FIG. 6 is a conceptual diagram of a cathode ray tube display device for explaining the operation. FIG. 6 is a side view showing the magnetic flux distribution when unnecessary radiation magnetic flux is measured using a conventional cathode ray tube display device. ■ is a cathode ray tube (CRT), 1 b is a funnel part, 2
is an annular core, 3 and 4 are horizontal coils, 5 and 6 are vertical coils, 8 is a magnetic shielding member, and 21 and 22 are canceling coils. Note that the same reference numerals in the figures indicate the same or corresponding parts. (2 others) 2nd reason Figure 3 4th Sky 5.6: Einako Koi 1 and 52nd 6th floor

Claims (1)

【特許請求の範囲】[Claims]  ファンネル部の拡開面に沿って磁気シールド部材を有
する陰極線管と、この陰極線管の細径部分に取り付けら
れる略円筒形の環状コアと、この環状コアの内周面に沿
って設けられる水平コイルと、上記環状コアに巻回され
る垂直コイルとを備えた陰極線管表示装置において、上
記ファンネル部の拡開面に沿って設けられた磁気シール
ド部材の周囲方向に沿ってキャンセルコイルを巻回した
ことを特徴とする陰極線管表示装置。
A cathode ray tube having a magnetic shielding member along the expanded surface of the funnel portion, a substantially cylindrical annular core attached to the narrow diameter portion of the cathode ray tube, and a horizontal coil provided along the inner peripheral surface of the annular core. and a vertical coil wound around the annular core, wherein a canceling coil is wound along a circumferential direction of a magnetic shielding member provided along an expanded surface of the funnel portion. A cathode ray tube display device characterized by:
JP31212087A 1987-12-11 1987-12-11 Cathode-ray tube display device Pending JPH01154442A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31212087A JPH01154442A (en) 1987-12-11 1987-12-11 Cathode-ray tube display device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP31212087A JPH01154442A (en) 1987-12-11 1987-12-11 Cathode-ray tube display device

Publications (1)

Publication Number Publication Date
JPH01154442A true JPH01154442A (en) 1989-06-16

Family

ID=18025486

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31212087A Pending JPH01154442A (en) 1987-12-11 1987-12-11 Cathode-ray tube display device

Country Status (1)

Country Link
JP (1) JPH01154442A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03182187A (en) * 1989-12-11 1991-08-08 Mitsubishi Electric Corp Cathode-ray tube device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03182187A (en) * 1989-12-11 1991-08-08 Mitsubishi Electric Corp Cathode-ray tube device

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