JPS6053988B2 - Image tube actuator - Google Patents

Image tube actuator

Info

Publication number
JPS6053988B2
JPS6053988B2 JP55176440A JP17644080A JPS6053988B2 JP S6053988 B2 JPS6053988 B2 JP S6053988B2 JP 55176440 A JP55176440 A JP 55176440A JP 17644080 A JP17644080 A JP 17644080A JP S6053988 B2 JPS6053988 B2 JP S6053988B2
Authority
JP
Japan
Prior art keywords
image pickup
pickup tube
circuit
circuit system
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.)
Expired
Application number
JP55176440A
Other languages
Japanese (ja)
Other versions
JPS5799877A (en
Inventor
正弘 吉本
隆久 川島
徹 望月
多加志 末岡
孝 山下
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.)
Japan Broadcasting Corp
Panasonic Holdings Corp
Original Assignee
Nippon Hoso Kyokai NHK
Matsushita Electric Industrial Co 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 Nippon Hoso Kyokai NHK, Matsushita Electric Industrial Co Ltd filed Critical Nippon Hoso Kyokai NHK
Priority to JP55176440A priority Critical patent/JPS6053988B2/en
Publication of JPS5799877A publication Critical patent/JPS5799877A/en
Publication of JPS6053988B2 publication Critical patent/JPS6053988B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N23/00Cameras or camera modules comprising electronic image sensors; Control thereof
    • H04N23/40Circuit details for pick-up tubes
    • H04N23/41Beam current control

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)

Description

【発明の詳細な説明】 本発明は、撮像管への入射光量が被写体の変化により
過大となつても、当該電荷像を中和させ得るに足る大き
さのビーム電流が流れるように構成した撮像管作動装置
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides an imaging system configured to flow a beam current large enough to neutralize the charge image even if the amount of light incident on the image pickup tube becomes excessive due to a change in the subject. It relates to a tube actuator.

一般に、ビジコン等の光導電型撮像管を用いた撮像管
作動装置ては、撮像管の光電変換面を走査する電子ビー
ムのビーム量が過大となると解像度に低下をきたすので
、前記ビーム量を適当に制限することが行なわれている
Generally, in image pickup tube operating devices using photoconductive type image pickup tubes such as vidicon, if the amount of electron beam that scans the photoelectric conversion surface of the image pickup tube becomes excessive, the resolution will decrease, so the beam amount should be adjusted appropriately. is being restricted to.

しかし、ビーム量を一律に制限すると、被写体中の明る
い部分を撮像したとき、当該光電変換面部分に蓄積され
た電荷を一回の電子ビーム走査で完全に中和させ得なく
なり、いわゆる白つぷれ現象を生じ、明るい被写体部分
が動くことによつては、普星の尾に似た尾引き現象(コ
メツトテイル現象)がモニタ画面上に現われる。この解
決策として、撮像管のビーム制御電極電圧を信号電流の
大きさに応じて変化させ、明るい被写体部分を撮像した
ときに限りビーム電流を増加させる自動ビーム最適化回
路が堤案されている。
However, if the beam amount is uniformly limited, when a bright part of the subject is imaged, the charges accumulated on the photoelectric conversion surface cannot be completely neutralized with one electron beam scan, resulting in so-called whiteout. When this phenomenon occurs and the bright object part moves, a comet tail phenomenon similar to the tail of a common star appears on the monitor screen. As a solution to this problem, an automatic beam optimization circuit has been proposed that changes the beam control electrode voltage of the image pickup tube according to the magnitude of the signal current and increases the beam current only when a bright object part is imaged.

この回路は特公昭52−36648号公報に詳しくのべ
られているが、第1図に示すような負帰還回路からなる
。ここで、撮像管1の相互コンダクタンスを胛、カソー
ド電流をし、ビーム電流をI5、信号電流をし、戻りビ
ーム電流1R1ビーム電流制御電極電圧をECl、比較
増幅器2の増幅率をA、基準電源3からの基準電流をI
。、抵抗4の抵抗値をR、定数をαとすると、ビーム電
流1,および戻りビーム電流1Rは、でそれぞれ表わす
ことができる。
This circuit, which is described in detail in Japanese Patent Publication No. 52-36648, consists of a negative feedback circuit as shown in FIG. Here, set the mutual conductance of the image pickup tube 1, set the cathode current, set the beam current as I5, set the signal current, return beam current 1R1, set the beam current control electrode voltage as ECl, set the amplification factor of the comparator amplifier 2 as A, and set the reference power supply. The reference current from 3 is I
. , the resistance value of the resistor 4 is R, and the constant is α, the beam current 1 and the return beam current 1R can be respectively expressed as follows.

また であるから、これらの式から が成立する。Also Therefore, from these expressions holds true.

式(5)から明らかなように、信号電流Lと戻りビーム
電流hとは、第2図に直線aで示すような関係を有して
いる。
As is clear from equation (5), the signal current L and the return beam current h have a relationship as shown by the straight line a in FIG.

一方、信号電流Lは、撮像管1の、特性によつて決まる
有限値しMを有しているのて、α(A−R−Gmにして
かつ一]ピb鼾一の値力汁分小さくなるようA,Rのα
+A−R−Grn値を定めるならば、戻りビーム電流1
Rを信号電流Lの値に関係なく一定値1。
On the other hand, since the signal current L has a finite value M determined by the characteristics of the image pickup tube 1, α of A and R to become smaller
To determine the +A-R-Grn value, return beam current 1
R is a constant value 1 regardless of the value of signal current L.

に近づけることができ、つまり明るい部分を撮像して信
号電流Lが増大しても戻りビーム電流1Rがあまり減少
しないのでビーム電流hを増大させることができる。第
2図の直線bはその極限値を示す。ところで、前述のよ
うな負帰還回路による安定化動作は、従来の三極管構造
電子銃を有する撮像の作動においてのみ成立し、ダイオ
ードガンを有する撮像管にかかる回路を適用すると発振
現象が起り、実用に供し得なくなる。
In other words, even if a bright portion is imaged and the signal current L increases, the return beam current 1R does not decrease much, so the beam current h can be increased. Straight line b in FIG. 2 shows its limit value. By the way, the above-mentioned stabilizing operation by the negative feedback circuit can only be achieved in the operation of an imaging device with a conventional triode structure electron gun, and when the circuit is applied to an image pickup tube with a diode gun, an oscillation phenomenon occurs, making it impractical for practical use. It becomes impossible to provide.

なぜなら、従来の三極管構造電子銃では、式(1)に示
したようにカソード電流10がビーム電流hに比例する
のに対し、ダイオードガンではこの関係が成立せずにと
なり、また式(3)は となるからである。
This is because in a conventional triode structure electron gun, the cathode current 10 is proportional to the beam current h, as shown in equation (1), whereas in a diode gun, this relationship does not hold, and equation (3) This is because it becomes .

そして、式(2),(4),(6),(7)より戻りビ
ーム電流IRを求めるとただしG=]K.Kム4(〜4 (β+G。
Then, the return beam current IR is calculated from equations (2), (4), (6), and (7), where G=]K. Kmu4 (~4 (β+G.

・R−A)2となる。・R-A) becomes 2.

これを図で表わすと第3図に示すような二次曲線となり
、IRをしの値如何にかかわらず一定とすることは困難
となる。
If this is represented graphically, it becomes a quadratic curve as shown in FIG. 3, and it is difficult to keep the IR constant regardless of the value of .

なお、ダイオードガンは第4図のaに示すように構成さ
れ、同図のbに示す三極管構造の、電子銃と対比して、
電極構造が若干異なるほか、ビーム制御電極G1に正の
電位が与えられる点で異なり、電子ビームはクロスオー
バを形成しない(層流形)。
The diode gun is constructed as shown in FIG.
In addition to the slightly different electrode structure, the difference is that a positive potential is applied to the beam control electrode G1, and the electron beam does not form a crossover (laminar flow type).

本発明の撮像管作動装置における撮像管は、タイオード
ガンを有し、たとえば第5図に示すような帰還回路によ
つてビーム制御を受ける。
The image pickup tube in the image pickup tube operating device of the present invention has a diode gun and receives beam control by, for example, a feedback circuit as shown in FIG.

第5図に示す回路構成が第1図に示した回路構成と異な
る点は、分流器5からとり出したカソード電流を二乗回
路6に与え、二乗回路6の出力信号を演算回路7に与え
ていることと、比較増幅器8の出力信号を平方根回路9
に与え、平方根回路9の出力信号を光導電型撮像管10
のビーム制御電極G1に与えていることの2点であり、
撮像管10はダイオードガンを有している。このような
構成においては つので、式式(2),(4),(6),(9)からの関
係式が成立する。
The circuit configuration shown in FIG. 5 differs from the circuit configuration shown in FIG. and the output signal of the comparator amplifier 8 is connected to the square root circuit 9.
and output the output signal of the square root circuit 9 to the photoconductive image pickup tube 10.
There are two points given to the beam control electrode G1 of
The image pickup tube 10 has a diode gun. In such a configuration, the relational expressions from equations (2), (4), (6), and (9) hold true.

またここでβ<A(G..・R)2が成立し、信号電流
Lは撮像管10の特性で決まるある有限の値しMをもつ
ので、ーー護?−ー力汁分小さくなるようにA−Rのβ
+A(?・R)2値を定めるなら、戻りビーム電流1R
を一定値1。
Also, here β<A(G...R)2 holds true, and the signal current L has a certain finite value M determined by the characteristics of the image pickup tube 10, so... - - β of A-R so that the power juice is smaller
+A (?・R) If you define the binary value, return beam current 1R
is a constant value of 1.

に近づけることができる。なお、二乗回路6および平方
根回路9は、たとえば第6図および第7図にそれぞれ示
すように、広帯域乗算器用集積回路MCl595L(米
国モトローラ社製)11を用いて構成することできる。
12は差動増幅器を示す。
can be approached. Note that the square circuit 6 and the square root circuit 9 can be constructed using a wideband multiplier integrated circuit MCl595L (manufactured by Motorola, USA) 11, as shown in FIGS. 6 and 7, respectively, for example.
12 indicates a differential amplifier.

本発明の第2の実施例を第8図に示す。同図に示す回路
構成では、ダイオードガンを有する光導電型撮像管10
のターゲット電極と演算増幅器7との間に信号補正回路
11を設けており、その他の回路構成は第1図に示した
回路構成と変りがない。信号補正回路11は第9図に示
すような入力信号し一出力信号し″特性を有し1S−7
11S@ υ1X′U′IV暴)VV−ーρで表わされ
る二本折線からなる。
A second embodiment of the invention is shown in FIG. In the circuit configuration shown in the figure, a photoconductive image pickup tube 10 having a diode gun is used.
A signal correction circuit 11 is provided between the target electrode and the operational amplifier 7, and the other circuit configuration is the same as that shown in FIG. The signal correction circuit 11 has an input signal and an output signal characteristic as shown in FIG.
11S@ υ1X'U'IV) Consists of a two-fold line represented by VV--ρ.

ただしここでγ。,γ,はそれぞれの領域における仝V
であ ΔI,る。
However, here γ. , γ, is the V in each region
And ΔI,ru.

この場合 が成立し、しがO〜し,においては、式(2),(4)
,(6),(11),(13)により、戻りビーム電流
1Rはとなる。
This case holds, and if O~, then Equations (2) and (4)
, (6), (11), and (13), the return beam current 1R becomes.

また、hがし〉Islにおいては、式(2),(4),
(6),(12),(13)により、戻りビーム電流h
は式(14),(15)の特性は、第10図に実線曲線
A,bで示すような2つの放物線として表わされる。
In addition, in h > Isl, formulas (2), (4),
By (6), (12), and (13), the return beam current h
The characteristics of equations (14) and (15) are expressed as two parabolas as shown by solid curves A and b in FIG.

同図の破線曲線cは、信号補正回路11を設けないとき
の特性で、このような特性であれば発振現象を起す。本
発明の装置では、し,とγ1とを適切な値に選ぶことに
よつて実線曲線A,bで示す戻りビーム特性を得ること
ができるので、非常に大きい信号電流しが流れてもきわ
めて安定に所期のビーム制御効果を得ることができる。
The broken line curve c in the figure shows the characteristic when the signal correction circuit 11 is not provided, and such a characteristic causes an oscillation phenomenon. In the device of the present invention, the return beam characteristics shown by the solid curves A and b can be obtained by selecting appropriate values for γ1 and γ1, so it is extremely stable even when a very large signal current flows. The desired beam control effect can be obtained.

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

第1図は従来の自動ビーム最適化回路のブロック図、第
2図は同回路に三極管構造電子銃を有する撮像管を用い
た場合の撮像管信号電流と戻りビーム電流との関関係を
示すし−1R特性図、第3図は同回路にダイオードガン
を有する撮像管を用,いた場合のし−1R特性図、第4
図のaはダイオードガンの電極構成図、同図のbは三極
管構造電子銃の電極構成図、第5図は本発明の一実施例
の回路構成を示すブロック図、第6図は二乗回路のブロ
ック図、第7図は平方根回路のブロック図、)第8図は
本発明の他の実施例の回路構成を示すブロック図、第9
図は第8図の回路構成における信号補正回路の入力信号
と出力信号との関係を示すし−1s″特性図、第10図
は同回路構成におけるL−h特性図である。 S5・・・・・・分流器、6・・・・・・二乗回路、7
・・・・・・演算増幅器、8・・・・・・比較増幅器、
9・・・・・・平方根回路、10・・・・・・撮像管、
11・・・・・・信号補正回路、12・・クランプ回路
、13・・・・・・変換係数補正回路、15・・・・・
加算回路。
Figure 1 is a block diagram of a conventional automatic beam optimization circuit, and Figure 2 shows the relationship between the image pickup tube signal current and the return beam current when the circuit uses an image pickup tube with a triode structure electron gun. -1R characteristic diagram, Figure 3 is a -1R characteristic diagram when an image pickup tube with a diode gun is used in the same circuit, Figure 4.
Figure a is a diagram of the electrode configuration of a diode gun, b of the figure is a diagram of the electrode configuration of a triode structure electron gun, Figure 5 is a block diagram showing the circuit configuration of an embodiment of the present invention, and Figure 6 is a square circuit diagram. Figure 7 is a block diagram of the square root circuit; Figure 8 is a block diagram showing the circuit configuration of another embodiment of the present invention;
The figure shows the relationship between the input signal and the output signal of the signal correction circuit in the circuit configuration of FIG. 8, and FIG. 10 is an L-h characteristic diagram in the same circuit configuration. ...Shunt, 6... Square circuit, 7
...Operation amplifier, 8...Comparison amplifier,
9...Square root circuit, 10...Image tube,
11... Signal correction circuit, 12... Clamp circuit, 13... Conversion coefficient correction circuit, 15...
addition circuit.

Claims (1)

【特許請求の範囲】 1 光導電型撮像管の出力信号を帰還用信号処理回路系
に導き、同回路系の出力信号を前記撮像管のビーム制御
電極に与えてビーム電流を制御せしめる撮像管作動装置
であつて、前記信号処理回路系が前記撮像管のターゲッ
ト電極から演算増幅器および比較増幅器を通じて前記ビ
ーム制御電極にいたる第1の回路系と、前記撮像管のカ
ソード回路の分流器から前記演算増幅器にいたる第2の
回路系とからなるものにおいて、前記記撮像管はダイオ
ードガンを有し、前記信号処理回路系はダイオードガン
を有する撮像管の非直線的なビーム電流対カソード電流
特性を、三極管構造を有する撮像管の直線的な同特性に
近似させるための補正回路を含んでいることを特徴とす
る撮像管作動装置。 2 前記補正回路は前記第1の回路系に含ませた平方根
回路と前記第2の回路系に含ませた二乗回路とからなる
ことを特徴とする特許請求の範囲第1項記載の撮像管作
動装置。 3 前記補正回路は前記第1の回路系に含まれ、折線か
らなる信号変換特性を有していることを特徴とする特許
請求の範囲第1項記載の撮像管作動装置。
[Scope of Claims] 1. Image pickup tube operation in which the output signal of the photoconductive type image pickup tube is guided to a feedback signal processing circuit system, and the output signal of the circuit system is applied to the beam control electrode of the image pickup tube to control the beam current. In the apparatus, the signal processing circuit system includes a first circuit system extending from a target electrode of the image pickup tube through an operational amplifier and a comparison amplifier to the beam control electrode, and a shunt of a cathode circuit of the image pickup tube to the operational amplifier. the image pickup tube has a diode gun, and the signal processing circuit system converts the non-linear beam current versus cathode current characteristic of the image pickup tube having the diode gun into 1. An image pickup tube operating device comprising a correction circuit for approximating linear characteristics of an image pickup tube having a structure. 2. The image pickup tube operation according to claim 1, wherein the correction circuit comprises a square root circuit included in the first circuit system and a square root circuit included in the second circuit system. Device. 3. The image pickup tube operating device according to claim 1, wherein the correction circuit is included in the first circuit system and has a signal conversion characteristic consisting of a broken line.
JP55176440A 1980-12-12 1980-12-12 Image tube actuator Expired JPS6053988B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55176440A JPS6053988B2 (en) 1980-12-12 1980-12-12 Image tube actuator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55176440A JPS6053988B2 (en) 1980-12-12 1980-12-12 Image tube actuator

Publications (2)

Publication Number Publication Date
JPS5799877A JPS5799877A (en) 1982-06-21
JPS6053988B2 true JPS6053988B2 (en) 1985-11-28

Family

ID=16013736

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55176440A Expired JPS6053988B2 (en) 1980-12-12 1980-12-12 Image tube actuator

Country Status (1)

Country Link
JP (1) JPS6053988B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6171774A (en) * 1984-09-14 1986-04-12 Sony Corp Beam current controller of television camera device

Also Published As

Publication number Publication date
JPS5799877A (en) 1982-06-21

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