JPS6053510B2 - television receiver - Google Patents
television receiverInfo
- Publication number
- JPS6053510B2 JPS6053510B2 JP6373077A JP6373077A JPS6053510B2 JP S6053510 B2 JPS6053510 B2 JP S6053510B2 JP 6373077 A JP6373077 A JP 6373077A JP 6373077 A JP6373077 A JP 6373077A JP S6053510 B2 JPS6053510 B2 JP S6053510B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- scanning speed
- output
- circuit
- video signal
- 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
Links
Landscapes
- Transforming Electric Information Into Light Information (AREA)
- Details Of Television Scanning (AREA)
Description
【発明の詳細な説明】
テレビジョン受像機で画像を映出させる場合、輝度の
高い部分では受像管のビーム電流が増加するためにビー
ムのスポットサイズが大きくなり鮮鋭度が低下してしま
う。DETAILED DESCRIPTION OF THE INVENTION When displaying an image on a television receiver, the beam current of the picture tube increases in areas with high brightness, which increases the beam spot size and reduces sharpness.
特に第1図Aに示すように水平方向の輪郭部分1や同図
Bに示すように線の部分2では、本来の映像信号は第2
図Aに示すように黒レベルと白レベルの間で急峻に変化
するが、受像機の伝送系の周波数特性のため高域成分が
減衰するので、信号は同図Bに示すようになまつて水平
方向の鮮鋭度は一層低下してしまう。 そこで、鮮鋭度
の低下を補償する方法として、第2図Bの映像信号50
から同図cに示すような2次微分信号SBを得、これを
信号s゜に加えて同図Dに示すような立トリ及び立下り
の急峻な映像信号Scを得、これを受像管に供給する方
法がある。 しカルながら、この方法では、信号のピー
クの部分でビーム電流がより増加するので、ビームのス
ポットサイズは一層大きくなり、そのため鮮鋭度はそれ
程改善されない。In particular, in the horizontal contour portion 1 as shown in FIG. 1A and the line portion 2 as shown in FIG. 1B, the original video signal is
As shown in Figure A, there is a sharp change between the black level and white level, but due to the frequency characteristics of the receiver's transmission system, the high-frequency components are attenuated, so the signal becomes distorted as shown in Figure B. Horizontal sharpness is further reduced. Therefore, as a method of compensating for the decrease in sharpness, the video signal 50 shown in FIG.
From this, we obtain a second-order differential signal SB as shown in c in the same figure, and add this to the signal s° to obtain a video signal Sc with steep rise and fall as shown in D in the same figure, which is input to the picture tube. There is a way to supply it. However, in this method, the beam current increases more at the peak of the signal, so the beam spot size becomes larger, so the sharpness is not improved as much.
また、別な方法として、第3図Aの映像信号50をそ
のまま受像管に供給するとともに、この映像信号50を
微分して同図Bに示すような信号SAを得、これを例え
ば主偏向コイルとは別に設けた補助偏向コイルに供給し
て水平偏向磁界を同図cに示すように補正し、これによ
りスクリーン上でのビームの走査速度を同図Dに示すよ
うに変調する方法がある。As another method, the video signal 50 shown in FIG. 3A is supplied as is to the picture tube, and this video signal 50 is differentiated to obtain a signal SA shown in FIG. There is a method in which the horizontal deflection magnetic field is supplied to an auxiliary deflection coil provided separately to correct the horizontal deflection magnetic field as shown in FIG.
この方法によれば、区間Taではビームの走査速度が早
くなつてスクリーン上の対応する点の発光量は減少し、
区間′几ではビームの走査速度が遅くなつてスクリーン
上の対応する点の発光量は増加するので、ビームのスポ
ットサイズを考慮するとスクリーン上の水平方向の発光
量は第3図Eに示すように変化し水平方向の鮮鋭度が改
善される。しかしながら、この方法によるときは、図か
ら明らかなように、スクリーン上の発光部分の幅が映像
信号SOの時間幅に対応せず細くなつてしまうという欠
点がある。According to this method, the scanning speed of the beam increases in the section Ta, and the amount of light emitted at the corresponding point on the screen decreases.
In section 1, the scanning speed of the beam slows down and the amount of light emitted at the corresponding point on the screen increases, so considering the spot size of the beam, the amount of light emitted in the horizontal direction on the screen is as shown in Figure 3E. horizontal sharpness is improved. However, as is clear from the figure, this method has the disadvantage that the width of the light-emitting portion on the screen does not correspond to the time width of the video signal SO and becomes narrow.
しかも、この場合、走査速度変調用信号のレベルを大き
くして、走査速度の変調をより強くかける場合ほど、ス
クリーン上の発光部分の幅がより細くなつてしまうとい
う不都合がある。この発明は、上述の点にかんがみ、走
査速度の変調を行つても発光部分の幅が細くなつてしま
うことがなく、しかも走査速度の変調の度合の強弱にか
かわらず発光部分の幅が一定になるようにしたものであ
る。Furthermore, in this case, there is a disadvantage that the width of the light-emitting portion on the screen becomes narrower as the level of the scanning speed modulation signal is increased and the scanning speed is more strongly modulated. In view of the above-mentioned points, this invention prevents the width of the light-emitting portion from becoming narrower even when the scanning speed is modulated, and furthermore, the width of the light-emitting portion remains constant regardless of the degree of modulation of the scanning speed. It was made so that it would become so.
第4図はその一例で、映像増幅器10を通じて取り出さ
れたもとの映像信号SO(第7図A)を微分信号発生回
路として例えば微分回路11にて微分して微分信号SA
(同図B)を得、この微分信号SAを極性反転回路12
を有する同極性化回路13に供給して信号SAのうちの
映像信号SOの立下り部に対応する部分を極性反転した
状態の信号SO(同図C)を得、この信号SDを可変利
得アンプ14に供給し、合成器15において、もとの映
像信号SOに対してアンプ14から得られる信号S8(
同図D)を合成する。FIG. 4 is an example of this, in which the original video signal SO (FIG. 7A) taken out through the video amplifier 10 is differentiated by a differential signal generation circuit, for example, a differential circuit 11, and a differential signal SA is generated.
(B in the same figure) is obtained, and this differential signal SA is sent to the polarity inversion circuit 12.
is supplied to the same polarization circuit 13 having a polarization circuit 13 to obtain a signal SO (C in the same figure) in which the polarity of the portion of the signal SA corresponding to the falling edge of the video signal SO is inverted, and this signal SD is sent to a variable gain amplifier. 14, and in the synthesizer 15, the signal S8(
D) in the same figure is synthesized.
この同極性化回路13と可変利得アンプ14とで補正信
号発生回路を構成する。このようにして、信号加算回路
として例えば合成器15から、もとの映像信号SOに比
べて白信号の幅が広くされた映像出力信号Sp″(同図
E)を得る。そして、この映像出力信号Spを受像管1
6のカソード17に供給して電子ビームを密度変調する
。一方、例えば映像出力信号S,を走査速度信号処理回
路内の微分回路20にて微分して微分信号SvO(同図
F)を得、この微分信号SvOを走査速度信号処理回路
の出力段に当たる可変利得アンプ21に供給し、アンプ
21から得られる信号Svを走査速度変調用信号として
受像管16に例えば水平及び垂直の偏向手段18とは別
個に設けた走査速度変調用偏向手段19に供給して、受
像管16のスクリーン上における電子ビームの走査速度
を変調する。This polarization circuit 13 and variable gain amplifier 14 constitute a correction signal generation circuit. In this way, a video output signal Sp'' (E in the same figure) in which the width of the white signal is made wider than that of the original video signal SO is obtained from the synthesizer 15 as a signal addition circuit, for example. Signal Sp to picture tube 1
The electron beam is supplied to the cathode 17 of No. 6 to density-modulate the electron beam. On the other hand, for example, the video output signal S, is differentiated by the differentiating circuit 20 in the scanning speed signal processing circuit to obtain the differential signal SvO (F in the same figure). The signal Sv obtained from the amplifier 21 is supplied to a gain amplifier 21, and the signal Sv obtained from the amplifier 21 is supplied as a scanning speed modulation signal to a scanning speed modulation deflection means 19 provided separately from the horizontal and vertical deflection means 18 in the picture tube 16, for example. , modulates the scanning speed of the electron beam on the screen of the picture tube 16.
この走査速度変調用偏向手段19は、偏向手段18の手
前側において管16のネック部内に2枚の静電偏向板を
水平方向に対向して配置して構成することができる。こ
こで、可変利得アンプ14及び21の利得は輪部補正量
の利得調整手段として可変抵抗器22を調整することに
より同時に変えられるようにし、しかも、アンプ21の
利得が大きくされるときはアンプ14の利得も大きくさ
れるような方向に変えられるようにする。This scanning speed modulation deflection means 19 can be constructed by arranging two electrostatic deflection plates facing each other in the horizontal direction within the neck of the tube 16 on the near side of the deflection means 18. Here, the gains of the variable gain amplifiers 14 and 21 can be changed simultaneously by adjusting the variable resistor 22 as a gain adjustment means for the limbal correction amount, and when the gain of the amplifier 21 is increased, the gain of the amplifier 14 so that the gain can be changed in a direction such that the gain is also increased.
この発明によれば、上述した走査速度を変調することに
よる発光部分の幅の縮少は、映像信号の白信号の幅自体
が広げられることにより、補正される。According to this invention, the reduction in the width of the light emitting portion due to modulation of the scanning speed described above is corrected by widening the width of the white signal of the video signal itself.
しかも、この場合、アンプ21の利得を大きくして走査
速度変調用信号のレベルを大きくし、走査速度の変調を
強くかけるときほど、従つて走査速度の変調による発光
部分の幅の縮少の度合が大きくなるほど、映像出力信号
Spにおける白信号の幅は広くされるので、走査速度の
変調の強弱にかかわらず、発光分布は第7図Hの線5で
示すように均一になり、発光部分の幅はもとの映像信号
SOの立上りの中間点から立下りの中間点までの時間に
対応した一定のものとなる。第5図の例のように、微分
回路11から得られる微分信号SAを可変利得アンプ2
1に供給して走査速度変調用信号Svを得るようにして
もよい。Moreover, in this case, when the gain of the amplifier 21 is increased to increase the level of the scanning speed modulation signal and the scanning speed is more strongly modulated, the width of the light emitting portion is reduced by the scanning speed modulation. The larger the width of the white signal in the video output signal Sp is, the wider the width of the white signal in the video output signal Sp becomes. Therefore, regardless of the strength of the scanning speed modulation, the light emission distribution becomes uniform as shown by line 5 in FIG. The width is a constant value corresponding to the time from the midpoint of the rise to the midpoint of the fall of the original video signal SO. As in the example shown in FIG.
1 to obtain the scanning speed modulation signal Sv.
また、もとの映像信号SOに合成すべき信号は、上述の
ようにもとの映像信号SOの1次微分信号SAではなく
、第7図1に示すような2次微分信号でもよく、あるい
はこれらを適当なレベルの比で合成したようなものであ
つてもよい。Further, the signal to be combined with the original video signal SO may be a second-order differential signal as shown in FIG. 71, instead of the first-order differential signal SA of the original video signal SO as described above, or It may be something like a combination of these at an appropriate level ratio.
走査速度変調用偏向手段19は、第6図に示すように受
像管16の電子銃の例えば集束電極を特殊に形成するこ
とにより構成することもできる。即ち、第6図は管16
のネック部内の電子銃を示すもので、カソード30、制
御電極31、加速電極32、第1陽極33、集束電極3
4及び第2陽極35が順次同じ軸心上に配列されている
。そして、集束電極34を、1つの円筒体をその中間部
において水平面と直交するも管軸と斜めに交わる平面に
よつて切断したような形状を有するように分割された2
個の電極部34A及び34Bにて構成し、電極部34A
及び34Bにはそれぞれ零Vないし数KVの集束電圧を
供給するとともに、これに重畳して両電極部34A及び
34B間に上述の走査速度変調用信号Svを供給する。
従つて、集束電極34の位置で信号Svによつて水平方
向の電界が発生し、これによりビーム36が水平方向に
偏向されてスクリーン上においてビーム36の走査速度
が変調される。また、水平偏向コイルを走査速度変調用
偏向手段に兼用させ、水平偏向信号に対して上述の走査
速度変調用信号を合成したものをこれに供給してもよい
。The scanning speed modulation deflection means 19 can also be constructed by specially forming, for example, a focusing electrode of the electron gun of the picture tube 16, as shown in FIG. That is, in FIG.
This figure shows the electron gun in the neck part of , which includes a cathode 30, a control electrode 31, an accelerating electrode 32, a first anode 33, and a focusing electrode 3.
4 and the second anode 35 are sequentially arranged on the same axis. The focusing electrode 34 is divided into two parts each having a shape similar to that of a single cylindrical body cut by a plane that is perpendicular to the horizontal plane at the middle part and diagonally intersects with the tube axis.
Consisting of electrode parts 34A and 34B, the electrode part 34A
and 34B are respectively supplied with a focusing voltage of zero V to several KV, and superimposed thereon, the above-mentioned scanning speed modulation signal Sv is supplied between both electrode portions 34A and 34B.
Therefore, a horizontal electric field is generated by the signal Sv at the location of the focusing electrode 34, which deflects the beam 36 horizontally and modulates the scanning speed of the beam 36 on the screen. Alternatively, the horizontal deflection coil may also be used as the deflection means for scanning speed modulation, and a combination of the above-mentioned scanning speed modulation signal and the horizontal deflection signal may be supplied thereto.
なお、この発明はカラーテレビジョン受像機にも適用で
きるもので、この場合には輝度信号を上述の映像信号と
して扱えばよい。Note that the present invention can also be applied to a color television receiver, and in this case, the luminance signal may be treated as the above-mentioned video signal.
【図面の簡単な説明】
第1図〜第3図はこの発明の説明のための図、第4図及
び第5図はそれぞれこの発明の一例の系統図、第6図は
走査速度変調用偏向手段の二例の断面図、第7図はこの
発明の説明のための波形図である。
10は映像増幅器、11及び20は微分回路、13は同
極性化回路、14及び21は可変利得アンプ、16は受
像管である。[Brief Description of the Drawings] Figures 1 to 3 are diagrams for explaining the present invention, Figures 4 and 5 are system diagrams of an example of the present invention, and Figure 6 is a deflection for scanning speed modulation. FIG. 7 is a sectional view of two examples of the means and a waveform diagram for explaining the present invention. 10 is a video amplifier, 11 and 20 are differentiating circuits, 13 is a polarization circuit, 14 and 21 are variable gain amplifiers, and 16 is a picture tube.
Claims (1)
発生回路と、この出力の負極性成分を反転してこの正極
性成分と加算して映像信号の立上り部及び立下り部で同
極性の補正信号を得る補正信号発生回路と、この出力を
可変利得アンプを介してもとの映像信号に加算して白信
号の幅が拡大された映像出力信号を得る信号加算回路と
、この映像出力信号又は上記もとの映像信号から走査速
度変調用信号を発生する走査速度信号処理回路と、この
出力で駆動され電子ビームの走査速度を変調する走査速
度変調用偏向手段と、上記可変利得アンプの利得を制御
する利得調整手段の夫々を設けるとともに、この利得調
整手段の制御出力を上記走査速度信号処理回路にも供給
し、もつて上記補正信号のレベルと上記走査速度変調の
変調度を連動して同時に可変できるようにしたことを特
徴とするテレビジョン受像機。1. A differential signal generation circuit that extracts this differential component from the original video signal, and inverts the negative polarity component of this output and adds it to this positive polarity component to correct the same polarity at the rising and falling parts of the video signal. a correction signal generation circuit that obtains a signal; a signal addition circuit that adds this output to the original video signal via a variable gain amplifier to obtain a video output signal in which the width of the white signal is expanded; a scanning speed signal processing circuit that generates a scanning speed modulation signal from the original video signal; a scanning speed modulation deflection means that is driven by the output of the circuit and modulates the scanning speed of the electron beam; In addition to providing respective gain adjustment means for controlling, the control output of the gain adjustment means is also supplied to the scanning speed signal processing circuit, so that the level of the correction signal and the modulation degree of the scanning speed modulation are linked and simultaneously controlled. A television receiver characterized by being variable.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6373077A JPS6053510B2 (en) | 1977-05-31 | 1977-05-31 | television receiver |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6373077A JPS6053510B2 (en) | 1977-05-31 | 1977-05-31 | television receiver |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53148324A JPS53148324A (en) | 1978-12-23 |
| JPS6053510B2 true JPS6053510B2 (en) | 1985-11-26 |
Family
ID=13237802
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6373077A Expired JPS6053510B2 (en) | 1977-05-31 | 1977-05-31 | television receiver |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6053510B2 (en) |
-
1977
- 1977-05-31 JP JP6373077A patent/JPS6053510B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53148324A (en) | 1978-12-23 |
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