JPS60160775A - Cathode-ray tube device - Google Patents
Cathode-ray tube deviceInfo
- Publication number
- JPS60160775A JPS60160775A JP1508684A JP1508684A JPS60160775A JP S60160775 A JPS60160775 A JP S60160775A JP 1508684 A JP1508684 A JP 1508684A JP 1508684 A JP1508684 A JP 1508684A JP S60160775 A JPS60160775 A JP S60160775A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- deflection
- external magnetic
- circuit
- ray tube
- 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
Links
Landscapes
- Details Of Television Scanning (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明はカラーテレビジョン等の陰極線管装置に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a cathode ray tube device such as a color television.
このような陰極線管を用いた表示装置においては、表示
品質が外部磁界の影響を受けて低下しやすい欠点を有し
ている。Display devices using such cathode ray tubes have the disadvantage that display quality tends to deteriorate due to the influence of external magnetic fields.
これを防ぐため、従来鉄板を用いた磁気シールドが行な
われているが、十分なシールド効果を得るため(Cは相
当に厚い鉄板で陰極線管を囲う必要があり、重量および
加工性の点で問題がちった。To prevent this, conventional magnetic shielding using iron plates has been used, but in order to obtain a sufficient shielding effect (C), it is necessary to surround the cathode ray tube with a considerably thick iron plate, which poses problems in terms of weight and workability. It was small.
本発明はこのような事情に鑑みてなされたもので、その
目的は、厚いシールド用鉄板を用いずに外部磁界の影響
を排除した陰極線管装置を提供することにある。The present invention has been made in view of the above circumstances, and its object is to provide a cathode ray tube device that eliminates the influence of external magnetic fields without using a thick iron plate for shielding.
このような目的を達成するために、本発明は、外部磁界
を検出する検出器を設け、その検し1月1力に応じて偏
向電流を、当該外部磁界の影響を加えてはじめて外部磁
界がない場合と同様の偏向特性が得ら!する値に補正す
るようにしたものである。In order to achieve such an object, the present invention provides a detector that detects an external magnetic field, and detects a deflection current according to the detected force, and only when the external magnetic field is affected by the external magnetic field. The same deflection characteristics as without it can be obtained! This is corrected to a value that is
以下実施し1」を用いて本発明の詳細な説明する3、〔
実施例〕
第1図は本発明の一実施例を示す構成図である。The present invention will be explained in detail using "Practice 1" below.
Embodiment] FIG. 1 is a configuration diagram showing an embodiment of the present invention.
図において、1は通常のテレビジョン回路を構成する水
平方向同期回路、2は同じく垂直方向同期回路、3は水
平偏向増幅器、4は垂直製向3′fI幅器であり、これ
ら各増幅器から水平偏向コイル5および垂直偏向コイル
6に偏向磁界を発生する電流を供給している。In the figure, 1 is a horizontal synchronization circuit that constitutes a normal television circuit, 2 is also a vertical synchronization circuit, 3 is a horizontal deflection amplifier, and 4 is a vertical 3'fI width amplifier. A current is supplied to the deflection coil 5 and the vertical deflection coil 6 to generate a deflection magnetic field.
これに削し、7は図示しない陰極線管周囲における画面
にイ行なX方向、すなわち水平方向の磁界強度および向
きを検出するX方向磁界検出器、8は同じくY方向の磁
界強度および向きを検出するY方向磁界検出器である。In addition to this, 7 is an X-direction magnetic field detector that detects the magnetic field strength and direction in the X direction, that is, the horizontal direction, which is parallel to the screen around the cathode ray tube (not shown), and 8 also detects the magnetic field strength and direction in the Y direction. This is a Y-direction magnetic field detector.
これら両検出器Iおよび8は、電磁コイル、ホール素子
あるいは磁気抵抗効果素子などを用いた磁界検出器で、
陰極線管の周囲に配置される。Both detectors I and 8 are magnetic field detectors using electromagnetic coils, Hall elements, magnetoresistive elements, etc.
placed around the cathode ray tube.
そこで、これら両磁界検出器・7およびgによシ、陰極
線管周囲のX方向およびY方向の外部磁界を検出し、増
幅器9および10によシ増幅した検出出力をもって、そ
れぞれ水平偏向増幅器3および垂直偏向増幅器4を制御
する。例えば、外部磁界の影響を受けない場合に垂直偏
向増幅器4の出力、すなわち垂直偏向電流が第2図(a
)に示すようなのこぎ多波形を有するものとして、同図
(b)に示すようなY方向外部磁界が存在する場合には
、同図(a)に示したような垂直偏向電流を流したので
は、実際の垂直偏向磁界は当該偏向iC6流により発生
する磁界と上記外部磁界とが重畳したものとなるために
良好な偏向特性が得られない。したがって上記各検出器
7およびgによシこの外部磁界を検出し、その影響を見
込んで同図(e)に示すように垂iri偏向電流を、予
め当該偏向電流による磁界に上記外部磁界が重畳しては
じめて目的の偏向量が得られるように、外部磁界の影響
分を差引いた値に補正する。X方向についても同様で、
検出される外部磁界がX方向のプラス側に存在するとき
はそれを相殺するようにその大きさに応じてマイナス側
に補正し、X方向のマイナス側に存在するときには、同
様にその大きさに応じてプラス側に補正する。Therefore, these two magnetic field detectors 7 and g detect the external magnetic fields in the X and Y directions around the cathode ray tube, and the amplified detection outputs are sent to the horizontal deflection amplifiers 3 and 10, respectively. Controls the vertical deflection amplifier 4. For example, when not affected by an external magnetic field, the output of the vertical deflection amplifier 4, that is, the vertical deflection current is as shown in FIG.
), and when there is an external magnetic field in the Y direction as shown in (b) of the same figure, the vertical deflection current shown in (a) of the same figure is applied. In this case, the actual vertical deflection magnetic field is a superposition of the magnetic field generated by the deflection iC6 flow and the external magnetic field, and therefore good deflection characteristics cannot be obtained. Therefore, each of the above-mentioned detectors 7 and g detects this external magnetic field, and in anticipation of its influence, a vertical deflection current is generated as shown in FIG. Then, the effect of the external magnetic field is subtracted so that the desired amount of deflection is obtained. The same goes for the X direction.
When the detected external magnetic field exists on the positive side of the X direction, it is corrected to the negative side according to its magnitude to cancel it out, and when it exists on the negative side of the X direction, it is corrected to the negative side according to the magnitude. Correct to the positive side accordingly.
これにより実質的に外部磁界の影響を相殺し、設計通り
の偏向特性を得ることができる。This substantially cancels out the influence of the external magnetic field and allows the deflection characteristics as designed to be obtained.
第3図に、本発明を実際のテレビジョン回路に適用した
場合の具体的構成例を示す。同図において100は通常
のテレビジョン回路であり、同期信号SYは、図上省略
したが、映像受信回路において中間周波数に変換されか
つ映像検波を受けた受信信号から振11フ分離によって
取出されて同期分離回路11に入力し、そこで周波数分
離によって水平回期化−gsyHと垂直同期信号syv
とに分離され、それぞれ水平偏向回路101、垂直偏向
回路102に入力する。各同期回路ではそれぞれ上記同
期信号に同期させて偏向磁界発生用ののこぎシ波電流を
水平偏向コイルLHおよび垂直偏向コイルLVに供給す
る。垂直偏向回路102は、のこぎシ波電流を発生させ
る垂直発振回路12、その出力を増11aする垂直ドラ
イブ回路13および偏向コイルLVにのこぎり波電流を
供給する垂直出力回路14から構成される。一種のロー
パスフィルタである積分回路を経て取り出される垂直同
期信号がパルス性雑音等を含寸ず、したがって直接垂直
発振回路12を制御できるのに対し、一種のバイパスフ
ィルタを通して取り出される水平同期信号にはパルス性
雑音などが混入される。このため、何個かの同期信号の
同t+;>1の平均で同期をとる同期AFCが用いられ
、水平偏向回路101は、水平発振回路15、水平ドラ
イブ回路16および水平出力回路1Tの他に位相検波回
路18および積分回路19を備えている。なお、FBT
はアノード高圧発生用のフライバンクトランス、CI、
Cmはコンデンサである。FIG. 3 shows a specific configuration example when the present invention is applied to an actual television circuit. In the figure, reference numeral 100 denotes a normal television circuit, and the synchronizing signal SY, although omitted in the figure, is extracted from the received signal that has been converted to an intermediate frequency and subjected to image detection in the video receiving circuit by 11 frequency separation. It is input to the synchronization separation circuit 11, where the horizontal synchronization signal -gsyH and the vertical synchronization signal syv are separated by frequency separation.
and are input to a horizontal deflection circuit 101 and a vertical deflection circuit 102, respectively. Each synchronization circuit supplies a sawtooth current for generating a deflection magnetic field to the horizontal deflection coil LH and the vertical deflection coil LV in synchronization with the synchronization signal. The vertical deflection circuit 102 includes a vertical oscillation circuit 12 that generates a sawtooth current, a vertical drive circuit 13 that increases its output 11a, and a vertical output circuit 14 that supplies the sawtooth current to the deflection coil LV. While the vertical synchronizing signal extracted through an integrating circuit, which is a type of low-pass filter, does not contain pulse noise and can therefore directly control the vertical oscillation circuit 12, the horizontal synchronizing signal extracted through a type of bypass filter does not contain any pulse noise. Pulse noise etc. are mixed in. For this reason, a synchronous AFC is used that synchronizes with the average of several synchronous signals with the same t+; A phase detection circuit 18 and an integration circuit 19 are provided. In addition, FBT
is a fly bank transformer for anode high voltage generation, CI,
Cm is a capacitor.
これに対し、200はX方向、すなわち水平方向の外部
磁界の寄与分を考慮して水平偏向電流を補正するX方向
補正回路でおる。X方向磁界検出器21によりX方向外
部磁界を検出し、増幅器22によシ増幅し、さらにX方
向補正出力口w524で増幅された検出出力をトランス
TIの1次コイルに加える。X方向ゲイン調整回路23
は、外部磁界の不均一等によりX方向磁界検出器21、
増幅器22およびX方向補正出力回路24では完全に捕
正しきれない分を、補正回路のゲインを手動で調整して
補償するためのものである。トランスTIの2次コイル
は、1端が水平出力回路1Tに接続された水平偏向コイ
ルLHの他端に接続されており、1次コイルの入力が増
加すれば水平偏向コイルLHを流れる水平偏向電流は減
少し、上記入力が減少すれば水平偏向電流は増加する。On the other hand, 200 is an X-direction correction circuit that corrects the horizontal deflection current in consideration of the contribution of an external magnetic field in the X-direction, that is, the horizontal direction. The X-direction external magnetic field is detected by the X-direction magnetic field detector 21, amplified by the amplifier 22, and the amplified detection output is applied to the primary coil of the transformer TI by the X-direction correction output port w524. X direction gain adjustment circuit 23
Due to the non-uniformity of the external magnetic field, the X-direction magnetic field detector 21,
This is to compensate for the amount that cannot be completely captured by the amplifier 22 and the X-direction correction output circuit 24 by manually adjusting the gain of the correction circuit. One end of the secondary coil of the transformer TI is connected to the horizontal deflection coil LH which is connected to the horizontal output circuit 1T, and when the input to the primary coil increases, the horizontal deflection current flowing through the horizontal deflection coil LH increases. decreases, and if the above input decreases, the horizontal deflection current increases.
同じ(,300はY方向、すなわち垂直方向の外部磁界
の寄与分を考だして手直偏向電流を補正するY方向補正
回路であり、Y方向磁界検出器31、増軒器?2、Y方
向ゲイン開立回路33、Y方向補正出力口[334:I
、−よびこのY方向補正出力回路34の出力を1次コイ
ル入力とし、2次コイルが垂直偏向コイルLVの他端に
接続されたトランスT3によって構成される。Y方向磁
界検出器31の検出出力が増加すれば垂直偏向コイルを
流れる垂直偏向電流は減少し、上記検出出力が減少すれ
ば垂直偏向電流は増加する。, 300 is a Y-direction correction circuit that corrects the deflection current by considering the contribution of the external magnetic field in the Y-direction, that is, the vertical direction; Gain opening circuit 33, Y direction correction output port [334:I
, - and the output of this Y-direction correction output circuit 34 are input to the primary coil, and the secondary coil is constituted by a transformer T3 connected to the other end of the vertical deflection coil LV. If the detection output of the Y-direction magnetic field detector 31 increases, the vertical deflection current flowing through the vertical deflection coil decreases, and if the detection output decreases, the vertical deflection current increases.
以上説明し、たように、本発明によれば、外部磁界を検
出する検出器を設け、その検出出力に応じて仰向電流を
、当該外部[1界の寄与分を差引いた値に補正するよう
にしたことによシ、外部磁界の存在ないしその変ωlに
A・かわらず常に一定の良好な表示品質を得ることがで
きる。また、破界υ−出器およびきわめて簡単な回路栴
成の追加て実現でき、厚いシールド用鉄板を用いる場合
のようfJ:Ifi月の増大および加工の困難性などの
問題も生じない。As described above, according to the present invention, a detector for detecting an external magnetic field is provided, and the supine current is corrected to a value obtained by subtracting the contribution of the external magnetic field according to the detection output of the detector. By doing so, it is possible to always obtain a constant good display quality regardless of the presence of an external magnetic field or its variation ωl. Further, it can be realized by adding a breakout υ-output device and extremely simple circuit construction, and problems such as an increase in fJ:Ifi and difficulty in processing that occur when using a thick iron plate for shielding do not occur.
第1図は本発明の一実施例を示す構成図、第2図(a)
〜(C)は本発明の詳細な説明するための波形図、第3
図は本発明をテレビジョン回路に適用した場合の実際例
を示す#IIi!、図である。
5、LH・拳・・水平偏向コイル、6.LV ・・・・
垂直偏向コイル、7,21−・・−X方向磁界検出器、
8,31・・・・Y方向磁界検出器、14・・會・垂直
出力回路、17゛・Φ・−水平出力回路、23・・11
−X方向ゲイン調整回路、24・・・・X方向補正出力
回路、33・・・・Y方向ゲイン調整回路、34・・・
ψY方向補正出力回路。
特許出願人 山武ハネウェル株式会社
代 理 人 山 川 政 樹(ほか2名)第1図
第2図
第3図
Z[J[JFig. 1 is a configuration diagram showing an embodiment of the present invention, Fig. 2(a)
~(C) is a waveform diagram for detailed explanation of the present invention, the third
The figure shows an actual example of applying the present invention to a television circuit #IIi! , is a diagram. 5. LH/Fist: Horizontal deflection coil, 6. LV...
Vertical deflection coil, 7, 21-...-X direction magnetic field detector,
8, 31...Y-direction magnetic field detector, 14...Vertical output circuit, 17゛・Φ--Horizontal output circuit, 23...11
-X direction gain adjustment circuit, 24...X direction correction output circuit, 33...Y direction gain adjustment circuit, 34...
ψY direction correction output circuit. Patent applicant Yamatake Honeywell Co., Ltd. Agent Masaki Yamakawa (and 2 others) Figure 1 Figure 2 Figure 3 Z[J[J
Claims (1)
を検出する検出器と、各検出器の検出出力に応じて水平
および垂直偏向電流を、検出器により検出される外部磁
界がない場合の電流値に対して」二記外部磁界が偏向量
に与える影響を差引いた値に補正する補正回路とを備え
たことを特徴とする陰極線管装置。A detector that detects the magnetic field around the cathode ray tube in horizontal and vertical directions parallel to the screen, and a horizontal and vertical deflection current according to the detection output of each detector, and a current in the absence of an external magnetic field detected by the detector. 1. A cathode ray tube device comprising: a correction circuit that corrects the value by subtracting the influence of the external magnetic field on the amount of deflection.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1508684A JPS60160775A (en) | 1984-02-01 | 1984-02-01 | Cathode-ray tube device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1508684A JPS60160775A (en) | 1984-02-01 | 1984-02-01 | Cathode-ray tube device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60160775A true JPS60160775A (en) | 1985-08-22 |
Family
ID=11879028
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1508684A Pending JPS60160775A (en) | 1984-02-01 | 1984-02-01 | Cathode-ray tube device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60160775A (en) |
-
1984
- 1984-02-01 JP JP1508684A patent/JPS60160775A/en active Pending
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