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JPH0586114B2 - - Google Patents

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Publication number
JPH0586114B2
JPH0586114B2 JP1429388A JP1429388A JPH0586114B2 JP H0586114 B2 JPH0586114 B2 JP H0586114B2 JP 1429388 A JP1429388 A JP 1429388A JP 1429388 A JP1429388 A JP 1429388A JP H0586114 B2 JPH0586114 B2 JP H0586114B2
Authority
JP
Japan
Prior art keywords
waveform
voltage
circuit
deflection
horizontal deflection
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 - Fee Related
Application number
JP1429388A
Other languages
Japanese (ja)
Other versions
JPH01190082A (en
Inventor
Shigeru Kashiwagi
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 JP1429388A priority Critical patent/JPH01190082A/en
Publication of JPH01190082A publication Critical patent/JPH01190082A/en
Publication of JPH0586114B2 publication Critical patent/JPH0586114B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は受像管を利用したテレビジヨン受像機
等の画像の形状歪を補正する画像歪補正回路であ
つて、特にラスター左右端部が直線にならない所
謂サイドピンクツシヨン歪(以下、SPC歪と略
す)を補正する画像歪補正回路に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention is an image distortion correction circuit for correcting shape distortion of an image of a television receiver or the like using a picture tube. The present invention relates to an image distortion correction circuit that corrects so-called side pink distortion (hereinafter abbreviated as SPC distortion) that does not occur.

(従来の技術) 従来、通常の受像管において、水平、垂直両偏
向コイルに単純なノコギリ波電流を流してラスタ
ーを形成しようとする正しく方形のラスターにな
らず、第3図の実線に示す様に所謂糸巻状歪を呈
する事がある。これは受像管偏向角が比較的大き
い割に、受像面の曲率が小さい時に顕著である。
この歪を特に左右端部について第3図の破線の様
に直線にしようとする時、水平偏向電流の波形は
どの様であるべきかを検討してみる。
(Prior Art) Conventionally, in an ordinary picture tube, when an attempt was made to form a raster by passing a simple sawtooth wave current through both the horizontal and vertical deflection coils, the raster was not formed into a correct rectangular raster, as shown by the solid line in Figure 3. may exhibit so-called pincushion distortion. This is noticeable when the curvature of the image receiving surface is small although the deflection angle of the picture tube is relatively large.
Let's consider what the waveform of the horizontal deflection current should be when trying to make this distortion straight, especially at the left and right ends, as shown by the broken line in FIG.

この補正前の左右端部の曲線の形状は、既に
1957年FinkのTelevision Engineering Hadbook
に明らかにされており、受像管の偏向中心から受
像面までの距離をl、受像面中心から左右方向の
端部までの距離をaとし、受像面が平面であると
仮定すると次式の様に表される(受像管面左右方
向をX軸、上下方向をy軸とする) x2/a2−y2/l2=1 (1) これは双曲線であるから、この波形に合わせて
水平偏向電流を変調してやれば目的の補正が達成
出来ることになる。実際には電磁偏向の場合、偏
向電流と偏向角は正確には比例しないので、厳密
に言うと若干の誤差は生じるが、水平偏向ノコギ
リ波電流のp−p(ピーク・ピーク)値を垂直偏
向周期の双曲線で変調してやれば、第3図の破線
の様にSPC歪はほゞ直線に修正される。
The shape of the curve at the left and right ends before this correction is already
1957 Fink's Television Engineering Hadbook
Assuming that the distance from the deflection center of the picture tube to the image receiving surface is l, the distance from the center of the image receiving surface to the end in the left and right direction is a, and the image receiving surface is a flat surface, the following equation is obtained. (The horizontal direction of the picture tube surface is the X-axis, and the vertical direction is the y - axis.) The desired correction can be achieved by modulating the horizontal deflection current. Actually, in the case of electromagnetic deflection, the deflection current and the deflection angle are not exactly proportional, so strictly speaking, there will be some errors, but the peak-to-peak (p-p) value of the horizontal deflection sawtooth current is used for the vertical deflection. If the modulation is performed using a hyperbolic period, the SPC distortion will be corrected to a nearly straight line as shown by the broken line in Figure 3.

この様な回路構成の例を第4図に示す。ここ
で、1は水平偏向出力回路、2は水平偏向コイ
ル、3は垂直偏向出力回路、4は垂直偏向コイ
ル、5は双曲線波形発生回路、6は水平振幅変調
回路であつて、水平偏向コイル2、垂直偏向コイ
ル4は図示されない受像管の頚部に取付けられ、
受像管の電子ビームを夫々水平及び垂直方向に偏
向するものとする。
An example of such a circuit configuration is shown in FIG. Here, 1 is a horizontal deflection output circuit, 2 is a horizontal deflection coil, 3 is a vertical deflection output circuit, 4 is a vertical deflection coil, 5 is a hyperbolic waveform generation circuit, 6 is a horizontal amplitude modulation circuit, and the horizontal deflection coil 2 , a vertical deflection coil 4 is attached to the neck of the picture tube (not shown),
It is assumed that the electron beam of the picture tube is deflected in the horizontal and vertical directions, respectively.

この様にすると、水平偏向出力回路1は水平偏
向周期のノコギリ波電流(水平偏向ノコギリ波電
流)Iyhを水平偏向コイル2に流し、また、垂直
偏向出力回路3は垂直偏向周期のノコギリ波電流
(垂直偏向ノコギリ波電流)Iyvを垂直偏向コイル
4に流して、受像管面上にほゞ方形のラスターを
形成する。また更に、これと同時に垂直偏向出力
回路3から双曲線発生回路5を通して垂直偏向周
期の双曲線波形電圧Vhpが得られ、これが水平振
幅変調回路6に加えられる。更に、こ水平振幅変
調回路6は水平偏向出力回路1に作用して水平偏
向ノコギリ波電流Iyhのp−p値を双曲線波形電
圧Vhpの値に応じて変調する様になつている。
In this way, the horizontal deflection output circuit 1 causes the sawtooth wave current (horizontal deflection sawtooth wave current) Iyh with the horizontal deflection period to flow through the horizontal deflection coil 2, and the vertical deflection output circuit 3 causes the sawtooth wave current (horizontal deflection sawtooth wave current) with the vertical deflection period to flow through the horizontal deflection coil 2. A vertical deflection sawtooth wave current (Iyv) is passed through the vertical deflection coil 4 to form a substantially rectangular raster on the picture tube surface. Furthermore, at the same time, a hyperbolic waveform voltage Vhp of the vertical deflection period is obtained from the vertical deflection output circuit 3 through the hyperbolic generating circuit 5, and is applied to the horizontal amplitude modulation circuit 6. Further, the horizontal amplitude modulation circuit 6 acts on the horizontal deflection output circuit 1 to modulate the pp value of the horizontal deflection sawtooth wave current Iyh in accordance with the value of the hyperbolic waveform voltage Vhp.

第5図は従来例の更に具体的な回路例を説明し
たものである。
FIG. 5 illustrates a more specific circuit example of the conventional example.

ここで、やはり番号1〜6の部分は先の第4図
の同一番号部分と同様な働きをするものとする。
そして、水平振幅変調回路6は直流電源電圧Eb
から所定のリツプルを持つた直流電源電圧Eb′を
得て、これを水平偏向出力回路1の動作電源電圧
とすることによつて、水平偏向ノコギリ波電流
Iyhのp−p値を目的に合わせて変調する様にし
た形式のものである。
Here, it is assumed that the parts numbered 1 to 6 function similarly to the parts with the same numbers in FIG. 4 above.
Then, the horizontal amplitude modulation circuit 6 receives the DC power supply voltage Eb
By obtaining a DC power supply voltage Eb' with a predetermined ripple from
This is a type of modulation in which the pp value of Iyh is modulated according to the purpose.

ここで、7は電圧制御NPN型トランジスタ、
8はそのベースバイアス抵抗、9は専ら水平偏向
周波数成分のリツプル電流を流す為の平滑コンデ
ンサ、10は結合コンデンサであつて、その一端
に変調電圧(ここでは双曲線波形電圧Vhp′)を
加えると、この電圧(波形)に応じて直流電源電
圧Eb′が変調される。
Here, 7 is a voltage controlled NPN type transistor,
8 is its base bias resistor, 9 is a smoothing capacitor for flowing the ripple current of the horizontal deflection frequency component exclusively, and 10 is a coupling capacitor, and when a modulation voltage (here, hyperbolic waveform voltage Vhp') is applied to one end of the capacitor, The DC power supply voltage Eb' is modulated according to this voltage (waveform).

また、ここには同時に制御回路11が付加され
る事があり、ここに流す制御電流isを回路に付属
する可変抵抗12で可変する事によつて、電圧制
御トランジスタ7のベース電圧、ひいては直流電
源電圧Eb′の電圧値も調節する事が出来る。
In addition, a control circuit 11 may be added at the same time, and by varying the control current is flowing here with a variable resistor 12 attached to the circuit, the base voltage of the voltage control transistor 7, and by extension the DC power supply. The voltage value of voltage Eb' can also be adjusted.

また、制御回路11は直流電源電圧Eb′の平均
電圧値に応じてその動作状態を変え、例えば、も
し電圧Eb′が上昇すると、制御電流isを増やして
電圧Eb′を下げる様な働き、即ちネガテイプ・フ
イールドバツク特性を持たせる事があり、この結
果、電圧Eb′の平均電圧値、そして、水平偏向コ
イル2を流れる水平偏向ノコギリ波電流Iyhの値
が安定化される。
Further, the control circuit 11 changes its operating state according to the average voltage value of the DC power supply voltage Eb'. For example, if the voltage Eb' increases, the control circuit 11 works to increase the control current is and lower the voltage Eb'. A negative tape feedback characteristic may be provided, and as a result, the average voltage value of the voltage Eb' and the value of the horizontal deflection sawtooth wave current Iyh flowing through the horizontal deflection coil 2 are stabilized.

ところで、水平偏向ノコギリ波電流Iyhの包絡
線の形状を双曲線にする為には、電圧Eb′の変調
電圧(波形)をそのまま双曲線にすれば良いと言
う訳ではない。
By the way, in order to make the shape of the envelope of the horizontal deflection sawtooth wave current Iyh a hyperbola, it is not necessary to just make the modulation voltage (waveform) of the voltage Eb' into a hyperbola.

即ち、ここでは双曲線波形電圧Vhpとは別に補
正波形発生回路13で生成した補正電圧波形
Vauxを双曲線波形電圧Vhpに加算回路14で合
成し、合成波形(双曲線波形電圧)Vhp′として
から、結合コンデンサ10を通して電圧制御トラ
ンジスタ7のベースに加えてやる様にしないと、
水平偏向ノコギリ波電流Iyhの包絡線が正しい双
曲線波形とはならない。
That is, here, in addition to the hyperbolic waveform voltage Vhp, the correction voltage waveform generated by the correction waveform generation circuit 13 is used.
Vaux must be combined with the hyperbolic waveform voltage Vhp in the adder circuit 14 to form a composite waveform (hyperbolic waveform voltage) Vhp', and then added to the base of the voltage control transistor 7 through the coupling capacitor 10.
The envelope of the horizontal deflection sawtooth current Iyh does not have a correct hyperbolic waveform.

これは、第6図に示す様に、水平偏向コイル2
がインダクタンス分Lと、直流抵抗分Rとからな
る事に起因する。即ち、第6図のインダクタンス
分Lと直流抵抗分Rとの直列回路に垂直偏向周期
のリツプル電流iを流そうとすると、直流抵抗分
Rの両端には電流iの波形と同様な波形VRが生
じるが、インダクタンス分Lの方には、これを時
間tに関して微分した形の波形VLが生じる。
This is the horizontal deflection coil 2 as shown in FIG.
This is because it consists of an inductance component L and a DC resistance component R. That is, when a ripple current i with a vertical deflection period is caused to flow through the series circuit of the inductance L and the DC resistance R shown in FIG. 6, a waveform V R similar to the waveform of the current i appears at both ends of the DC resistance R. However, in the inductance L, a waveform V L is generated by differentiating this with respect to time t.

従つて、この水平偏向コイル2の様なインダク
タンス分Lと直流抵抗分Rの直列回路にiの様な
電流を流そうとすると、ここにはVL+VRの電圧
を加えなければならい事になる。
Therefore, if you want to flow a current like i through a series circuit of inductance L and DC resistance R like this horizontal deflection coil 2, you will have to apply a voltage of V L + V R here. Become.

第5図補正波形発生回路13、加算回路14は
この為のものであつて、補正波形発生回路13で
波形VLに相当する垂直偏向周期の補助電圧(波
形)Vauxを作り、これを加算回路14で本来の
双曲線波形電圧Vhpと合成して装置の変調電圧
(双曲線波形電圧)Vhp′を得、これを結合コンデ
ンサ10を通して電圧制御トランジスタ7に加
え、直流電源電圧Eb′を変調してやれば、水平偏
向ノコギリ波電流Iyhの包絡線は正しく双曲線波
形電圧Vhpとする事が出来る。
The correction waveform generation circuit 13 and the addition circuit 14 shown in FIG. 14, combine it with the original hyperbolic waveform voltage Vhp to obtain the modulation voltage (hyperbolic waveform voltage) Vhp' of the device, and add this to the voltage control transistor 7 through the coupling capacitor 10 to modulate the DC power supply voltage Eb'. The envelope of the deflection sawtooth wave current Iyh can be correctly determined as the hyperbolic waveform voltage Vhp.

(発明が解決しようとする課題) ところで、先の第5図の双曲線波形電圧Vhpや
補助電圧(波形)Vauxを受動素子だけで作るの
は困難であり、デイジタル的に作るか、あるいは
ダイオード等の非直線素子を用いて折れ線近似で
作るしかない。いずれにしても、この様にして、
これ等二つの波形を作るのは回路が甚だしく複雑
になる問題点がある。
(Problem to be solved by the invention) By the way, it is difficult to create the hyperbolic waveform voltage Vhp and the auxiliary voltage (waveform) Vaux shown in FIG. The only way to create it is by using a polygonal line approximation using non-linear elements. In any case, in this way,
Creating these two waveforms has the problem that the circuit becomes extremely complicated.

また、偏向振幅をオーバースキヤン/アンダー
スキヤンの様に切える必要が有る時は、当然、双
曲線波形発生回路5及び補正波形発生回路13の
両回路の定数を同時に切換えて、双曲線波形電圧
Vhp、補助電圧(波形)Vauxの振幅を水平偏向
ノコギリ波電流Iyhに比例して変化させてやらね
ばならず、回路構成としては非常に繁雑なものに
なつてしまう問題点があつた。
Also, when it is necessary to change the deflection amplitude like overscan/underscan, it is natural to change the constants of both the hyperbolic waveform generation circuit 5 and the correction waveform generation circuit 13 at the same time to generate a hyperbolic waveform voltage.
The amplitude of Vhp and the auxiliary voltage (waveform) Vaux had to be changed in proportion to the horizontal deflection sawtooth wave current Iyh, which resulted in a problem that the circuit configuration became extremely complicated.

(課題を解決するための手段) 本発明は以上の様な問題点を解決すべく為され
たものであつて、受像管を水平偏向するための水
平偏向回路と、同じく垂直偏向するための垂直偏
向回路と、前記水平偏向回路の電源電圧を変調す
る電源電圧変調回路とがあつて、前記垂直偏向回
路より得た垂直偏向周期の偏向補正波形を、前記
電源電圧変調回路に加えてラスター左右端の形状
を補正する画像歪補正回路において、前記偏向補
正波形は、垂直偏向周期のノコギリ波状の電圧波
形を波形整形回路を通し、該電圧波形のピーク値
及び、もしくはボトム値の付近の形状を整形して
得た第1の信号と、前記第1の信号を積分回路を
通して得た第2の信号とを加算する事によつて得
る様にした事によつて、簡単な構成で、水平偏向
ノコギリ波電流の包絡線が、正しく前記積分回路
の出力波形に一致する様にしたものであつて、よ
り正確で簡単にラスター左右端の形状の補正が出
来る様にし、特にサイドピンクツシヨン歪補正に
効果がある画像歪補正回路を提供するものであ
る。
(Means for Solving the Problems) The present invention has been made to solve the above-mentioned problems, and includes a horizontal deflection circuit for horizontally deflecting a picture tube and a vertical deflection circuit for vertically deflecting a picture tube. There is a deflection circuit and a power supply voltage modulation circuit that modulates the power supply voltage of the horizontal deflection circuit, and the deflection correction waveform of the vertical deflection period obtained from the vertical deflection circuit is added to the power supply voltage modulation circuit to the right and left ends of the raster. In the image distortion correction circuit that corrects the shape of the deflection correction waveform, a sawtooth voltage waveform with a vertical deflection period is passed through a waveform shaping circuit to shape the shape of the voltage waveform near its peak value and/or bottom value. By adding the first signal obtained through the above-mentioned first signal and the second signal obtained by passing the first signal through an integrating circuit, the horizontal deflection saw can be obtained with a simple configuration. The envelope of the wave current is made to correctly match the output waveform of the integrating circuit, and it is possible to more accurately and easily correct the shape of the left and right edges of the raster, especially for side pink tension distortion correction. The present invention provides an effective image distortion correction circuit.

(実施例) 第1図は本発明による画像歪補正回路の一実施
例を例したものである。ここで、番号1〜4,
6,14は先の第5図の同一番号部分と同様な働
きをするものとする。ここで新たに付加された1
5は波形整形回路、16は積分回路である。
(Embodiment) FIG. 1 illustrates an embodiment of an image distortion correction circuit according to the present invention. Here, numbers 1 to 4,
6 and 14 function in the same manner as the portions with the same numbers in FIG. 5 above. Newly added 1 here
5 is a waveform shaping circuit, and 16 is an integrating circuit.

この様にすると、先ず垂直偏向出力回路3から
は容易に垂直偏向周期ノコギリ電圧Vstが得られ
るので、これを波形整形回路15に加える。この
波形整形回路15では垂直偏向周期ノコギリ波電
圧Vstを圧縮して、走査周期の始点付近ではその
傾斜がほゞ水平で、走査中央に向かうにつれて傾
斜が急になり、走査終点になると傾斜がほゞ水平
になる様な垂直偏向周期ノコギリ波電圧Vst′が得
られる。
In this way, first, the vertical deflection period sawtooth voltage Vst can be easily obtained from the vertical deflection output circuit 3, and this is applied to the waveform shaping circuit 15. This waveform shaping circuit 15 compresses the vertical deflection period sawtooth wave voltage Vst, so that its slope is almost horizontal near the start point of the scan period, becomes steeper toward the center of the scan, and becomes less sloped toward the end point of the scan.ゞA vertical deflection periodic sawtooth wave voltage Vst′ that becomes horizontal can be obtained.

そして、次の積分回路16に、この垂直偏向周
期ノコギリ波電圧Vst′を加えると、その出力には
双曲線に良く近似した双曲線波形電圧Vhpが得ら
れる。
Then, when this vertical deflection periodic sawtooth wave voltage Vst' is applied to the next integrating circuit 16, a hyperbolic waveform voltage Vhp that closely approximates a hyperbola is obtained as its output.

一方、この双曲線波形電圧Vhpと、先の垂直偏
向周期ノコギリ波電圧Vst′とが加算回路14で合
成されて双曲線波形電圧Vhp′を得、この双曲線
波形電圧Vhp′に従つて直流電源電圧Ebが変調さ
れて直流電源電圧Eb′となり、これが水平偏向出
力回路1の動作電源電圧となるので、水平偏向ノ
コギリ波電流Iyhのp−p値が目的に応じて変調
される。
On the other hand, this hyperbolic waveform voltage Vhp and the previous vertical deflection periodic sawtooth wave voltage Vst' are combined in an adder circuit 14 to obtain a hyperbolic waveform voltage Vhp', and according to this hyperbolic waveform voltage Vhp', the DC power supply voltage Eb is The modulated DC power supply voltage Eb' becomes the operating power supply voltage of the horizontal deflection output circuit 1, so that the pp value of the horizontal deflection sawtooth wave current Iyh is modulated according to the purpose.

先に、第2図で説明した様に、水平偏向ノコギ
リ波電流Iyhの包絡線に所定の波形を得ようとす
ると、回路の直流電源電圧Eb′の波形、即ち、双
曲線波形電圧Vhp′は、水平偏向ノコギリ波電流
Iyhの包絡線の波形そのままの波形とその微分波
形とを適当な割合で合成してやれば良い事にな
る。
As previously explained in Fig. 2, when trying to obtain a predetermined waveform in the envelope of the horizontal deflection sawtooth current Iyh, the waveform of the DC power supply voltage Eb' of the circuit, that is, the hyperbolic waveform voltage Vhp' is Horizontal deflection sawtooth current
All you have to do is synthesize the Iyh envelope waveform as it is and its differential waveform at an appropriate ratio.

ところが、双曲線波形電圧Vhpは垂直偏向周期
ノコギリ波電圧Vst′を積分して得た波形であるか
ら、電圧Vhpの微分形は必ず電圧Vst′となり、従
つて、電圧Vst′と電圧Vhpを適当な割合で(偏向
コイルのL,R比に従つて)合成してやれば、水
平偏向ノコギリ波電流Iyhの包絡線の形は双曲線
波形電圧Vhpと同じくなる。
However, since the hyperbolic waveform voltage Vhp is a waveform obtained by integrating the vertical deflection periodic sawtooth wave voltage Vst', the differential form of the voltage Vhp is always the voltage Vst'. If they are combined in proportion (according to the L and R ratios of the deflection coils), the shape of the envelope of the horizontal deflection sawtooth wave current Iyh will be the same as that of the hyperbolic waveform voltage Vhp.

この事から、もし、SPC歪補正の為に、水平偏
向ノコギリ波電流Iyhの包絡線の形を正しく双曲
線にしたい場合は、先ず積分して双曲線になる様
な電圧Vst′を作り、これとその積分波形とを合成
して、水平偏向出力回路1の電源電圧を変調して
やれば良い。
From this, if you want to make the envelope of the horizontal deflection sawtooth wave current Iyh correctly hyperbolic for SPC distortion correction, first create the voltage Vst' that becomes a hyperbola by integrating it, and then What is necessary is to synthesize the integrated waveform and modulate the power supply voltage of the horizontal deflection output circuit 1.

この様にすると、例えば偏向振幅を変化させる
場合、水平偏向ノコギリ波電流Iyhの振幅の変化
に応じてその変調包絡線の振幅も変えなければな
らないが、この第1図の場合は電圧Vst′の振幅だ
け変えてやれば、電圧Vst′Vhp共、同時に比例し
て変化するから、水平偏向ノコギリ波電流Iyhの
包絡線もそのままの形を保ちながら変化させる事
が出来る。
In this way, for example, when changing the deflection amplitude, the amplitude of the modulation envelope must be changed in accordance with the change in the amplitude of the horizontal deflection sawtooth current Iyh. If only the amplitude is changed, the voltage Vst'Vhp will also change proportionally at the same time, so the envelope of the horizontal deflection sawtooth wave current Iyh can also be changed while keeping its shape.

また、包絡線波形の微調整の為に、電圧Vst′の
波形が多少変形しても、必ず双曲線波形電圧Vhp
の波形と水平偏向ノコギリ波電流Iyhの包絡線の
波形とは一致し、調整が極めてやりやすい。
In addition, due to fine adjustment of the envelope waveform, even if the waveform of the voltage Vst′ is slightly deformed, the hyperbolic waveform voltage Vhp is always
The waveform of and the waveform of the envelope of the horizontal deflection sawtooth current Iyh match, making adjustment extremely easy.

また、第2図は同じく本発明を更に詳細に説明
する為の回路図であつて、やはり先の第1図と同
一番号部分は同様な働きをしているものとする。
FIG. 2 is also a circuit diagram for explaining the present invention in more detail, and it is assumed that the same numbered parts as in FIG. 1 have the same functions.

波形整形回路15の内部回路構成の一例をここ
で説明すると、先ず、17は第一の直流阻止コン
デンサ、18は充放電抵抗、19は第一のスライ
スダイオード、20は第一の放電抵抗、21は第
二の直流阻止コンデンサ、22は第二のスライス
ダイオード、23は第二の放電抵抗兼補正振幅調
整用可変抵抗である。
An example of the internal circuit configuration of the waveform shaping circuit 15 will be described here. First, 17 is a first DC blocking capacitor, 18 is a charging/discharging resistor, 19 is a first slice diode, 20 is a first discharging resistor, 21 2 is a second DC blocking capacitor, 22 is a second slice diode, and 23 is a second discharge resistor/variable resistor for adjusting the correction amplitude.

また、積分回路16の内部については、先ず2
4は第一の演算増幅器、25は前段よりの結合コ
ンデンサ、26は第一の演算増幅器24の入力抵
抗、27,28は第一の演算増幅器24の直流動
作点決定用抵抗、29は積分用時定数コンデン
サ、30は直流利得制限抵抗である。
Also, regarding the inside of the integrating circuit 16, first 2
4 is the first operational amplifier, 25 is a coupling capacitor from the previous stage, 26 is an input resistance of the first operational amplifier 24, 27 and 28 are resistors for determining the DC operating point of the first operational amplifier 24, and 29 is for integration. The time constant capacitor 30 is a DC gain limiting resistor.

また更に、加算回路14の内部については、3
1は第二の演算増幅器、32は入力結コンデン
サ、33は演算増幅器31の入力抵抗、34,3
5は演算増幅器31の直流動作点決定用抵抗、3
6は補助電圧(波形)の入力結合コンデンサ、3
7は同じく補助電圧(波形)の振幅制限用入力抵
抗、38は演算増幅器31の利得決定用負帰還抵
抗である。
Furthermore, regarding the inside of the adder circuit 14, 3
1 is the second operational amplifier, 32 is the input capacitor, 33 is the input resistance of the operational amplifier 31, 34, 3
5 is a resistor for determining the DC operating point of the operational amplifier 31;
6 is an input coupling capacitor for auxiliary voltage (waveform), 3
7 is an input resistor for limiting the amplitude of the auxiliary voltage (waveform), and 38 is a negative feedback resistor for determining the gain of the operational amplifier 31.

また、6は先に第5図で説明した電源電圧変調
による水平振幅変調回路であつて、その内部の
個々の構成も同じものを例にとつているので、そ
の説明は省略する。
Further, reference numeral 6 is a horizontal amplitude modulation circuit using power supply voltage modulation as previously explained with reference to FIG. 5, and since the individual internal configurations are also the same, the explanation thereof will be omitted.

この第2図の様にすると、先ず波形整形回路1
5では垂直周期ノコギリ波電圧Vstの正側ピーク
付近(走査前端付近)で第一のスライスダイオー
ド19が時間t1だけ導通し、電圧(波形)Vst
の頂部をスライスする。また、第二のスライスダ
イオード22は走査終端付近で時間t2だけ導通
し、電圧(波形)Vstの下端部をスライスする。
この両方のスライス時間t1,t2の長さは、直
流阻止コンデンサ17,21、充放電抵抗18、
放電抵抗20、可変抵抗23の定数によつてて、
夫々独立に決定する事が出来る。
If the configuration is as shown in Fig. 2, first the waveform shaping circuit 1
5, the first slice diode 19 conducts for a time t1 near the positive peak of the vertical periodic sawtooth wave voltage Vst (near the scanning front end), and the voltage (waveform) Vst
Slice off the top. Further, the second slicing diode 22 becomes conductive for a time t2 near the end of the scan, slicing the lower end of the voltage (waveform) Vst.
The lengths of both slice times t1 and t2 are as follows: DC blocking capacitors 17, 21, charging/discharging resistor 18,
Depending on the constants of the discharge resistor 20 and variable resistor 23,
They can each decide independently.

そして、これらの定数が変らなければ時間t
1,t2は入力垂直周期ノコギリ波電圧Vstの振
幅が変つてもt一定であり、電圧Vst′は変らな
い。更に、この電圧VSt′は可変抵抗23によつ
て大きさを調整されて次段に加えられる。
And if these constants do not change, time t
1, t2 remains constant even if the amplitude of the input vertical periodic sawtooth wave voltage Vst changes, and the voltage Vst' does not change. Further, this voltage VSt' is adjusted in magnitude by a variable resistor 23 and is applied to the next stage.

次の積分回路16で電圧VSt′は結合コンデン
サ25で直流分をカツトされた後、入力抵抗26
を通して演算増幅器24の反転入力端子に加えら
れる。すると、コンデンサ29、抵抗30の積の
値を積分時定数として、演算増幅器24の出力端
子には電圧(波形)VSt′を反転して積分した電
圧(波形)−Vhpが得られる。
In the next integrating circuit 16, the voltage VSt' has its DC component cut off by a coupling capacitor 25, and then the input resistor 26
is applied to the inverting input terminal of operational amplifier 24 through the input terminal. Then, with the value of the product of the capacitor 29 and the resistor 30 as an integration time constant, a voltage (waveform) -Vhp obtained by inverting and integrating the voltage (waveform) VSt' is obtained at the output terminal of the operational amplifier 24.

また、抵抗27の一端は直流電源(電圧)+E
に接続し、抵抗27と28の値は出力電圧−Vhp
の電圧レベルが、充分、演算増幅器24のダイナ
ミツクレンジに収まる様設定する。
Also, one end of the resistor 27 is connected to the DC power supply (voltage) +E
and the value of resistors 27 and 28 is the output voltage - Vhp
The voltage level is set so as to be sufficiently within the dynamic range of the operational amplifier 24.

ここで得られた電圧−Vhpは、コンデンサ3
2、抵抗33を通し次の演算増幅器31の反転入
力端子に加えられる。すると、演算増幅器31の
出力端子には電圧−Vhpが抵抗38,33の比に
従つて反転増幅されて現われ、一方、電圧Vst′が
結合コンデンサ36、抵抗37を通してやはり演
算増幅器31の非反転入力端子に加わるので、電
圧Vst′が37,34,35の抵抗により分圧され
た後、演算増幅器31で増幅され、結局、演算増
幅器31の出力には電圧(波形)Vhpと電圧(波
形)VSt′との合成波形(双曲線波形電圧)
Vhp′となつて現われる。この合成波形Vhp′の電
圧波高値、及びVhp成分とVst′成分との割合は、
これまでの説明から明らかな様に、抵抗33,3
8,37,34,35等の値で自在に設定でき
る。
The voltage obtained here - Vhp is the capacitor 3
2. It is applied to the inverting input terminal of the next operational amplifier 31 through a resistor 33. Then, the voltage -Vhp appears at the output terminal of the operational amplifier 31 after being inverted and amplified according to the ratio of the resistors 38 and 33, while the voltage Vst' appears at the non-inverting input of the operational amplifier 31 through the coupling capacitor 36 and the resistor 37. Since it is applied to the terminal, the voltage Vst' is divided by the resistors 37, 34, and 35, and then amplified by the operational amplifier 31. Eventually, the output of the operational amplifier 31 is the voltage (waveform) Vhp and the voltage (waveform) VSt. ′ composite waveform (hyperbolic waveform voltage)
It appears as Vhp′. The voltage peak value of this composite waveform Vhp′ and the ratio of the Vhp component to the Vst′ component are:
As is clear from the explanation so far, the resistance 33,3
It can be freely set to values such as 8, 37, 34, 35, etc.

また、演算増幅器24と同様、抵抗34の一端
は直流電源+Eに接続されているが、抵抗34と
35の比は演算増幅器31の出力Vhp′の電圧レ
ベルが、丁度、演算増幅器31のダイナミツクレ
ンジ内に収まる様に設定すれば良い。
Also, like the operational amplifier 24, one end of the resistor 34 is connected to the DC power supply +E, but the ratio between the resistors 34 and 35 is such that the voltage level of the output Vhp' of the operational amplifier 31 is just the same as the dynamic voltage level of the operational amplifier 31. Just set it so that it stays within the range.

この様にして得られた合成波形Vhp′は、先の
第5図の場合と同様、結合コンデンサ10を介し
て電圧制御トランジスタ7のベースに加えられ
る。すると、水平偏向出力回路1の供給直流電源
電圧Eb′の変調電圧(波形)が合成波形Vhp′と同
じくなり、水平偏向コイル2を流れる水平偏向ノ
コギリ波電流Iyhの包絡線の形が先に説明した原
理により電圧(波形)Vhpの形で一致する様にな
る。
The composite waveform Vhp' thus obtained is applied to the base of the voltage control transistor 7 via the coupling capacitor 10, as in the case of FIG. 5 above. Then, the modulation voltage (waveform) of the DC power supply voltage Eb' supplied to the horizontal deflection output circuit 1 becomes the same as the composite waveform Vhp', and the shape of the envelope of the horizontal deflection sawtooth wave current Iyh flowing through the horizontal deflection coil 2 is explained first. Due to this principle, the voltage (waveform) Vhp will match.

尚、この様にしてノコギリ波の上下端をスライ
スして得た電圧(波形)st′を積分した場合、完
全な双曲線になる訳ではなく、走査両端が直線で
中央部が放物線である様な波形となる。
Note that when integrating the voltage (waveform) st′ obtained by slicing the upper and lower ends of the sawtooth wave in this way, it does not become a perfect hyperbola, but rather a straight line at both ends of the scan and a parabola at the center. It becomes a waveform.

しかし、これで、充分、双曲線に近似出来、従
来よく見られる様に単純な放物線だけで水平偏向
ノコギリ波電流Iyhを変調するよりは、はるかに
良好にラスターのSPC歪を補正出来る。
However, this can be sufficiently approximated to a hyperbola, and the raster SPC distortion can be corrected much better than modulating the horizontal deflection sawtooth wave current Iyh with only a simple parabola, as is often seen in the past.

また、もとのノコギリ波電圧Vstの生成の際、
斜降部分が直線とならずエクスポーネンシヤル成
分が入つて湾曲する事がある。
Also, when generating the original sawtooth wave voltage Vst,
The sloped part may not be a straight line but may be curved due to an exponential component.

この様な場合、走査後端のスライス時間t2は
時間t1よりも、更に短くした方が結果として対
称性の良い疑似双曲線が得られる事が多く、時間
t1だけのスライスでも充分実用になる場合があ
る。
In such cases, it is often better to make the slice time t2 at the rear end of the scan even shorter than time t1, resulting in a pseudo-hyperbola with better symmetry, and slicing only at time t1 may be sufficient for practical use. be.

また、水平偏向コイルの特性と、受像管受像面
の形状によつては、水平偏向ノコギリ波電流の包
絡線の形は完全な双曲線から若干ずらした方がよ
い場合がある。
Further, depending on the characteristics of the horizontal deflection coil and the shape of the picture tube image receiving surface, it may be better to slightly deviate the shape of the envelope of the horizontal deflection sawtooth wave current from a perfect hyperbola.

この様な場合の回路の例について、一つ一つ図
示しないが、例えば19,22のスライスダイオ
ードに適当なインピーダンスを挿入してハーフク
ランプにしたり、あるいは充放電抵抗18に小容
量を並列に付加して微分波形を加えたりして双曲
線波形電圧Vhpの波形、即ち水平偏向ノコギリ波
電流Iyhの包絡線の波形を細かく修正する方法が
ある。
Examples of circuits in such a case are not shown one by one, but for example, a suitable impedance is inserted into the slice diodes 19 and 22 to create a half clamp, or a small capacitance is added in parallel to the charging/discharging resistor 18. There is a method of finely modifying the waveform of the hyperbolic waveform voltage Vhp, that is, the waveform of the envelope of the horizontal deflection sawtooth wave current Iyh, by adding a differential waveform.

この様な場合、双曲線波形電圧Vhpの波形をど
のよううに修正したとしても、水平偏向出力回路
1の電源電圧としての直流電源電圧Eb′の変調電
圧(波形)は、必ず本来の目的の電圧Vhpとそれ
を微分した電圧(波形)VSt′との一定割合での
合成波形になり、正しく水平偏向ノコギリ波電流
Iyhを双曲線波形電圧Vhpで変調する事が出来る。
In such a case, no matter how the waveform of the hyperbolic waveform voltage Vhp is modified, the modulation voltage (waveform) of the DC power supply voltage Eb' as the power supply voltage of the horizontal deflection output circuit 1 will always be the original target voltage Vhp. The resulting waveform is a composite waveform of the voltage (waveform) VSt′ obtained by differentiating it at a constant ratio, and the horizontal deflection sawtooth wave current is correctly calculated.
Iyh can be modulated with hyperbolic waveform voltage Vhp.

(発明の効果) 以上の様に、本発明の画像歪補正回路によれ
ば、必ず双曲線波形電圧(Vhp)の波形と同じ波
形で水平偏向ノコギリ波電流(Iyh)を変調する
事が出来るので、極めて容易に水平偏向ノコギリ
波電流を目的の波形で自在に変調する事が出来、
受像管ラスターの左右端の形状の補正が出来、特
にSPC歪補正をより精密に行なう場合に効果があ
るものである。
(Effects of the Invention) As described above, according to the image distortion correction circuit of the present invention, it is possible to modulate the horizontal deflection sawtooth wave current (Iyh) with the same waveform as the hyperbolic waveform voltage (Vhp). It is extremely easy to modulate the horizontal deflection sawtooth wave current with the desired waveform.
It is possible to correct the shape of the left and right ends of the picture tube raster, and is particularly effective when performing SPC distortion correction more precisely.

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

第1図は本発明による画像歪補正回路の一実施
例を示すブロツク図、第2図は本発明のより具体
的な回路の一例を示す図、第3図は本発明によつ
て補正されるべき受像管のSPC歪を説明するため
の図、第4図はSPC歪補正のための従来例のブロ
ツク図、第5図はやはり従来例のより具体的な回
路の一例を示す図、第6図は本発明に関する水平
偏向コイルの等価回路とそこに生じる波形を示す
図である。 1…水平偏向出力回路、2…水平偏向コイル、
3…垂直偏向出力回路、4…垂直偏向コイル、5
…双曲線波形発生回路、6…水平振幅変調回路、
7…電圧制御NPN型トランジスタ、8…ベース
バイアス抵抗、9…平滑コンデンサ、10,25
…結合コンデンサ、11…制御回路、12,23
…可変抵抗、13…補正波形発生回路、14…加
算回路、15…波形整形回路、16…積分回路、
17,21…直流阻止コンデンサ、18…充放電
抵抗、20…放電抵抗、19,22…スライスダ
イオード、24,31…演算増幅器、Eb…直流
電源電圧、Eb′…変調された直流電源電圧、Iyh
…水平偏向ノコギリ波電流、Iyv…垂直偏向ノコ
ギリ波電流、i…水平偏向コイルに流れる垂直周
期のリツプル電流、is…制御電流、L…水平偏向
コイルのインダクタンス分、R…水平偏向コイル
の直流抵抗分、Vaux…補正電圧(波形)、Vhp…
双曲線波形電圧、Vhb′…補正波形を加えた双曲
線波形電圧、Vst…垂直周期ノコギリ波電圧、
Vst′…スライスされた垂直周期ノコギリ波電圧。
FIG. 1 is a block diagram showing an embodiment of an image distortion correction circuit according to the present invention, FIG. 2 is a diagram showing an example of a more specific circuit according to the present invention, and FIG. 3 is a block diagram showing an example of an image distortion correction circuit according to the present invention. FIG. 4 is a block diagram of a conventional example for correcting SPC distortion, FIG. 5 is a diagram showing an example of a more specific circuit of the conventional example, and FIG. The figure is a diagram showing an equivalent circuit of a horizontal deflection coil and waveforms generated therein according to the present invention. 1...Horizontal deflection output circuit, 2...Horizontal deflection coil,
3... Vertical deflection output circuit, 4... Vertical deflection coil, 5
...Hyperbolic waveform generation circuit, 6...Horizontal amplitude modulation circuit,
7... Voltage control NPN type transistor, 8... Base bias resistor, 9... Smoothing capacitor, 10, 25
...Coupling capacitor, 11...Control circuit, 12, 23
...variable resistor, 13...correction waveform generation circuit, 14...addition circuit, 15...waveform shaping circuit, 16...integrator circuit,
17, 21... DC blocking capacitor, 18... Charging/discharging resistor, 20... Discharging resistor, 19, 22... Slice diode, 24, 31... Operational amplifier, Eb... DC power supply voltage, Eb'... Modulated DC power supply voltage, Iyh
...Horizontal deflection sawtooth wave current, Iyv...Vertical deflection sawtooth wave current, i...Vertical cycle ripple current flowing through the horizontal deflection coil, is...Control current, L...Inductance of the horizontal deflection coil, R...DC resistance of the horizontal deflection coil Minutes, Vaux…corrected voltage (waveform), Vhp…
Hyperbolic waveform voltage, Vhb′...Hyperbolic waveform voltage with correction waveform added, Vst...Vertical periodic sawtooth wave voltage,
Vst′…Sliced vertical periodic sawtooth wave voltage.

Claims (1)

【特許請求の範囲】 1 受像管を水平偏向するための水平偏向回路
と、同じく垂直偏向するための垂直偏向回路と、
前記水平偏向回路の電源電圧を変調する電源電圧
変調回路とがあつて、前記垂直偏向回路より得た
垂直偏向周期の偏向補正波形を、前記電源電圧変
調回路に加えてラスター左右端の形状を補正する
画像歪補正回路において、 前記偏向補正波形は、垂直偏向周期のノコギリ
波状の電圧波形を波形整形回路を通し、該電圧波
形のピーク値及び、もしくはボトム値の付近の形
状を整形して得た第1の信号と、前記第1の信号
を積分回路を通して得た第2の信号とを加算する
事によつて得る様にした事を特徴とする画像歪補
正回路。
[Claims] 1. A horizontal deflection circuit for horizontally deflecting the picture tube, and a vertical deflection circuit for vertically deflecting the picture tube,
A power supply voltage modulation circuit modulates the power supply voltage of the horizontal deflection circuit, and a deflection correction waveform of the vertical deflection period obtained from the vertical deflection circuit is added to the power supply voltage modulation circuit to correct the shape of the left and right ends of the raster. In the image distortion correction circuit, the deflection correction waveform is obtained by passing a sawtooth voltage waveform of a vertical deflection period through a waveform shaping circuit and shaping the shape of the voltage waveform near its peak value and/or bottom value. An image distortion correction circuit characterized in that the image distortion correction circuit is obtained by adding a first signal and a second signal obtained by passing the first signal through an integrating circuit.
JP1429388A 1988-01-25 1988-01-25 Picture distortion correcting circuit Granted JPH01190082A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1429388A JPH01190082A (en) 1988-01-25 1988-01-25 Picture distortion correcting circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1429388A JPH01190082A (en) 1988-01-25 1988-01-25 Picture distortion correcting circuit

Publications (2)

Publication Number Publication Date
JPH01190082A JPH01190082A (en) 1989-07-31
JPH0586114B2 true JPH0586114B2 (en) 1993-12-09

Family

ID=11857046

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1429388A Granted JPH01190082A (en) 1988-01-25 1988-01-25 Picture distortion correcting circuit

Country Status (1)

Country Link
JP (1) JPH01190082A (en)

Also Published As

Publication number Publication date
JPH01190082A (en) 1989-07-31

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