JPS6171770A - Horizontal deflection amplitude modulation circuit - Google Patents

Horizontal deflection amplitude modulation circuit

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Publication number
JPS6171770A
JPS6171770A JP19336484A JP19336484A JPS6171770A JP S6171770 A JPS6171770 A JP S6171770A JP 19336484 A JP19336484 A JP 19336484A JP 19336484 A JP19336484 A JP 19336484A JP S6171770 A JPS6171770 A JP S6171770A
Authority
JP
Japan
Prior art keywords
horizontal
horizontal deflection
circuit
voltage
current
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
JP19336484A
Other languages
Japanese (ja)
Inventor
Shigeru Kashiwagi
柏木 茂
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.)
Victor Company of Japan Ltd
Original Assignee
Victor Company of Japan Ltd
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 Victor Company of Japan Ltd filed Critical Victor Company of Japan Ltd
Priority to JP19336484A priority Critical patent/JPS6171770A/en
Publication of JPS6171770A publication Critical patent/JPS6171770A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To attain the accurate modulation of a horizontal deflection amplitude by producing a sawtooth wave current which is flowed to a horizontal deflection coil so that the amplitude of said sawtooth wave current in response to the shape of a reference waveform and therefore compensating a phase delay due to the nonlinearity of a transistor or a circuit element. CONSTITUTION:A harmonic wave detecting circuit 8 delivers a voltage equivalent to the modulated wave parabolic component of the sawtooth wave current which is flowed to a horizontal deflection coil. An operational amplifier 9 serving as a comparator compares a reference voltage obtained from a waveform shaping circuit 7 with a detection voltage obtained from the circuit 8 and applies an output voltage V0 to a horizontal amplitude modulation circuit 5 for horizontal deflection coil current IH. Thus the voltage V0 of the amplifier 9 is set automatically so as to secure the coincidence at all times between a parabolic voltage W1 obtained in proportion to the parabolic modulated wave component of the current IH and the reference parabolic voltage W2 set previously. Thus the circuit 5 modulates the horizontal amplitude.

Description

【発明の詳細な説明】 (産業上の利用分野) この発明は、受像管を使用した直視型や投射型ノテレヒ
ション受像機などの画像ディスプレイ装置における画面
形状の補正を行なう水平偏向−幅変調回路に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a horizontal deflection-width modulation circuit for correcting the screen shape of an image display device such as a direct view type or projection type notelevision receiver using a picture tube. It is something.

(従来の技術) 従来、通常の受像管において、水平、垂百両偏向コイル
に単純なのこぎり波電流を流してラスターを形成しよう
とすると、正しく矩形状にならず、第3図に示すように
、いわゆる糸巻状歪を呈することがある。こn、は受像
管の偏向角が比較的大きい割に、受像面の油率が小さい
ときに起き易く、この歪を特に左右方向について、43
図の破線で示すように直線にしようとするときは、水平
偏向コイルに流すべき電流1.  は框4図に示すよう
になる。すなわち、水平偏向コイルHののこぎり波を垂
直偏向周期Vのパラボラ波で変調してやむ、ばよい。
(Prior Art) Conventionally, when trying to form a raster by passing a simple sawtooth wave current through the horizontal and vertical deflection coils in a normal picture tube, the raster does not form correctly, as shown in Figure 3. , so-called pincushion distortion may occur. Although the deflection angle of the picture tube is relatively large, this phenomenon tends to occur when the oil ratio on the image receiving surface is small.
When trying to make a straight line as shown by the broken line in the figure, the current that should be passed through the horizontal deflection coil is 1. will be as shown in Figure 4. That is, it is sufficient to modulate the sawtooth wave of the horizontal deflection coil H with the parabolic wave of the vertical deflection period V.

また、投射型ディスプレイ装置などでは、受像管の配置
によっては第5図に示すような台形状のラスターが必要
になる場合がある。このようなときには、第6図に示す
ように水平偏向周期Hののこぎり波電流を垂直偏向周期
Vののこぎり波で変調したものを水平偏向コイルに流し
でやnばよい。
Further, in a projection type display device or the like, a trapezoidal raster as shown in FIG. 5 may be required depending on the arrangement of the picture tube. In such a case, as shown in FIG. 6, a sawtooth wave current having a horizontal deflection period H that is modulated by a sawtooth wave having a vertical deflection period V may be applied to the horizontal deflection coil.

いずnの場合も、このように水平偏向のだめののこぎり
波軍流を垂直偏向周間の別な波形で変調し2てやるには
、従来第7図に示すような構成がとらn、ていた。すな
わち、この図で、1は水平偏向出力回路であり、ここか
ら水平偏向コイル3と、さらに水平振幅変調回路5が接
続さr、ていて、水平偏向コイル3に水平偏向周期のの
こぎり波重流が流nている。2は垂直偏向出力回路で、
負荷に垂直偏向コイル4が接チさnていて、ここに垂直
偏向周期ののこきり波亀流を流している。また、6は波
形整形回路であって、垂直偏向出力回路2の出力の一部
を得て1的に応じて整形し上記水平振幅変調回路5に加
えている。
In any case of n, in order to modulate the sawtooth wave flow of horizontal deflection with a different waveform of the vertical deflection period, a conventional configuration as shown in Fig. 7 has been used. Ta. That is, in this figure, 1 is a horizontal deflection output circuit, from which a horizontal deflection coil 3 and further a horizontal amplitude modulation circuit 5 are connected. is flowing. 2 is a vertical deflection output circuit,
A vertical deflection coil 4 is in contact with the load, and a sawtooth wave current with a vertical deflection period is applied thereto. Further, 6 is a waveform shaping circuit which obtains a part of the output of the vertical deflection output circuit 2, shapes it according to the signal, and applies it to the horizontal amplitude modulation circuit 5.

水平振幅変調回路5は、種々の方式が考えらnるが、こ
こでは最もよ〈使わ1ている可飽和リアクタによるイン
ダクタンス変調方式を例にとって説明する。第8図はこ
の変調に可飽和リアクタを使った場合の接続を示し2、
その変調巻線5αに波形整形回路6からの変調出力電流
tを流し、被変調を線5bは水平偏向コイル3に直列に
接続さnる。第9図(−1この可飽和リアクタの構造を
説明するための図で、この可飽和リアクタは通常はE−
IまたはE−E型のコア5Cを使用し、変調巻線5aは
中央脚に、被変調を線5bは左右脚に分割して巻かjる
。このようにすると、変調巻線5αに電流iが流rてい
ない場合は、被変調巻線5bによる磁束はコア5Cに破
線矢印で示したように環流する。ここで、変調巻線5α
に電流iを流すと、こn、による磁束は第9図のコア5
cに実線矢印で示すように流層、必らず左右どちらかの
コア脚で前述の被変調巻・祿5bによる破線の磁束と方
向が一致する。従って、この部分でコア5Cが飽和し、
結局、被変調巻線5bのインダクタンスLが減少する。
Although various methods are conceivable for the horizontal amplitude modulation circuit 5, an inductance modulation method using a saturable reactor, which is the most commonly used method, will be explained here as an example. Figure 8 shows the connection when a saturable reactor is used for this modulation2.
The modulated output current t from the waveform shaping circuit 6 is passed through the modulation winding 5α, and the modulated wire 5b is connected in series to the horizontal deflection coil 3. Figure 9 (-1) This is a diagram for explaining the structure of this saturable reactor. This saturable reactor is normally E-
An I or E-E type core 5C is used, the modulating winding 5a is wound on the center leg, and the modulated wire 5b is divided and wound on the left and right legs. In this way, when the current i is not flowing through the modulating winding 5α, the magnetic flux from the modulated winding 5b circulates through the core 5C as indicated by the broken line arrow. Here, the modulation winding 5α
When a current i is applied to the core 5 of Fig. 9, the magnetic flux due to this n is
As shown by the solid line arrow in c, the direction of the flow layer always coincides with the magnetic flux shown by the broken line due to the modulated winding 5b in either the left or right core leg. Therefore, core 5C is saturated in this part,
As a result, the inductance L of the modulated winding 5b decreases.

この現象を図示すると、第10図に示すような変調出力
電流iとインダクタンスLの関係になる。被変調!i5
bのインダクタンスLが減少すると、水平偏向コイル3
の水平のこぎり波電流が増加するので、結局、上記電流
iの値を第10図のパラボラ波形Pに示すように垂直偏
向周期Vのパラボラ状に変化てせてやわ、ば、水平偏向
コイル3に流nる電流は第4図に示すようになり、第3
図のラスクーの左右端が直線に補正される。
To illustrate this phenomenon, the relationship between the modulated output current i and the inductance L is as shown in FIG. Modulated! i5
When the inductance L of b decreases, the horizontal deflection coil 3
As the horizontal sawtooth current increases, the value of the current i is changed in a parabolic manner with a vertical deflection period V as shown in the parabolic waveform P in FIG. 10. The current that flows is as shown in Figure 4, and the third
The left and right ends of the rasku in the figure are corrected to straight lines.

(発明力;解、導11’らシナスはH「層内)以上詳述
した従来例で最も問題となるのは、第10図に示すi−
Lの関係が直線でなく、電流iの小さい部分、大きい部
分の両方で勾配が小さくなっていることである。従って
、第10図のパラボラ波形Pを正しい波形としても、第
4図に示すようなのこぎり波形の包絡線が必ずしもパラ
ボラ波形になるとは限らず、従って、第3図の補正結果
の左右端が直線にならず、うねってしまうことが多かっ
た。こnを防ぐには、コア5cに充分大型のものを使い
、パラボラ波形Pの振幅に比べてi −Lカーブの中央
の直線部分が充分にらるようにすn、ばよい。しかし、
このようにすnば、重量的、価格的に不利1cなること
は当然である。
(Inventive power; Solution, Derivation 11' et al. sinus is in the H layer) The most problematic problem in the conventional example detailed above is the i-
The relationship between L is not a straight line, and the slope is small both in the small portion and the large portion of the current i. Therefore, even if the parabolic waveform P in Figure 10 is a correct waveform, the envelope of the sawtooth waveform shown in Figure 4 does not necessarily become a parabolic waveform, and therefore the left and right ends of the correction result in Figure 3 are straight lines. In many cases, it would not move and would undulate. In order to prevent this, it is sufficient to use a sufficiently large core 5c so that the central straight portion of the i-L curve is sufficiently large compared to the amplitude of the parabolic waveform P. but,
Naturally, if this is done, there will be disadvantages in terms of weight and cost.

また、この種の可飽和リアクタはコアの飽和特性を利用
する関係上、第10図のi−Lカーブのばらつきが多く
、まだ、混1度によっても変化し易く、従って、この点
からも第3図のラスターの左右端の縦線補正を正確に行
なうことができないという問題を抱えていた。
In addition, since this type of saturable reactor utilizes the saturation characteristics of the core, the i-L curve shown in Figure 10 has many variations, and it still changes easily depending on the degree of mixing. There was a problem in that it was not possible to accurately correct the vertical lines at the left and right ends of the raster shown in Figure 3.

C問題を解決するだめの手段) この発明は、上述の問題点を解決するため、受像管と、
その電子ビームを水平方向に電磁偏向する偏向コイルを
有し、この偏向コイルに流す水平偏向同期ののこぎり波
電流の垂直偏向周期数の変調波成分(W1)を検出する
検出回路と、同様に垂直偏向周期を有する基準波形(W
2)を生成する手段と、さらに上記2つの各波形(W、
 ) 、 (w2)を比較する比較回路を有し、この比
較回路の出力によって上記水平偏向コイルに流すのこぎ
り波電流を変調する水平振幅変調回路を備えることによ
り、上3e水平偏向コイルに流すのこぎり波電流を前記
基準波形(W2)の形状に1忘じて、その振幅が変化す
るように構成した水平偏向旦幅変調回路を提供するもの
であろう (実施例) 第1図はこの発明の実施例を示した゛もので、第1図中
の符号1〜5を付した部分は、第7図の同一符号と同様
部分を示し、はぼ同一の働きをするものとする。
Solution to Problem C) In order to solve the above-mentioned problems, the present invention provides a picture tube;
It has a deflection coil that electromagnetically deflects the electron beam in the horizontal direction, and a detection circuit that detects the modulated wave component (W1) of the vertical deflection period number of the sawtooth current synchronized with the horizontal deflection flowing through the deflection coil. A reference waveform (W
2), and means for generating each of the above two waveforms (W,
) , (w2), and a horizontal amplitude modulation circuit that modulates the sawtooth wave current flowing through the horizontal deflection coil (upper 3e) by the output of this comparison circuit. This will provide a horizontal deflection width modulation circuit configured so that the current has the shape of the reference waveform (W2) and its amplitude changes (Embodiment) FIG. 1 shows an embodiment of the present invention. This is an example, and the parts numbered 1 to 5 in FIG. 1 are the same parts as the same reference numerals in FIG. 7, and have essentially the same functions.

7は波形整形回路で、垂直偏向出力回路2の出力の一部
を得て目的とする波形、例えば菓3図および第4図に示
すようなラスターの左右糸巻歪補正に使用する場合は、
垂直偏向同期のパラボラ波電圧を得るようにする。また
、8は変調波検出回路であって、第4図に示したような
水平偏向コイルに流すのこぎり波電流の変調波パラボラ
成分に相当する電圧を出力する。、9は比較回路となる
演算増幅器であって、波形整形回路7から得らn、た電
圧を基準とし、こn、と変調波検出回路8から得らnた
検出電圧を比較して、その出力電圧V。を水平偏向コイ
ル電流I++  の水平振幅変調回路5に加えている。
7 is a waveform shaping circuit, which obtains a part of the output of the vertical deflection output circuit 2 and uses it for correcting the desired waveform, for example, raster left and right pincushion distortion as shown in Figures 3 and 4.
A parabolic wave voltage with vertical deflection synchronization is obtained. Further, 8 is a modulated wave detection circuit which outputs a voltage corresponding to the modulated wave parabolic component of the sawtooth wave current flowing through the horizontal deflection coil as shown in FIG. , 9 is an operational amplifier serving as a comparison circuit, which uses the voltage obtained from the waveform shaping circuit 7 as a reference, compares this voltage with the detected voltage obtained from the modulated wave detection circuit 8, and calculates the result. Output voltage V. is applied to the horizontal amplitude modulation circuit 5 of the horizontal deflection coil current I++.

このようにすると、水平偏向コイル電流IHのパラボラ
変調渡分に比例して得らj、るパラボラ電圧W、が予め
設定さj、た基準パラボラ波電圧W2に常に一致するよ
うに自動的に演算増幅器9の出力電圧V。が定めらn2
、こn、によって水平振幅変調回路5が水平振幅変調1
乍用を行なう。従って、水平振幅変調回路5に前述した
従来例のような多少の非直線性あるいはばらつきがあっ
たとしても、この発明□の場合は全く無関係に水平偏向
コイル電流IHの変調波の形を定めらn、る。
In this way, the parabolic voltage W obtained in proportion to the parabolic modulation portion of the horizontal deflection coil current IH is automatically calculated so as to always match the preset reference parabolic voltage W2. Output voltage V of amplifier 9. is determined n2
, this causes the horizontal amplitude modulation circuit 5 to perform horizontal amplitude modulation 1.
Go about your business. Therefore, even if there is some nonlinearity or variation in the horizontal amplitude modulation circuit 5 as in the conventional example described above, in the case of the present invention □, the shape of the modulation wave of the horizontal deflection coil current IH is determined completely regardless. n.ru.

第2図に示すものは、上記変調波検出回路8の具体例1
であり、ここで、10は電流電圧変換用抵抗、11は直
流分阻止コンデンサ、12゜13は整流ダイオード、1
4は平滑コンデンサ、15は負荷抵抗、16は交流会の
結合コンデンサである。
What is shown in FIG. 2 is a specific example 1 of the modulated wave detection circuit 8.
Here, 10 is a current-voltage conversion resistor, 11 is a DC blocking capacitor, 12° and 13 are rectifier diodes, and 1
4 is a smoothing capacitor, 15 is a load resistor, and 16 is a coupling capacitor for exchange.

このようにすると、水平偏向コイル電流IIに比例した
電流電圧変換用抵抗10の両岸電圧vRが直流分阻止コ
ンデンサ11、整流ダイオード12,13、平滑コンデ
ンサ14および負?fiT抵抗15 Kよって両波整流
さn、た形になるので、負荷抵抗15の両端はパラボラ
のリップルを伴りた上記両端電圧VRのピーク、ピーク
値力!’) ラn1、このうち上記結合コンデンサ16
によって、そのパラボラ波のリップル分のパラボラ電圧
W、のみが演算増幅器90入力端子の1つに加えらn5
、こn、が前述したように常に基準パラボラ波電圧W2
と一致するように回路全体が働く。
In this way, the voltage vR across both sides of the current-voltage conversion resistor 10, which is proportional to the horizontal deflection coil current II, is adjusted to the DC blocking capacitor 11, the rectifier diodes 12, 13, the smoothing capacitor 14, and the negative voltage VR. Since the fiT resistor 15 K is rectified in both waves and has the shape n, both ends of the load resistor 15 are at the peak and peak value of the voltage VR at both ends with parabolic ripple! ') Run n1, of which the above coupling capacitor 16
Therefore, only the parabolic voltage W corresponding to the ripple of the parabolic wave is applied to one of the input terminals of the operational amplifier 90.
, this is always the reference parabolic wave voltage W2 as mentioned above.
The entire circuit works to match.

また、この基準パラボラ波′邂圧w2の波形を得るには
、垂直偏向出力回路2から得だ波形を波形整形回路7で
、例えば積分等を行なって導波電圧W2の波形はパラボ
ラ波になるのでこのような場合は特に複′Hな波形整形
回路を設ける必要はない。すなわち、通常偏向コイルに
は直流阻止用コンデンサが接続さjているので、このコ
ンデンサには垂直周期のパラボラ波が多少発生するから
、こn、を結合コンデンサによって演算増幅器に導贋て
やn、ばよ(、極めて簡単な構成でこの発明が実現でき
ることになる。
In addition, in order to obtain the waveform of this reference parabolic wave 'wave pressure w2, the waveform obtained from the vertical deflection output circuit 2 is subjected to, for example, integration in the waveform shaping circuit 7, and the waveform of the waveguide voltage W2 becomes a parabolic wave. Therefore, in such a case, it is not necessary to provide a multi-H waveform shaping circuit. That is, since a direct current blocking capacitor is usually connected to the deflection coil, some vertical period parabolic waves are generated in this capacitor, so this wave is introduced to the operational amplifier by a coupling capacitor. By the way, this invention can be realized with an extremely simple configuration.

また、こnまで第7図に示す水平振幅変調回路5の一例
として、可飽和リアクタ方式をあげて説明しだが、こn
、は他の方式、例、tはトランジスタなどの能動素子を
使い、その電圧変化を利用するようにしてもよく、この
ような場合でもこの発明によ1ば、トランジスタの非直
線性や回路素子による位相遅n、などを補償し7て正確
な変調を行なうことができる。
In addition, although the saturable reactor method has been described as an example of the horizontal amplitude modulation circuit 5 shown in FIG.
, for example, t may use an active element such as a transistor and utilize its voltage change. Even in such a case, according to the present invention, the non-linearity of the transistor and the circuit element can be It is possible to perform accurate modulation by compensating for the phase delay n, etc.

(発明の効果) この発明は、以上のような水平偏向振幅変調回路を提供
することによって、受像管の電子ビームの水平偏向にお
いて、その水平振幅を垂亘偏向制期で正確にかつ任意の
波形で変調することができるので、受像画面の左右糸巻
歪補正や台形補正に適用して極めて大きな効果がある。
(Effects of the Invention) By providing the horizontal deflection amplitude modulation circuit as described above, the present invention can accurately and arbitrarily control the horizontal amplitude of the horizontal deflection of the electron beam of the picture tube with vertical deflection control. Since it is possible to modulate the image, it is extremely effective when applied to left and right pincushion distortion correction and trapezoidal correction of the image receiving screen.

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

第1図はこの発明になる水平偏向振幅変調旦路の実施例
を示すブロック図、第2図はその一部の具体的回路図、
第3図〜第6図はこの発明の目的および効果を説明する
だめの説明図、第7図〜第9図は従来例を示す説明図、
第10図はその特性を示゛す曲線図である。 1・・・水平偏向出力回路、2・・・垂直偏向出力回路
、3・・・水平偏向コイル、4・・・垂直偏向コイル。 5・・・水平振幅変調回路、7・・・波形整形回路、8
・・・変調波検出回路、9・・・演算増幅器、10・・
・電、流電正変換用抵抗、11・・・直流分阻止コンデ
ンサ、12.13・・・整流ダイオード、14・・・平
滑コンデンサ、15・・・負荷抵抗、16・・・結合コ
ンデンサ。 特許出願人   日本ビクター株式会社代  理  人
    尾   股   行   雄同       
 荒   木   友 之 助第1図 第2図 第3図      第4図 門 第5図     第6図 第7図 第9図 C 第8図 第10図
FIG. 1 is a block diagram showing an embodiment of the horizontal deflection amplitude modulation circuit according to the present invention, and FIG. 2 is a specific circuit diagram of a part thereof.
FIGS. 3 to 6 are explanatory diagrams for explaining the purpose and effects of the present invention, and FIGS. 7 to 9 are explanatory diagrams showing conventional examples.
FIG. 10 is a curve diagram showing the characteristics. 1...Horizontal deflection output circuit, 2...Vertical deflection output circuit, 3...Horizontal deflection coil, 4...Vertical deflection coil. 5... Horizontal amplitude modulation circuit, 7... Waveform shaping circuit, 8
...Modulated wave detection circuit, 9...Operation amplifier, 10...
・Resistance for current and current positive conversion, 11... DC blocking capacitor, 12.13... Rectifier diode, 14... Smoothing capacitor, 15... Load resistor, 16... Coupling capacitor. Patent applicant: Yudo Omata, representative of Victor Japan Co., Ltd.
Tomonosuke Araki Figure 1 Figure 2 Figure 3 Figure 4 Gate Figure 5 Figure 6 Figure 7 Figure 9 C Figure 8 Figure 10

Claims (2)

【特許請求の範囲】[Claims] (1)受像管と、その電子ビームを水平方向に電磁偏向
する偏向コイルを有し、この偏向コイルに流す水平偏向
周期ののこぎり波電流の垂直偏向周波数の変調波成分(
W_1)を検出する検出回路と、同様に垂直偏向周期を
有する基準波形(W_2)を生成する手段と、さらに上
記2つの各波形(W_1)、(W_2)を比較する比較
回路を有し、この比較回路の出力によつて上記水平偏向
コイルに流すのこぎり波電流を変調する水平振幅変調回
路を備えることにより、上記水平偏向コイルに流すのこ
ぎり波電流を前記基準波形(W_2)の形状に応じて、
その振幅が変化するように構成したことを特徴とする水
平偏向振幅変調回路。
(1) It has a picture tube and a deflection coil that electromagnetically deflects the electron beam in the horizontal direction, and the modulated wave component (
W_1), a means for generating a reference waveform (W_2) having a vertical deflection period, and a comparison circuit for comparing the two waveforms (W_1) and (W_2). By providing a horizontal amplitude modulation circuit that modulates the sawtooth wave current flowing through the horizontal deflection coil according to the output of the comparison circuit, the sawtooth wave current flowing through the horizontal deflection coil can be adjusted according to the shape of the reference waveform (W_2).
A horizontal deflection amplitude modulation circuit characterized in that the amplitude is configured to vary.
(2)垂直偏向周期を有する基準波形(W_2)を生成
する手段として、垂直偏向コイルに直列に接続される直
流阻止コンデンサ上に発生するパラボラ電圧波形を基準
波形(W_2)として得るようにし、このパラボラ電圧
波形を基準波形とすることによつて、受像管上の画面の
左右糸巻歪を補正するように構成したことを特徴とする
特許請求の範囲第1項に記載の水平偏向振幅変調回路。
(2) As a means for generating a reference waveform (W_2) having a vertical deflection period, a parabolic voltage waveform generated on a DC blocking capacitor connected in series with the vertical deflection coil is obtained as the reference waveform (W_2). 2. The horizontal deflection amplitude modulation circuit according to claim 1, wherein the horizontal deflection amplitude modulation circuit is configured to correct left and right pincushion distortion of a screen on a picture tube by using a parabolic voltage waveform as a reference waveform.
JP19336484A 1984-09-14 1984-09-14 Horizontal deflection amplitude modulation circuit Pending JPS6171770A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19336484A JPS6171770A (en) 1984-09-14 1984-09-14 Horizontal deflection amplitude modulation circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19336484A JPS6171770A (en) 1984-09-14 1984-09-14 Horizontal deflection amplitude modulation circuit

Publications (1)

Publication Number Publication Date
JPS6171770A true JPS6171770A (en) 1986-04-12

Family

ID=16306680

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19336484A Pending JPS6171770A (en) 1984-09-14 1984-09-14 Horizontal deflection amplitude modulation circuit

Country Status (1)

Country Link
JP (1) JPS6171770A (en)

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