JPS6045228A - Detecting device of information on object to be photographed - Google Patents

Detecting device of information on object to be photographed

Info

Publication number
JPS6045228A
JPS6045228A JP58153680A JP15368083A JPS6045228A JP S6045228 A JPS6045228 A JP S6045228A JP 58153680 A JP58153680 A JP 58153680A JP 15368083 A JP15368083 A JP 15368083A JP S6045228 A JPS6045228 A JP S6045228A
Authority
JP
Japan
Prior art keywords
circuit
photographed
amplitude
high luminance
aperture
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
JP58153680A
Other languages
Japanese (ja)
Inventor
Tadashi Okino
沖野 正
Shinji Sakai
堺 信二
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP58153680A priority Critical patent/JPS6045228A/en
Publication of JPS6045228A publication Critical patent/JPS6045228A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B7/00Control of exposure by setting shutters, diaphragms or filters, separately or conjointly
    • G03B7/28Circuitry to measure or to take account of the object contrast

Abstract

PURPOSE:To eliminate an influence of an object to be photographed of high luminance, which is entered into a part of a picture, by providing an amplitude compressing circuit which inputs a photoelectric converting output and has a characteristic set in advance. CONSTITUTION:A luminance of each part of a picture of light of an object to be photographed, which has passed through a diaphragm 2 is brought to photometry 3a-3d, each photometric value is brought to amplitude compression 4a-4d and added, and basing on this added value, the diaphragm is servo-controlled. In case when a part of a picture is in high luminance, when each photoelectric converting output is added as it is, it is feared that a main object to be photographed becomes underexposure by being influenced by a high luminance part, but photographing within an allowable exposure range can be executed by setting a characteristic of the amplitude compressing circuit so as to intensify a degree of compression at the time of high luminance.

Description

【発明の詳細な説明】 〔技術分野〕 本発明は複数の光電変換手段を有し、撮影画面を空間的
に分割して測光する小によって被写体情報を検出する被
写体情報検出装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to a subject information detection device that has a plurality of photoelectric conversion means and detects subject information by spatially dividing a photographic screen and measuring light.

〔従来技術〕[Prior art]

従来この種の装置においては、被写体中の目的とする物
の露出を正確に制御するため様々な重みづけがなされて
きた。しかしながら重み付けの為に空間分割された各画
面の中や主要被写体の他にさらに小さな暗点や輝点含有
する場合の露出精度に難点があった。即ち空間分割され
た各要素の絵の中や、主要被写体の中に空間的にごく一
部だけ明るさが平均値から著しくかけはなれているもの
があった場合でも正確な測光データを得るのは極めで困
難であった。
Conventionally, in this type of apparatus, various weights have been applied in order to accurately control the exposure of a target object in a subject. However, there was a problem with exposure accuracy when each screen was spatially divided for weighting or when there were smaller dark spots or bright spots in addition to the main subject. In other words, it is difficult to obtain accurate photometric data even if there is a small part of the spatially divided picture of each element or the main subject whose brightness deviates significantly from the average value. It was extremely difficult.

例えば平均値からのずれが大きい場合低輝度よりも高輝
度の影響の方が大きい。具体的な数値をであった場合そ
の被写体の輝度は平均と比べてすなわち 21°g20.901 ’−2−0.”’ (−0,1
5EV)・・・・・・・・・■たけ低いものと判断され
、これだけの誤差が発生する。
For example, when the deviation from the average value is large, the effect of high brightness is greater than that of low brightness. If a specific value is given, the brightness of the subject is compared to the average, i.e. 21°g20.901'-2-0. ”' (-0,1
5EV)・・・・・・・・・■It is judged that it is extremely low, and this much error occurs.

一方コ丁の面積の輝度が平均輝度の100倍であっすな
わち 210g210゛9−23°45(+3.45EV) 
(4)たけ高いものと判断され、これだ+−1の誤差が
発生する。
On the other hand, the brightness of the area of the corner is 100 times the average brightness, i.e. 210g210゛9-23°45 (+3.45EV)
(4) It is judged to be very high, and an error of +-1 will occur.

(2)式と(4)弐企見比べてみれば明らかなように微
小な暗点または輝点があった場合輝点による誤差の方が
はるかに大きい。
Comparing Equation (2) and (4), it is clear that when there is a minute dark or bright spot, the error caused by the bright spot is much larger.

このように画面の一部に高輝度被写体が入り込むと露出
データは大巾に狂ってしまう。このような欠点は画面の
各部の信号に重みづけをしたとしても充分には除去でき
ないものであった。
If a high-brightness subject enters a part of the screen in this way, the exposure data will be drastically distorted. Such drawbacks could not be sufficiently removed even if the signals of each part of the screen were weighted.

〔目的〕〔the purpose〕

本発明の目的は画面の一部に入り込んだ高輝度部分によ
る影響を大rjjに除失しイUる被写体情報検出袋y+
Uを提供する事にある。
The object of the present invention is to provide a subject information detection bag that can largely eliminate the influence of high-brightness areas that have entered a part of the screen.
The goal is to provide U.

〔実施例〕〔Example〕

以下添付した図面を参照しながら本発明について詳しく
説明する。第1図中加算図(j本発明の第1実施例を示
す図である。
The present invention will be described in detail below with reference to the attached drawings. Addition diagram in FIG. 1 (j is a diagram showing the first embodiment of the present invention.

第1図は本発明の第1実施例の電気系ブロック図であり
、1は測光光学系2は絞りであり、1,2は測光系と 
撮影系とで共用してもよいし、それぞれ別にもっていて
もよい。a、b、c、dは光電変換手段としての受光素
子であり、例えは第2図の如く被写体像を空間分割する
。ろa、 3b、ろC9ろdは光電変換回路、4a、4
b、4c、4dは振巾圧縮手段としての振幅圧縮回路、
5は混合手段としての加算回路、10は誤差増幅および
絞り駆動コイルの駆動のための電流を供給する増幅器で
ある。
FIG. 1 is an electrical system block diagram of the first embodiment of the present invention, where 1 is a photometric optical system 2 is an aperture, and 1 and 2 are photometric systems.
It may be shared with the imaging system, or may be kept separately. A, b, c, and d are light receiving elements as photoelectric conversion means, which spatially divide the subject image as shown in FIG. 2, for example. Ro a, 3b, Ro C9 rod d is photoelectric conversion circuit, 4a, 4
b, 4c, and 4d are amplitude compression circuits as amplitude compression means;
5 is an adder circuit as a mixing means, and 10 is an amplifier that supplies current for error amplification and driving the aperture drive coil.

11は絞り駆動コイルであり端子11aに正電圧が印加
されたとき絞り2を閉じ、負電圧が印加されたとき絞り
2を開く様Bη成されている。
Reference numeral 11 denotes an aperture drive coil, which is configured to close the aperture 2 when a positive voltage is applied to the terminal 11a and open the aperture 2 when a negative voltage is applied.

ここで光電変換回路3a、3b、3c、3dは例えば第
6図の如き構成となっており、この回路において受光素
子102の電流すなわち増幅器101の出力電圧は入射
光量に比例している。また振幅圧縮回路4 a + 4
b+ 4 ’ + 4dは例えば第4図又は第5図の如
き回路構成となっている。
Here, the photoelectric conversion circuits 3a, 3b, 3c, and 3d have a configuration as shown in FIG. 6, for example, and in this circuit, the current of the light receiving element 102, that is, the output voltage of the amplifier 101 is proportional to the amount of incident light. Also, amplitude compression circuit 4 a + 4
b+4'+4d has a circuit configuration as shown in FIG. 4 or FIG. 5, for example.

!( まず第4図について説明すると201 、202は抵抗
であり、203はトランジスタ、204は基準電圧発生
回路である。基準電圧発生回路204の発生する基環X
電圧を■2o4とすると入力電圧V1がV2o4よりも
低い場合トランジスタ203のベース・エミッタは逆バ
イアスされてトランジスタ203はカットオフし、トラ
ンジスタ206には電流が流れず出力電圧■。は入力電
圧に等しくなる。
! (First of all, referring to FIG. 4, 201 and 202 are resistors, 203 is a transistor, and 204 is a reference voltage generation circuit.
Assuming that the voltage is ■2o4, when the input voltage V1 is lower than V2o4, the base and emitter of the transistor 203 are reverse biased, the transistor 203 is cut off, no current flows through the transistor 206, and the output voltage becomes ■. is equal to the input voltage.

■−V・ (5) l 一方入力電圧V、が■2o4よりも十分高くなるとンジ
スタ203に従って抵抗202に電流が流れる。
■-V・ (5) l On the other hand, when the input voltage V is sufficiently higher than ■2o4, a current flows through the resistor 202 according to the resistor 203.

トランジスタ20ろのベース・エミッタ間電圧を無視し
、抵抗201 、202の抵抗値をR2o□、R2o2
とすると出力電圧■。と入力電圧■iの関係はとなる。
Ignoring the base-emitter voltage of transistor 20, the resistance values of resistors 201 and 202 are R2o□, R2o2
Then, the output voltage is ■. The relationship between and input voltage ■i is as follows.

これを図示したのが第5図である。即ぢ例えばR201
” ”202 = 9 ” 1とすると’201”’2
02 ソ十1 ’ILJとなって微分利得aは■i>V
2o4において■1〈■2o4の1/10に圧縮される
。 8 次に第6図について説明する。301は抵抗、302は
ダイオード、603は基準電圧発生回路である。
FIG. 5 illustrates this. For example, R201
” ”202 = 9 ” If 1, then '201''2
02 So11 'ILJ and the differential gain a is ■i>V
In 2o4, ■1 <■ is compressed to 1/10 of 2o4. 8 Next, FIG. 6 will be explained. 301 is a resistor, 302 is a diode, and 603 is a reference voltage generation circuit.

基準電圧発生回路606の発生する基準電圧を■3o3
とすると入力電圧Viが■3o3よりも低い場合ダイオ
ード602はカットオフして■3o3と■iけ遮断され
るから入出力電圧は埼しい。
The reference voltage generated by the reference voltage generation circuit 606 is
Then, when the input voltage Vi is lower than 3o3, the diode 602 is cut off and 3o3 and 2i are cut off, so the input/output voltage is high.

■・=V (8) ! 〇 一方入力電圧Viが■3o3よりも高くなった場合ダイ
オード602がオンし、ダイオード302のj111方
向電圧降下を無視すると出力11j、圧■。は■3o3
に等しくなる。
■・=V (8)! 〇On the other hand, when the input voltage Vi becomes higher than ■3o3, the diode 602 turns on, and if the voltage drop in the j111 direction of the diode 302 is ignored, the output 11j becomes voltage ■. is■3o3
is equal to

V−V (9) 0 303 これを図示したのが第7図である。V-V (9) 0 303 FIG. 7 illustrates this.

第1図中加算回路5は第8図の如き回路で1Mj成され
る。図中401〜405は抵抗、406は演算増幅器で
ある。このように第1り成した場合入出力トテ性は Vo−−(Via+V、b+V、o+Vid) (10
)となる。
The adder circuit 5 in FIG. 1 is composed of 1Mj of circuits as shown in FIG. In the figure, 401 to 405 are resistors, and 406 is an operational amplifier. In this way, the input/output characteristics are Vo−−(Via+V, b+V, o+Vid) (10
).

ただし抵抗401〜405の値は全て等しく抵抗201
 、202 、301の抵抗値よりも十分高いものとす
る。
However, the values of resistors 401 to 405 are all equal to resistor 201.
, 202, and 301.

本発明の第1実施例は上述の如き構成をとるものであり
以下にその動作について説明する。撮影光学系1および
絞り2を介して被写体像が受光素子al b、 c、 
d上に結像される。それを光電変換回路3a、3b、3
c、3dにより各部の輝度に比例した電圧に変換し、振
幅圧縮回路4a、 4b、 4c、 4dにより振幅圧
縮した信号を加算回路5で加齢し、誤差増幅器10によ
って誤差を増幅するとともに絞り2を駆動する事により
受光素子a、 b、 c、 dの入射光を一定にする。
The first embodiment of the present invention has the configuration as described above, and its operation will be explained below. The subject image passes through the photographic optical system 1 and the aperture 2 to the light receiving elements al b, c,
The image is formed on d. The photoelectric conversion circuits 3a, 3b, 3
The signal is converted into a voltage proportional to the brightness of each part by c and 3d, and the amplitude is compressed by amplitude compression circuits 4a, 4b, 4c and 4d. By driving the light receiving elements a, b, c, and d, the incident light is made constant.

これを説明する為に話を簡単にする意味で被写体が均一
輝度面すなわち受光素子a、 b、 c、 dに入射す
る光が等しいものとする。
To simplify the explanation, it is assumed that the subject has a uniform brightness surface, that is, the light incident on the light receiving elements a, b, c, and d is equal.

まず各受光素子に入射する光の強度が高すぎる場合、光
電変換回路3a、3b、3c、3d従って振幅圧縮回路
4a、4b、4c、4dの出力が平衡値よりも高くなり
それらの反転加算値である加算回路5の出力は基準電圧
発生回路90基準電圧よりも低くなる。従って誤差増幅
器10の出力は正となり絞り駆動コイル11の端子11
aが正に駆動されるから絞り2は閉じて、受光素子a、
 b、 c、 dに入射する光をより少なくする。
First, if the intensity of light incident on each light receiving element is too high, the outputs of the photoelectric conversion circuits 3a, 3b, 3c, 3d and therefore the amplitude compression circuits 4a, 4b, 4c, 4d will be higher than the equilibrium value, and their inverted sum value The output of the adder circuit 5 becomes lower than the reference voltage of the reference voltage generating circuit 90. Therefore, the output of the error amplifier 10 is positive, and the terminal 11 of the aperture drive coil 11
Since a is driven positively, the aperture 2 is closed and the light receiving elements a,
Reduce the amount of light incident on b, c, and d.

逆に受光素子a、 b、 c、 dに入射する光の強度
が低すぎる場合加算回路5の出力は基準電圧発生回路9
の基準電圧よりも高くなる。従って誤差増幅器10の出
力は負になり絞り駆動コイル11の端子11aが負に駆
動されるから絞り2は開いて受光素子al b、 c、
 dに入射する光をより多くする。かくしで基準値より
も入射光量が高い場合も低い場合も絞り2の駆動により
常に基準値に戻そうとする働きがあり、10の利得が十
分高ければ加′J3器5の出力電圧が一定値(基準電圧
発生回路9のグ6生する基準電圧に等しい値)になるよ
うな制御がなされる。すなわち均−河1度被写体に対し
ては振幅圧縮回路4 a+ 4 b + 4 c + 
4 dの特性によらず常に、 1゜ 適切な露光制御がなされる。 1・ 次に受光素子a、 b、 c、 dのうちの1つaの部
分に入射する光強度が他Gこ対して10倍強かった場合
について考える。まず振幅圧縮回路4a、 4b。
Conversely, if the intensity of the light incident on the light receiving elements a, b, c, and d is too low, the output of the adder circuit 5 is applied to the reference voltage generating circuit 9.
higher than the reference voltage. Therefore, the output of the error amplifier 10 becomes negative and the terminal 11a of the aperture drive coil 11 is driven negatively, so the aperture 2 is opened and the light receiving elements al b, c,
Increase the amount of light incident on d. Hiddenly, whether the amount of incident light is higher or lower than the reference value, there is a function that always tries to return it to the reference value by driving the aperture 2, and if the gain of 10 is high enough, the output voltage of the adder 5 remains at a constant value. (a value equal to the reference voltage generated by the reference voltage generating circuit 9). In other words, for a 1-degree subject, the amplitude compression circuit 4 a + 4 b + 4 c +
4 Appropriate exposure control is always performed by 1° regardless of the characteristics of d. 1. Next, consider a case where the intensity of light incident on one of the light receiving elements a, b, c, and d, a, is 10 times stronger than the other G elements. First, amplitude compression circuits 4a and 4b.

4c、4dが熱い場合全体としての明るさは均一な場合
に比べて 3 1 l3 −X1+HX10−’T倍 だと感じるため絞り2の開口面積を均一被写体の場合に
比較して■として加算回路5の出力が一定となるように
制御してしまう。この場合もしもす。
When 4c and 4d are hot, the overall brightness is felt to be 3 1 l3 - control so that the output is constant. In this case, maybe.

c、dが主要な被写体(例えば人物等)であり、aが背
景の輝点(空、照明装置等)であった場合主要な被写体
には望ましい値の(邪心)の60%しか露光量がなく撮
影は失敗となる。
If c and d are the main subjects (for example, a person), and a is a bright spot in the background (the sky, a lighting device, etc.), the exposure amount for the main subject is only 60% of the desired value (evil mind). Otherwise, the shooting will fail.

一方同一の被写体条件に対して振幅圧縮回路4a。On the other hand, the amplitude compression circuit 4a for the same subject condition.

4b、4c、4dの特性を第5図の如く設定し、■20
4を均一輝度被写体の平衡出力でありR2o1とR20
2の比をの式の如く設定すると受光素子aに入射する光
の強さは 1 9 19 r (1+IT) in であるとみなされ、受光素子a、 b、 c、 d全部
に入射する光は 被写体の場合に比較して皿として加算回路5の9 出力が一定となるように制御してしまう。この場合主要
な被写体す、 c、 dの露光量は望ましい値の0 (−2iV二)82%あり、撮影は失敗とならない。
Set the characteristics of 4b, 4c, and 4d as shown in Figure 5, and
4 is the balanced output of a subject with uniform brightness, and R2o1 and R20
When the ratio of Compared to the case of a subject, the output of the adding circuit 5 is controlled to be constant as a plate. In this case, the exposure amount of the main subjects A, C, and D is 0 (-2 iV2) 82% of the desired value, and the photographing is not a failure.

もしも主要被写体との輝度差がさらに大きい場合第9図
の如く段階的に圧縮の度合を強めたり、さらには第10
図の如くあるレベル以上は出力をクリップする事により
高輝度の輝点の影響を除去できる。第9図および第10
図の入出力特性は第4図および第5図の回路を組み合わ
せて容易に実現できる。
If the brightness difference with the main subject is even larger, the degree of compression will be increased step by step as shown in Figure 9, or even the 10th
As shown in the figure, the influence of high-intensity bright spots can be removed by clipping the output above a certain level. Figures 9 and 10
The input/output characteristics shown in the figure can be easily realized by combining the circuits shown in FIGS. 4 and 5.

また、上の例では話を簡単にするために4つの受ツC素
不の場合の例で説明したが実際には分割をさらに多くし
たり、その中に重みづけをしたりする事も容易にできる
。特に重みづけをしたい揚りは第8図に示した加算回路
の入力抵抗401〜404の各々の値を変えればよい。
Also, in the above example, to simplify the discussion, we explained the case of 4 Utsu C base, but in reality, it would be easy to increase the number of divisions or add weights to them. Can be done. In particular, if weighting is desired, the values of the input resistors 401 to 404 of the adder circuit shown in FIG. 8 may be changed.

第11図は本発明の第2の実施例を示す図でありCCD
や撮像管等の撮像デバイスを利用したムービ又はスチル
カメラに適用したものである。このようなカメラにおい
て撮像デバイスそのものが被写体を細かく空間分割して
測光する複数の受光素子の集合体とみなせるのでより精
密な測光が可能となる。
FIG. 11 is a diagram showing a second embodiment of the present invention.
This is applied to movie or still cameras that use imaging devices such as cameras and image pickup tubes. In such a camera, the imaging device itself can be regarded as an assembly of a plurality of light-receiving elements that spatially divide the subject into finely divided areas and measure the light, thereby enabling more precise light measurement.

図において501は光学系、502は絞り、 50ろは
光電変換手段としてのCOD等の撮像デバイス、504
はCCDの光電変換出力を処理して輝度成分を抽出する
信号処理回路である。505は振幅圧縮手段としての振
幅圧縮回路であり第4図の構成又は第6図の構成或いは
その組合せの回路構成から成る。506は混合手段とし
ての積分回路であり全画面に対する時系列的な輝度(振
幅圧縮後の)信号の時間的加算混合出力としての積分値
をめる回路であり最もfftj単には第12図の如く抵
抗601、キャパシタ602の直列回路によって構成で
きる。507は誤差増1iIiIi器および紋り駆動回
路であり例えば第1図の10と全く同じ構成で実現でき
る。50Bは絞り駆動コイルでありこれの駆動により絞
り502の口径か変化する。
In the figure, 501 is an optical system, 502 is an aperture, 50 is an imaging device such as COD as a photoelectric conversion means, 504
is a signal processing circuit that processes the photoelectric conversion output of the CCD and extracts the luminance component. Reference numeral 505 denotes an amplitude compression circuit as an amplitude compression means, which has the configuration shown in FIG. 4, the configuration shown in FIG. 6, or a combination thereof. Reference numeral 506 is an integrating circuit as a mixing means, which calculates an integral value as a time-added mixed output of time-series luminance (after amplitude compression) signals for the entire screen, and most fftj is simply as shown in FIG. It can be configured by a series circuit of a resistor 601 and a capacitor 602. Reference numeral 507 denotes an error multiplier 1iIiIi and a frizz driving circuit, which can be realized, for example, with exactly the same configuration as 10 in FIG. Reference numeral 50B is an aperture drive coil, and the aperture of the aperture 502 is changed by driving this coil.

第11図の第2実施例は上述の如き構成より成る。第1
図と第11LAを比べると ダ3 1 図 第 11 図 光学系1←−→光学系501 絞 リ 2 くミーーーーー〜−−−−ら〉 絞 リ 
502受光素子a、b、c、d(’−ラ撮像素子503
誤差増幅器10(−÷誤差増幅器 507絞り駆動コイ
ル 11%絞り駆fJ11コイル 51、〕8とが対応
するので第11図は第1図と同様に動作し被写体の輝点
の悪影響を除去できる。但し第1図において5の加算回
路は反転特性を有し、第11図における積分回路506
は反転qモ性を有しないので絞り駆動コイル508の端
子5osaが負電圧で駆動された場合絞り502を閉じ
、正電圧で駆動され、、4□、5o2□8.よう6oイ
、1.¥ 、Bオゎ7いお。 ・Jl、・〔効 果〕 以上説明した小から明らかなように、本発明によれば簡
単な振幅圧縮回路を追加する事により被写体空間内の輝
点の影響を除失し、被写体情報の精度を大幅に向上でき
る。
The second embodiment shown in FIG. 11 has the configuration described above. 1st
Comparing the figure and No. 11 LA, 3 1 Figure 11 Optical system 1←-→Optical system 501 Aperture 2
502 light receiving elements a, b, c, d ('-ra image sensor 503
Since the error amplifier 10 (-÷error amplifier 507 aperture drive coil 11% aperture drive fJ11 coil 51, )8 corresponds to each other, FIG. 11 operates in the same way as FIG. The adder circuit 5 in FIG. 1 has an inversion characteristic, and the integrator circuit 506 in FIG.
does not have an inverted q-mo property, so when the terminal 5osa of the diaphragm drive coil 508 is driven with a negative voltage, the diaphragm 502 is closed, and when it is driven with a positive voltage, , 4□, 5o2□8. 6 o i, 1. ¥, B 7io.・Jl, ・[Effect] As is clear from the above explanation, according to the present invention, by adding a simple amplitude compression circuit, the influence of bright spots in the object space can be eliminated, and the accuracy of object information can be improved. can be significantly improved.

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

第1図は本発明の第1実施例の1u気回路ブロック図、
第2図は受光素子a −dの空間配置の例を示す図、第
6図は光電変換回路3−〜ろdの具体的構成例図、第4
図、第6図は夫々振幅圧縮回路の実施例を示す図、第5
図、第7図は夫々第4図。 第6図示回路の入出力振幅特性図、第8図は加算回路の
構成例図、第9図、第10図は振巾圧縮回路の他の実施
例の入出力特性図、第11図は本発明の第2実施例の構
成図、第12図は第11図中の積分回路の具体回路例図
である。 1・・・・・・・・・光学系 2・・・・・・・・・絞
りa−d・・・・・・・・・光電変換手段としての受光
素子6a〜ろd・・・・・・光電変換回路 4a〜4d・・・・・・振幅圧縮手段としての振幅圧縮
回路5・・・・・・・・・混合手段としての加算回路1
0・・・・・・誤差増幅器および絞り駆動コイル駆動回
路11・・・・・・絞り駆動回路 501・・・・・・光学系 502・・・・・・絞り5
06・・・・・・撮像手段としてのCCD等の撮像デノ
くイス504・・・・・・信号処理回路 506・・・・・・振幅圧縮手段としての振幅圧縮回路
507・・・・・・混合手段としての積分回路508・
・・・・・誤差増幅器
FIG. 1 is a 1u air circuit block diagram of the first embodiment of the present invention,
FIG. 2 is a diagram showing an example of the spatial arrangement of light receiving elements a to d, FIG. 6 is a diagram showing a specific configuration example of photoelectric conversion circuits 3--d, and
Figure 6 is a diagram showing an embodiment of the amplitude compression circuit, and Figure 5 shows an embodiment of the amplitude compression circuit, respectively.
Figures 7 and 7 are respectively Figure 4. 6 is an input/output amplitude characteristic diagram of the illustrated circuit, FIG. 8 is a configuration example diagram of an adder circuit, FIGS. 9 and 10 are input/output characteristic diagrams of other embodiments of the amplitude compression circuit, and FIG. 11 is a diagram of the present invention. A block diagram of the second embodiment of the invention, FIG. 12 is a specific circuit diagram of the integrating circuit in FIG. 11. 1... Optical system 2... Aperture a-d... Light-receiving elements 6a to d... as photoelectric conversion means ...Photoelectric conversion circuits 4a to 4d...Amplitude compression circuit 5 as amplitude compression means...Addition circuit 1 as mixing means
0...Error amplifier and aperture drive coil drive circuit 11...Aperture drive circuit 501...Optical system 502...Aperture 5
06...Imaging device 504 such as a CCD as an imaging means...Signal processing circuit 506...Amplitude compression circuit 507 as an amplitude compression means...・Integrator circuit 508 as mixing means・
...Error amplifier

Claims (1)

【特許請求の範囲】[Claims] 被写体像を複数の部分に分割して光電変換する複数の光
電変換手段と、該光電変換手段の出力を夫々振巾圧縮す
る振巾圧縮手段と、該振巾圧縮手段の出力を混合する混
合手段とを有する被写体情報検出装置。
A plurality of photoelectric conversion means that divides a subject image into a plurality of parts and photoelectrically converts them, amplitude compression means that amplitude compresses the outputs of the photoelectric conversion means, and mixing means that mixes the outputs of the amplitude compression means. A subject information detection device comprising:
JP58153680A 1983-08-23 1983-08-23 Detecting device of information on object to be photographed Pending JPS6045228A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58153680A JPS6045228A (en) 1983-08-23 1983-08-23 Detecting device of information on object to be photographed

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58153680A JPS6045228A (en) 1983-08-23 1983-08-23 Detecting device of information on object to be photographed

Publications (1)

Publication Number Publication Date
JPS6045228A true JPS6045228A (en) 1985-03-11

Family

ID=15567810

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58153680A Pending JPS6045228A (en) 1983-08-23 1983-08-23 Detecting device of information on object to be photographed

Country Status (1)

Country Link
JP (1) JPS6045228A (en)

Similar Documents

Publication Publication Date Title
US5001552A (en) White balance correction using prestored flash lamp color temperature data
US9167167B2 (en) System and method for high dynamic range image sensor sensitive array
US3690234A (en) Apparatus for taking photographs at times of minimum image motion
CN103369252A (en) Image processing apparatus and control method therefor
US5465116A (en) Image pickup device having white balance control function
US5041911A (en) Exposure information feedback in electronic and/or hybrid film/electronic cameras
US4247186A (en) Photometric circuit for camera
JPH0466303B2 (en)
JPS6045228A (en) Detecting device of information on object to be photographed
US5351080A (en) Color temperature control by comparing chrominance signals with reference levels
JPS5965829A (en) Automatic electronic flash device
JPS6356964B2 (en)
US4023910A (en) Electronic photometer with two variable indicators
JPS59122084A (en) Photometric circuit of automatic aperture lens for cctv camera
JP3058994B2 (en) Video camera and photometric method thereof
JP3010373B2 (en) Imaging device
JP2952518B2 (en) Imaging device
JPH02274073A (en) Exposure control method
JPS63246084A (en) Automatic exposure controller for electronic camera
JPS61124925A (en) Automatic exposure correcting device
JPS60125527A (en) Photometric circuit of camera
JPS6338119A (en) Photometry instrument
JPH06189184A (en) Video camera and photometric method therefor
JPH04147235A (en) Image pickup device
JPS6190141A (en) Camera