JPS5974780A - Method and device for measurement of convergence - Google Patents

Method and device for measurement of convergence

Info

Publication number
JPS5974780A
JPS5974780A JP18511182A JP18511182A JPS5974780A JP S5974780 A JPS5974780 A JP S5974780A JP 18511182 A JP18511182 A JP 18511182A JP 18511182 A JP18511182 A JP 18511182A JP S5974780 A JPS5974780 A JP S5974780A
Authority
JP
Japan
Prior art keywords
color
measurement
pattern
measured
turn
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
JP18511182A
Other languages
Japanese (ja)
Inventor
Shinichi Uno
宇野 伸一
Mitsuji Inoue
井上 三津二
Riyuuhachirou Douro
堂路 隆八郎
Nobushi Suzuki
鈴木 悦四
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP18511182A priority Critical patent/JPS5974780A/en
Publication of JPS5974780A publication Critical patent/JPS5974780A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N17/00Diagnosis, testing or measuring for television systems or their details
    • H04N17/04Diagnosis, testing or measuring for television systems or their details for receivers

Landscapes

  • Engineering & Computer Science (AREA)
  • Health & Medical Sciences (AREA)
  • Biomedical Technology (AREA)
  • General Health & Medical Sciences (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Testing, Inspecting, Measuring Of Stereoscopic Televisions And Televisions (AREA)

Abstract

PURPOSE:To obtain effectively the quantity of misconvergence, by picking up a pattern for measurement with a CRT to be measured and then obtaining a measurement pattern of each emitted light color on the basis of the position information of each light emission pattern obtained previously from said picked-up measurement pattern. CONSTITUTION:A pattern generator 10 generates the white color pattern to the entire surface of a three color picture receiving CRT1 to be measured, and the information is displayed by a TV electronic circuit 11. At the same time, an optical filter 3 is revolved by a filter switching mechanism 4 to set a blue separating filter. Under such conditions, a specific area of a display pattern of the CRT1 is picked up by an ITV camera 2. This image pickup signal undergoes an A/D conversion through an image memory circuit 6 and then an aritmetic control 7 to obtain the region information. Then measurement patterns are picked up at a time and not detected in time division for each color. Thus the quantity of misconvergence can be calculated.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、3色カラー受像管における3電子ビ一ムo集
中状m、、つまシコンパーゼンスヲ測定するだめのコン
バーゼンス測定方法およびその測定装置の改良に関する
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a convergence measuring method and a measuring device for measuring the convergence of three electron beams in a three-color picture tube. Regarding the improvement of

〔発明の技術的背景〕[Technical background of the invention]

従来、3色カラー受像管のコンバ−ゼンスを測定する方
法としては、例えば被測定受像管としてのカラー受像管
にコンバーゼンス測定用の・ぐターン(測定パターン)
を表示させ、この表示パターン金色分離フィルタによシ
青、赤、緑の各発光色毎に分離して各単色ツヤターン毎
に工業用テレビジョン(ITV )カメラで撮像し、こ
れらの撮像情報から各発光色毎に測定ツヤターンの発光
中心を求めてその相対位置のずれヲミスコンパーゼンス
社情報として得るものがある。
Conventionally, as a method for measuring the convergence of a three-color picture tube, for example, a color picture tube as a picture tube to be measured has a pattern (measurement pattern) for convergence measurement.
This display pattern is separated into blue, red, and green light emitting colors using a golden separation filter, and images are taken with an industrial television (ITV) camera for each monochromatic gloss turn. For each luminescent color, the luminescent center of the measured gloss turn is determined and the relative position deviation is obtained as information from Miscompersence.

〔背景技術の問題点〕[Problems with background technology]

ところが、このような従来の測定方法は、各色の測定パ
ターンをいわゆる時分割で検出しているため、各色の測
定パターンを検出する間に電源の変動や雑音の発生、テ
レビジョン電子回路とITVカメラとの同期ずれによる
カラー受像管表示面の輝度変化等が生じると、各色測定
iJ?ターンの測定条件が変化することになシ、これに
より正確なミスコンノ々−ゼンス量が得られないという
欠点がある。
However, in this conventional measurement method, the measurement pattern of each color is detected in a so-called time-division manner, which causes fluctuations in the power supply, generation of noise, and interference between the television electronic circuit and ITV camera while detecting the measurement pattern of each color. If the brightness of the color picture tube display surface changes due to synchronization with the iJ? This method has the drawback that the measurement conditions for the turns change, and as a result, accurate misconception amounts cannot be obtained.

また、別のコンバーゼンス測定方法として、色分離フィ
ルタを用いずに各発光色に対応する電子ビームを時分割
で出力させ、これによシ各発光色毎の測定・ぐターン金
得るものがある。しかし、この方法にあっても、各色の
測定パターンを得るまでに時間差があることに変わりは
なく、このため前記色分離フィルタを用いた場合と同様
に電源変動等の影響を避けることができない。また、こ
の種の方法では各色の電子ビームを切換えてからそれに
よる発光状態が安定するまでに時間がかかるため、測定
に多くの時間を必要として測定能率が悪かった。
Another convergence measuring method is to emit electron beams corresponding to each emission color in a time-division manner without using a color separation filter, thereby obtaining measurements for each emission color. However, even with this method, there is still a time difference until the measurement pattern of each color is obtained, and therefore, as in the case of using the color separation filter, the influence of power supply fluctuations etc. cannot be avoided. Furthermore, in this type of method, it takes time to stabilize the light emitting state after switching the electron beams of each color, so a large amount of time is required for measurement, resulting in poor measurement efficiency.

〔発明の目的〕[Purpose of the invention]

本発明は、測定ノfターンを各発光色毎に各別に検出す
ることなく同時に検出できるようにし、これによ9時間
的変動要素を除去してコンバーゼンス測定精度を高め、
かつ測定時間を短縮して測定能率の向上をはかシ得るコ
ンバーゼンス測定方法およびその測定装置を提供するこ
とを目的とする。
The present invention enables measurement f-turns to be detected simultaneously without having to detect each emission color separately, thereby eliminating temporal fluctuation elements and improving convergence measurement accuracy.
Another object of the present invention is to provide a convergence measuring method and a measuring device thereof, which can shorten measurement time and improve measurement efficiency.

〔発明の概要〕[Summary of the invention]

本発明は、上記目的を達成するために、被測定受像管に
先ず白色・母ターンを表示させてその表示パターンを各
発光色毎に撮像し、その各撮像信号から被測定受像管表
示面における各色発光パターンの位置情報をそれぞれ求
め、次に被測定受像管に測定用の・ヤターンを表示させ
てこの測定/4’ターンを撮像し、この測定パターンを
先に求めておいた各色発光パターンの位置情報に基づい
て各発光色の測定ノセターンを得、これらの各単色・ヤ
ターンの相対位置関係よυミスコンバーゼンス量を求め
るようにしたものである。
In order to achieve the above object, the present invention first displays a white color/main turn on a picture tube to be measured, images the display pattern for each emitted color, and uses the imaged signals to display a pattern on the display surface of the picture tube to be measured. The positional information of each color emission pattern is obtained, and then the measuring tube is displayed with a 4' turn for measurement, and this measurement/4' turn is imaged. The measured nosetan of each luminescent color is obtained based on the position information, and the amount of υ misconvergence is determined from the relative positional relationship of each of these monochromatic colors.

〔発明の実施例〕[Embodiments of the invention]

第1図は本発明の一実施例におけるコン・々−ゼンス測
定装置の概略構成図で、図中1は被測定受像管としての
3色カラー受像管(c−cRT )を示している。この
C−CRT 1は図示しない固定装置にセットされる。
FIG. 1 is a schematic diagram of a consense measuring device according to an embodiment of the present invention, and in the figure, numeral 1 indicates a three-color picture tube (c-cRT) as a picture tube to be measured. This C-CRT 1 is set in a fixing device (not shown).

この’C−CRT7の表示面1aには、工業用テレビジ
ョン(ITV )カメラ2が対向配置されておシ、この
ITVカメラ2と上記C−にRT 1との間には光学フ
ィルタ3が配置されている。この光学フィルタ3は、例
えば第2図に示す如く円板3aに青、赤、緑の色分離フ
ィルタ3b、3c。
An industrial television (ITV) camera 2 is placed facing the display surface 1a of this 'C-CRT 7, and an optical filter 3 is placed between this ITV camera 2 and the C-CRT 1. has been done. This optical filter 3 includes, for example, a circular plate 3a and blue, red, and green color separation filters 3b and 3c as shown in FIG.

3dと減光フィルタ3eとを相互に90°の間隔で配設
したもので、フィルタ切換機構4によシ切換わるように
なっている。このフィルタ切換機構4は、第2図に示す
ようにステップモータ4aを有し、このステップモータ
4aの動力全歯車機構4bを介して円板3aに伝達し、
これによシ円板3aを回転させて所望のフィルタを選択
するものとなっている。なお、このフィルタの選択制御
はフィルタ切換回路5によυなされる。
3d and a neutral density filter 3e are arranged at an interval of 90 degrees from each other, and are switched by a filter switching mechanism 4. The filter switching mechanism 4 has a step motor 4a as shown in FIG. 2, and the power of the step motor 4a is transmitted to the disk 3a via a full gear mechanism 4b.
Accordingly, the desired filter is selected by rotating the disc 3a. Note that this filter selection control is performed by the filter switching circuit 5.

ところで、前記ITVカメラ2の撮像信号は、A/D変
換回路とバッファメモリとからなる画像メモリ回路6に
導ひかれ、ここでディジタル画像情報として一時記憶さ
れたのち、演算制御回路7に導かれる。この演算制御回
路7は例えばマイクロプロセッサを中央処理部として有
するもので、メモリ8に記憶しである制御プログラムに
従って装置各部を動作制御するとともに、画像メモリ回
路6からの撮像情報を演算してコンバーゼンスを求める
。また演算制御回路7は、演算結果をメモリ8に記憶す
るとともに、データ出力装置9に表示あるいは記録させ
る。なお、10は上記演算制御回路7の指示に従って2
種類の画像パターン全発生するパターン発生器で、これ
らのパターンをテレビジョン電子回路1ノに一供給して
前記C−CRT 1に表示せしめる。
By the way, the imaging signal of the ITV camera 2 is led to an image memory circuit 6 consisting of an A/D conversion circuit and a buffer memory, where it is temporarily stored as digital image information, and then led to an arithmetic control circuit 7. The arithmetic control circuit 7 has, for example, a microprocessor as a central processing unit, and controls the operation of each part of the device according to a control program stored in the memory 8, and also calculates the imaging information from the image memory circuit 6 to achieve convergence. demand. Further, the arithmetic control circuit 7 stores the arithmetic results in the memory 8 and causes the data output device 9 to display or record the results. Note that 10 is 2 according to instructions from the arithmetic control circuit 7.
A pattern generator generates all kinds of image patterns and supplies these patterns to the television electronic circuit 1 for display on the C-CRT 1.

次に、上記構成に基づいて杢実施例の測定方法を説明す
る。先ず所定の位置にセットしたC−CRT 7に対し
、パターン発生器10から全面に白色パターン1ド♂報
を発生させてテレビジ璽ン電子回路11によりこれを表
示させる。そして、同時にフィルタ切換機構4によシ光
学フィルタ3を回転させて先ず前分離フィルタ3bをセ
ットし、この状態でITVカメラ2によシ上記C−CR
T1の表示i4’ターンの特定のエリアを撮像する。
Next, the measurement method of the heather embodiment will be explained based on the above configuration. First, with respect to the C-CRT 7 set at a predetermined position, a pattern generator 10 generates a white pattern 1 code signal over the entire surface, and the television electronic circuit 11 displays this. At the same time, the filter switching mechanism 4 rotates the optical filter 3 to first set the front separation filter 3b, and in this state, the ITV camera 2 is connected to the C-CR.
Display of T1: Image a specific area of the 4' turn.

そうすると、ITVカメラ2によシ撮像信号が得られ、
との撮像信号は画像メモリ回路6でA7D変換され、演
算制御回路2に導ひかれる。そして、この演算制御回路
7で、二値化情報に変換しく例えば第3図に示すVSの
″H″レベル部分の長さALから各螢光体の中心線XO
の位置を算出し、この中心filJ X Oを中心に隣
接する2個の螢光体の間隔の−に相当する長さXAf、
シラス方向およびマイナス方向に設定し、これによって
求めた領域情報BXn fメモリ8に記憶する。こうし
て、青の螢光体の領域情報BXnを算出すると、次に光
学フィルタ3の光分離フィルタ3cfセットし、上記前
分離フィルタ3bの場合と同様に撮像信号から赤の螢光
体の領域情報RXn f求め、メモリ8に記憶する。以
下同様に、klO色分離フィルタ3dfセットしてそれ
に対応する螢光体の領域情報GXn f求め、メモリ8
に記憶する。第4図(a) 、 (b) 、 (e)は
それぞれ上記前、赤、緑各色発光パターンの領域イ)〜
報を示すものである。なお、これらの領域情報の算出エ
リアの大きさは、X方向が最大コン・ぐ−センス範囲(
図中XL)に、またY方向が後述する電子ビームの照射
直径の大きさに対応する長さく図中ys)に定められる
Then, an image signal is obtained by the ITV camera 2,
The image pickup signal is A7D converted by the image memory circuit 6 and guided to the arithmetic control circuit 2. Then, this arithmetic control circuit 7 converts it into binary information, for example, from the length AL of the "H" level portion of VS shown in FIG. 3 to the center line XO of each phosphor.
The position of filJ
The area information BXn is set in the whitebait direction and the minus direction, and is stored in the BXn f memory 8. Once the area information BXn of the blue phosphor is calculated in this way, the light separation filter 3cf of the optical filter 3 is set, and the area information RXn of the red phosphor is obtained from the imaging signal as in the case of the pre-separation filter 3b. f is determined and stored in the memory 8. Similarly, the klO color separation filter 3df is set, the corresponding phosphor area information GXn f is obtained, and the memory 8
to be memorized. Figure 4 (a), (b), and (e) are the areas of the front, red, and green color light emitting patterns, respectively.
It shows the information. Note that the size of the calculation area for these area information is based on the maximum con- sense range in the X direction (
XL) in the figure, and the length in the Y direction is determined to be ys) in the figure, which corresponds to the irradiation diameter of the electron beam, which will be described later.

かくして、宣、赤2、緑の各螢光体における領域情報B
Xn 、 RXn 、 GXnの算出を終了と、次にツ
ヤターン発生器10から測定パターンとして例えば第5
図に示す如き白色ドツトパターン(図中DP)’に発生
させ、このノ々ターンi C−CRT 1に表示させる
。そして、光学フィルタ3ff:回転させて減光フィル
タ3efセツトし、この状態でITVカメラ2により上
記白色ドラトノやターンDPのうちの例えばひとつを含
む所定のエリアを撮像する。第6図は、その撮像エリア
を丞すもので、その太きさはX方向が前記領域情報の算
出時と同じ長さXLに、一方Y方向が最大コンバーゼン
ス範囲YLにそれぞれ設定される。
Thus, area information B for each of the red, red 2, and green phosphors
After completing the calculation of
A white dot pattern (DP in the figure) as shown in the figure is generated and displayed on the multi-turn iC-CRT 1. Then, the optical filter 3ff is rotated and the neutral density filter 3ef is set, and in this state, the ITV camera 2 images a predetermined area including, for example, one of the white dots and the turn DP. FIG. 6 shows the imaging area, and its thickness is set to the same length XL in the X direction as when calculating the area information, and to the maximum convergence range YL in the Y direction.

なお、図中■、@、θはそれぞれ青、赤、緑の電子ビー
ムの照射領域を示すもので、各領域中の青、赤、緑の螢
光体(図中斜線で示した螢光体)のみが発光する。
In the figure, ■, @, and θ indicate the irradiation areas of the blue, red, and green electron beams, respectively. ) only emit light.

との撮像信号は領域情報の算出時と同様に画像メモリ回
路6でA/D変換され、演算制御回路7に尋かれる。演
算制御回路7では、既にメモリ8に記憶されている前記
各領域情報に基づいて、各色の領域の中の前記A/D変
換4]]報だけを演算し、その画像中に含まれる発光螢
光体(第6図余1線部)の重心全算出し、これらの各重
心、例えば第6図BO、RO、Goのうち、緑の発光螢
光体の重心GOに対する青および亦の各発光螢光体の重
心BO、RO位置の離間距離BX。
The image signal is A/D converted by the image memory circuit 6 and sent to the arithmetic control circuit 7 in the same way as when calculating the area information. The arithmetic control circuit 7 calculates only the A/D conversion information in each color area based on the area information already stored in the memory 8, and calculates the luminescent light contained in the image. Calculate all the centroids of the light bodies (1 extra line in Fig. 6), and calculate each of these centroids, for example, among the centroids of BO, RO, and Go in Fig. 6, each of the blue and other luminescence with respect to the centroid GO of the green light-emitting phosphor. The separation distance BX between the center of gravity BO and RO position of the fluorescent body.

BYおよびRX 、RYをそれぞれ求め、これらの算出
結果をコンバーゼンス情報としてデータ出力装置9で記
録あるいは表示させる。
BY, RX, and RY are each calculated, and the results of these calculations are recorded or displayed on the data output device 9 as convergence information.

このような実施例の方法であれば、各色、′4y:の領
域情報BXn 、 RXn + GXn ft求めた後
は、測定パターンを各色毎に時分割で検出することなく
、同時に撮像してミスコンバーゼンス敷の演vJ−に行
なえるΩで、従来のような電源変動等による影響を受け
ずに、精度の良い測定結果を得ることができる。また、
電子ビームを各色毎に各別に発生するようにした場合に
比べて、短時間で測定できる利点がある。
With the method of this embodiment, after obtaining the region information BXn, RXn + GXn ft for each color, '4y:', the measurement pattern is not detected in a time-division manner for each color, but is imaged simultaneously to avoid misconvergence. With Ω that can be calculated on the basis of VJ-, highly accurate measurement results can be obtained without being affected by power supply fluctuations, etc., as in conventional methods. Also,
Compared to the case where electron beams are generated separately for each color, this method has the advantage that measurement can be performed in a shorter time.

なお、本発明は上記実施例に限定されるものではない。Note that the present invention is not limited to the above embodiments.

例えば、前記実施例でぼ三色の各分離フィルタを用いて
青、赤、緑の各螢光体の領域情報金それぞれ検出するよ
うにしたが、−色分の領域情報Ωみを得て、他の二色の
領域情報は上記検出した領域情報から予測することによ
り求めてもよい。このようにすれば、n1l)定の所要
時間をさらに短縮することができる。また、測定パター
ンとしては、ドツトパターンに限らず、クロメノ・ツチ
パターンを適用してもよい。
For example, in the above embodiment, three color separation filters were used to detect the area information of each of the blue, red, and green phosphors. Area information for the other two colors may be obtained by predicting from the detected area information. In this way, n1l) the required time can be further shortened. Furthermore, the measurement pattern is not limited to the dot pattern, but may also be a black-and-white pattern.

その他、撮像情報の信号処理方法や演算方法、装置各部
の構成についても、本発明の要旨を逸脱しない範囲で種
々変形して実施できる。
In addition, the signal processing method and calculation method of image pickup information, and the configuration of each part of the apparatus can be modified in various ways without departing from the gist of the present invention.

〔発明の効果〕〔Effect of the invention〕

以上詳述したように本発明によれば、予め各色発光・ぞ
ターンの位置情報を求めておき、しかるのち測定i+タ
ーンを撮像してこのパターンを上記位置情報と比較する
ことにより、測定パターン?告発光色毎に分離し、これ
らの分離した情報からコ/パーゼンスを求めるようにし
ているので、測定パターンを各発光色毎に各別に検出゛
することなく同時に検出することができ、これによシ時
間的変動袈累を除去してコンバーゼンス測定精度を高め
得、かつ測定時間を短縮して測定能率の向上をはかり得
るコンバーゼンス測定方法およびその測置装置?L−提
供することができる。
As described in detail above, according to the present invention, the positional information of each color light emission and each turn is obtained in advance, and then the measured i+turn is imaged and this pattern is compared with the above positional information to determine the measurement pattern. Since each light emitting color is separated and the co/parity is calculated from this separated information, the measurement pattern can be detected simultaneously without having to detect each emitted color separately. A convergence measurement method and measuring device that can improve convergence measurement accuracy by removing temporal fluctuations, shorten measurement time, and improve measurement efficiency? L-Can be provided.

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

第1図は本発明の一実施例におけるコンバーゼンス測定
装置の概略構成図、第2図は同装置の一部分の構成を示
す斜視図、第3図〜第6図はそれぞれ本発明の一実施例
におけるコン、パーゼンス測定方法を説明するだめのも
ので、第3図は撮像信号の処理方法を示す模式図、第4
図(a)〜(c)は各螢光体の領域情報金示す模式図、
第5図は測定パターンを示す模式図、第6図は測定・や
ターンの撮像結果を示す模式図である。 1・・・カラー受像管(、c−CR’r )、2・・・
ITVカメラ、3・・・光学フィルタ、4・・・フィル
タ切換機構、5・・・フィルタ切換回路、6・・・画像
メモリ回路、7・・・演算制御回路、8・・・メモリ、
9・・・データ出力装置、10・・りやターン発生器、
1ノ・・・テレビジョン電子回路。
FIG. 1 is a schematic configuration diagram of a convergence measuring device according to an embodiment of the present invention, FIG. 2 is a perspective view showing the configuration of a part of the same device, and FIGS. 3 to 6 are each according to an embodiment of the present invention. Figure 3 is a schematic diagram showing the imaging signal processing method;
Figures (a) to (c) are schematic diagrams showing area information of each phosphor;
FIG. 5 is a schematic diagram showing the measurement pattern, and FIG. 6 is a schematic diagram showing the measurement and turn imaging results. 1... Color picture tube (, c-CR'r), 2...
ITV camera, 3... Optical filter, 4... Filter switching mechanism, 5... Filter switching circuit, 6... Image memory circuit, 7... Arithmetic control circuit, 8... Memory,
9...Data output device, 10...Riya turn generator,
1. Television electronic circuit.

Claims (2)

【特許請求の範囲】[Claims] (1)被測定カラー受像管に白色パターンを表示させ、
この表示ツヤターンを各螢光色毎に撮像してその撮像信
号から上記被測定受像管の表示画面における各色発光パ
ターンの位置情報を各発光色毎に検出し、しかるのち前
記被測定受像管に特定の測定/4’ターンを表示させ、
4この測定ノeターンを撮像してその撮像信号を前記発
光ノ4ターンの検出位置情報に基づき各発光色毎の測定
ノ9ターンを求め、これらの測定ノリーンの相対位置関
係よシミスコンパーゼンス量を求めるようにしたことを
特徴とするコンバーゼンス測定方法。
(1) Display a white pattern on the color picture tube to be measured,
This display gloss turn is imaged for each fluorescent color, and position information of each color light emission pattern on the display screen of the picture tube to be measured is detected for each light emission color from the image signal, and then specified to the picture tube to be measured. Measure/display 4' turn,
4 This measurement turn is imaged and the imaging signal is used to obtain the measurement turn 9 for each emission color based on the detection position information of the light emission turn 4, and the relative positional relationship of these measurement turns is calculated based on the simis comparence. A convergence measurement method characterized by determining the amount.
(2)被測定カラー受像管に対し白色ノ9ターンおよび
コンバーゼンス測定用の特定の測定A?ターンを選択的
に表示せしめる手段と、前′配積測定受像管の表示画面
上の同一位置に表示された前記各/4’ターンを各発光
色別に撮像する撮像手段と、前記白色A?ターンを各発
光色毎に分離する色フイルタ部と、前記撮像手段によシ
各発光色毎に得られた撮像情報から前記被測定受像管の
表示画面における各色発光パターンの位置情報をそれぞ
れ検出するとともに前記撮像手段によシ得られた前記測
定パターン全上記各色発光ツヤターンの位置情報に基づ
き各発光色IIFの゛測定パターンを求めかつこれらの
も測定ツヤターンの相対位置からミスコンバーゼンス量
を求める演算手段とを具備したことを特徴とするコンバ
ーゼンス測定装置。
(2) Specific measurement A for white 9 turns and convergence measurement for the color picture tube to be measured? means for selectively displaying the turns; an imaging means for taking images of each of the 4' turns displayed at the same position on the display screen of the front 4' arrangement measuring picture tube for each emission color; a color filter unit that separates the turn for each emission color; and a color filter unit that detects positional information of each color emission pattern on the display screen of the picture tube to be measured from imaging information obtained for each emission color by the imaging means. and calculation means for calculating the measurement pattern of each luminescent color IIF based on the positional information of the luminescent gloss turns of all the above-mentioned colors obtained in the measurement pattern obtained by the imaging means, and also calculates the amount of misconvergence from the relative positions of the measured gloss turns. A convergence measuring device characterized by comprising:
JP18511182A 1982-10-21 1982-10-21 Method and device for measurement of convergence Pending JPS5974780A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18511182A JPS5974780A (en) 1982-10-21 1982-10-21 Method and device for measurement of convergence

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18511182A JPS5974780A (en) 1982-10-21 1982-10-21 Method and device for measurement of convergence

Publications (1)

Publication Number Publication Date
JPS5974780A true JPS5974780A (en) 1984-04-27

Family

ID=16165046

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18511182A Pending JPS5974780A (en) 1982-10-21 1982-10-21 Method and device for measurement of convergence

Country Status (1)

Country Link
JP (1) JPS5974780A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61154392A (en) * 1984-12-27 1986-07-14 Mitsubishi Electric Corp Image quality inspecting device of color image receiving tube
JPS62279797A (en) * 1986-05-29 1987-12-04 Hitachi Ltd Measuring instrument for mis-convergence quantity
JPS63116337A (en) * 1986-11-05 1988-05-20 Minolta Camera Co Ltd Convergence measuring method for color cathode-ray tube
JPH0199395A (en) * 1987-10-13 1989-04-18 Matsushita Electron Corp Mis-convergence measuring method for color picture tube
US5028849A (en) * 1987-10-14 1991-07-02 Minolta Camera Kabushiki Kaisha Device for measuring convergence of color cathode ray tube

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61154392A (en) * 1984-12-27 1986-07-14 Mitsubishi Electric Corp Image quality inspecting device of color image receiving tube
JPS62279797A (en) * 1986-05-29 1987-12-04 Hitachi Ltd Measuring instrument for mis-convergence quantity
JPS63116337A (en) * 1986-11-05 1988-05-20 Minolta Camera Co Ltd Convergence measuring method for color cathode-ray tube
JPH0199395A (en) * 1987-10-13 1989-04-18 Matsushita Electron Corp Mis-convergence measuring method for color picture tube
US5028849A (en) * 1987-10-14 1991-07-02 Minolta Camera Kabushiki Kaisha Device for measuring convergence of color cathode ray tube

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