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JPH0346809B2 - - Google Patents
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JPH0346809B2 - - Google Patents

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Publication number
JPH0346809B2
JPH0346809B2 JP55152157A JP15215780A JPH0346809B2 JP H0346809 B2 JPH0346809 B2 JP H0346809B2 JP 55152157 A JP55152157 A JP 55152157A JP 15215780 A JP15215780 A JP 15215780A JP H0346809 B2 JPH0346809 B2 JP H0346809B2
Authority
JP
Japan
Prior art keywords
light
photometry
liquid crystal
electro
brightness
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 - Lifetime
Application number
JP55152157A
Other languages
Japanese (ja)
Other versions
JPS5776533A (en
Inventor
Yoshiaki Takahashi
Kazuo Shiozawa
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.)
Konica Minolta Inc
Original Assignee
Konica Minolta 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 Konica Minolta Inc filed Critical Konica Minolta Inc
Priority to JP55152157A priority Critical patent/JPS5776533A/en
Publication of JPS5776533A publication Critical patent/JPS5776533A/en
Publication of JPH0346809B2 publication Critical patent/JPH0346809B2/ja
Granted 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
    • G03B7/08Control effected solely on the basis of the response, to the intensity of the light received by the camera, of a built-in light-sensitive device
    • G03B7/099Arrangement of photoelectric elements in or on the camera

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Liquid Crystal (AREA)
  • Exposure Control For Cameras (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

この発明は、TTL測光装置の改良にかかり、
受光素子、測光回路を特に複雑にすることなく、
種種の撮影条件に対して対応出来、特にカメラに
組込むに適した測光装置に関するものである。 従来、TTL測光装置は、画面全体の平均の明
るさを測光する平均測光方式、画面の一部の明る
さを測光する部分測光方式およびその中間である
中央重点平均測光方式等が用いられている。しか
し、被写体の輝度分布はまちまちであり、平均測
光では逆光の場合は主要被写体に対して適正露出
を得ることは難しい。部分測光の場合も、マニユ
アル撮影の場合はよいが、EE機構によりシヤツ
タレリーズ直前に露出条件が決定されるようなも
ので画面中央に主要被写体がない場合等、適正露
出を得ることが難しい場合が少なくない。 このため、平均測光の部分測光とを任意に切換
えられる方式(特開昭55−101921号)や受光器の
受光領域を複数に区分し、各区分ごとの受光量を
適宜組合せることによつて適切な露光条件を得る
ようにする法式(特開昭54−123030号)等が提案
されている。しかし、前者は平均測光と部分測光
とを組合せようとすれば2回測光となるざるを得
ず、測光値の処理回路が複雑になり、主要被写体
を遮蔽する方式では、測光しない部分が撮影者に
見えなくなり、ピント合せと測光を同時に行うこ
とが出来ない。一方、後者は上述のような欠点は
ないが、受光素子を細分化する必要があり、細分
化された各部の受光量を測定するため電気回路が
複雑となる。また、撮影者は具体的・感覚的に測
光位置を知ることが出来ない。 この発明は、カメラに組込まれたピント板の各
部の透過率を変化させ、フアインダー内で視野の
各部分の輝度をほぼ平均させて測光することによ
り上記の欠点を除いた測光装置を得ようとするも
のである。以下図面を参照して詳細に説明する。 第1図は、この発明を1眼レフカメラに組込ん
だ場合の測光装置全体の概念図で通常のTTL1眼
レフと同様に撮影レンズ6から入射した被測定光
は反射鏡5で反射された後ピン1板1に像を結
ぶ。このピント板で後述のように部分的な輝度調
整を受けた被測定光はペンタプリズム2の射出口
すなわちアイピース3の近傍に配置されたただ1
つの受光素子4によつて光量検出が行われる。 ピント板1は電気光学的拡散板、例えば液晶に
よつて作られ、例えば第2図A,B,Cに示すよ
うに、適宜のパターンに区分され、各区分はそれ
ぞれ個別の電極によつて電圧を別々に印加出来る
ように構成されている。このため、後述のよう
に、各区分ごとにパルス電圧の印加によつて透明
状態、半透明状態、濃度最大の状態へと変化させ
ることが可能である。 例えば、第3図のような海岸で水辺に立つ人物
像の撮影では、背景の光量は非常に大きく、平均
測光あるいは中央重点測光では背景の空の明るさ
に影響されて、中央のaの部分の人物の露光はア
ンダー気味になる。このような場合、上半部の
b、c部の液晶の電圧を上げて透過率を下げ、ピ
ント板上の照度を下げて測光するか、さらには反
射の強い海岸部を含むd、e部を含めてb、c、
d、e部の液晶の濃度を上げて測光すれば、a部
の人物がアンダー気味の露光になるのを防ぐこと
が出来る。このように、被写体輝度に大きな差が
あり、適正露光にしたい被写体が低輝度になつて
いる場合には、高輝度側の照度を液晶によつて低
下させ、全面一様なピント板照度にして測光する
ものである。逆に高輝度側に主要被写体の輝度が
片寄つている場合は、主要被写体以外の液晶濃度
を下げ、ピント板上で全面をほぼ一様な照度の被
写体として測光出来ることはいうまでもない。 このようなピント板を用いた測光装置の作動回
路を第4図に示す。被測定光を受ける光電素子P
の光電流は、演算増幅器O1によつて対数変換さ
れる。一方、電気光学的拡散板の透過部分の違い
による受光素子Pの出力の差を補償するため、切
り換えスイツチS1が設けられる。このスイツチS1
によるレベル設定情報及びフイルム感度設定部
S、シヤツタ速度設定部Tからの露出決定情報
は、それぞれ演算増幅器O2,O3,O5を経て上記
の光強度の情報と共に演算増幅器O4に入力され、
絞値F相当電圧として出力される。ACは露出制
御回路で公知のようにソレノイド等により絞り、
シヤツタを制御する。 測光位置選択スイツチS2は電気光学的拡散板の
部分透過率を選択するためのもので、レベル設定
を切り換えスイツチS1と連動し、例えば第2図A
に示すピント板とスイツチ選択位置を下記のよう
に対応させておく。
This invention involves improving a TTL photometry device,
without complicating the photodetector and photometry circuit.
The present invention relates to a photometry device that can be adapted to various photographic conditions and is particularly suitable for being incorporated into a camera. Traditionally, TTL photometry devices use an average metering method that measures the average brightness of the entire screen, a partial metering method that measures the brightness of a part of the screen, and a center-weighted average metering method that is in between. . However, the brightness distribution of the subject varies, and it is difficult to obtain a proper exposure for the main subject when the subject is backlit using average metering. Partial metering is fine for manual shooting, but when it is difficult to obtain the correct exposure, such as when the EE mechanism determines the exposure conditions immediately before the shutter release and the main subject is not in the center of the screen. There are quite a few. For this reason, a method that allows arbitrary switching between average photometry and partial photometry (Japanese Unexamined Patent Publication No. 101921/1982), and a method that divides the light receiving area of the receiver into multiple parts and appropriately combines the amount of light received for each division are available. A method (Japanese Unexamined Patent Publication No. 123030/1983) has been proposed for obtaining appropriate exposure conditions. However, in the former case, if you try to combine average metering and partial metering, you have to measure the light twice, and the metering value processing circuit becomes complicated. It becomes impossible to focus and meter at the same time. On the other hand, although the latter does not have the above-mentioned drawbacks, it is necessary to subdivide the light receiving element, and the electric circuit becomes complicated because the amount of light received by each subdivided part is measured. Further, the photographer cannot concretely or intuitively know the photometry position. This invention attempts to obtain a photometry device that eliminates the above-mentioned drawbacks by changing the transmittance of each part of the focusing plate built into the camera and measuring the brightness of each part of the field of view within the viewfinder by approximately averaging it. It is something to do. A detailed explanation will be given below with reference to the drawings. FIG. 1 is a conceptual diagram of the entire photometering device when this invention is incorporated into a single-lens reflex camera. Similar to a normal TTL single-lens reflex camera, the light to be measured enters from the photographing lens 6 and is reflected by the reflector 5. Focus the image on the rear pin 1 plate 1. The light to be measured, which has undergone partial brightness adjustment as described later with this focusing plate, is transmitted to a single point located near the exit port of the pentaprism 2, that is, the eyepiece 3.
Light amount detection is performed by the two light receiving elements 4. The focusing plate 1 is made of an electro-optical diffuser, for example a liquid crystal, and is divided into appropriate patterns, for example as shown in FIG. It is configured so that it can be applied separately. Therefore, as will be described later, by applying a pulse voltage to each section, it is possible to change the state to a transparent state, a translucent state, and a state with maximum density. For example, when photographing a person standing by the water on a beach as shown in Figure 3, the amount of light in the background is very large, and with average metering or center-weighted metering, the brightness of the background sky will affect the brightness of the central part a. The exposure of the person is slightly underexposed. In such a case, increase the voltage of the liquid crystal in parts b and c of the upper half to lower the transmittance, lower the illuminance on the focusing plate, and measure the light, or furthermore, measure the light by increasing the voltage of the liquid crystal in parts b and c of the upper half. including b, c,
By increasing the density of the liquid crystal in sections d and e and performing photometry, it is possible to prevent the person in section a from being slightly underexposed. In this way, if there is a large difference in subject brightness and the subject you want to properly expose is low brightness, the illuminance on the high brightness side is lowered by the liquid crystal and the focus plate illuminance is uniform across the entire surface. It measures light. On the other hand, if the brightness of the main subject is biased toward the high-brightness side, it goes without saying that you can lower the liquid crystal density of the objects other than the main subject and measure the entire surface on the focus board with almost uniform illuminance. FIG. 4 shows an operating circuit of a photometric device using such a focusing plate. Photoelectric element P that receives the light to be measured
The photocurrent of is logarithmically converted by the operational amplifier O1 . On the other hand, a changeover switch S1 is provided to compensate for differences in the output of the light-receiving elements P due to differences in the transmitting portions of the electro-optic diffuser. This switch S 1
The level setting information and the exposure determination information from the film sensitivity setting section S and shutter speed setting section T are input to the operational amplifier O4 together with the above light intensity information via operational amplifiers O2 , O3 , and O5, respectively. ,
It is output as a voltage corresponding to the aperture value F. The AC is throttled by a solenoid, etc., as is known in the exposure control circuit.
Control the shutters. The photometric position selection switch S2 is used to select the partial transmittance of the electro-optic diffuser plate, and is linked to the level setting switch S1 .
The focus plate shown in and the switch selection position correspond as shown below.

【表】 スイツチS2からの入力をデータDは上表のよう
に出力Sa〜Seにデコードして出力する。S3は液
晶の濃度切換えスイツチでHに投入されるとS0
ら1信号が出力され、アナログスイツチA1をオ
ンし、A2をオフにして液晶への印加電圧をVrに
設定する。スイツチS3をLに投入すればS0からの
出力は0信号となりアナログスイツチA1をオフ
に、A2をオンにし、液晶印加電圧は1/2Vrとな
り、印加電圧の低下によつて液晶の透過率は向上
する。 OCは発振器で露出制御回路ACに基準パルスを
供給すると共に、液晶に交番電界を印加するため
に駆動パルスを発生している。 ゲートG1,G2,アナログスイツチAa1,Aa2
液晶電極aの駆動回路を構成しており、同様の駆
動回路が電極b〜eにもそれぞれ設けられている
が図では省略してある。G1,G2は電極選択用ゲ
ートでデコーダDのSaの出力が1のときだけ交
番信号をアナログスイツチに供給して電極aに交
流電圧を印加する。 Saからの出力が1で、かつ発振器OCからの駆
動パルスが1の状態の時はアナログスイツチAa2
がオンとなり、液晶の共通電極fはスイツチAf1
がオンとなるので、f(Vr)→a(0)方向に電圧が印加さ
れる。次に発振器OCからの駆動パルスが0にな
ると、スイツチAa1,Af2がオンになるので、逆
にa(Vr)→f(0)の方向に電圧が印加される。したがつ
て、デコーダDのSaから1の信号が出力されて
いる間は電極aとfとの間に発振器OCからの駆
動パルスに同期した交流電界が印加され、電極
a、f間の液晶は拡散状態を保つことになる。部
分電極b〜eについても同様で、デコーダDの出
力により所定の部分が交流電界を印加されて拡散
状態になる。この実施例では、説明の都合上、液
晶の一ケ所だけが透明状態になるようにしてある
が、複数個所を透明状態にすることもデコーダの
構成を変えることによつて容易に実現出来る。 以上のように、この発明はピント板に電気光学
的拡散板を用い、部分的に光透過率を変えてピン
ト板全面の照度をほぼ一様にして測光するように
したので、 フアインダー中で主要被写体の像が常にそのま
まの状態で確認出来、ピント合せと同時に測光が
出来る。 フアインダー中でピント板全体の照度が同じに
なるよう各部の明るさを確認しながら操作出来る
ので、信頼感を持つことが出来、主要被写体が画
面のどの位置にあつても同じような操作でよい。 受光素子は従来のものを用いることが出来、特
にその個数を増す必要はない。 測光回路に従来のものを使用することが出来
る。等、多くの利点を有するものである。
[Table] Data D decodes the input from switch S2 into outputs Sa to Se as shown in the table above. S3 is a liquid crystal concentration changeover switch, and when turned to H, a 1 signal is output from S0 , turning on analog switch A1 , turning off A2 , and setting the voltage applied to the liquid crystal to Vr. When switch S 3 is turned to L, the output from S 0 becomes a 0 signal, turning off analog switch A 1 and turning on A 2 , and the voltage applied to the liquid crystal becomes 1/2V r . The transmittance of is improved. The OC is an oscillator that supplies reference pulses to the exposure control circuit AC, and also generates drive pulses to apply an alternating electric field to the liquid crystal. Gates G 1 and G 2 and analog switches Aa 1 and Aa 2 constitute a drive circuit for liquid crystal electrode a, and similar drive circuits are provided for electrodes b to e, respectively, but are omitted in the figure. . G 1 and G 2 are electrode selection gates that supply an alternating signal to the analog switch and apply an alternating voltage to electrode a only when the output of Sa of decoder D is 1. When the output from Sa is 1 and the drive pulse from the oscillator OC is 1, the analog switch Aa 2
is turned on, and the common electrode f of the liquid crystal is switched to Af 1
is turned on, so a voltage is applied in the direction f (Vr) → a (0) . Next, when the drive pulse from the oscillator OC becomes 0, the switches Aa 1 and Af 2 are turned on, so that a voltage is applied in the opposite direction from a (Vr) to f (0) . Therefore, while a signal of 1 is being output from Sa of decoder D, an AC electric field synchronized with the drive pulse from the oscillator OC is applied between electrodes a and f, and the liquid crystal between electrodes a and f is It will maintain a diffused state. The same applies to partial electrodes b to e, and predetermined portions are applied with an alternating current electric field by the output of decoder D, and are brought into a diffused state. In this embodiment, for convenience of explanation, only one portion of the liquid crystal is made transparent, but it is also possible to make a plurality of portions transparent by easily changing the configuration of the decoder. As described above, this invention uses an electro-optic diffuser for the focus plate and partially changes the light transmittance to make the illuminance almost uniform over the entire surface of the focus plate for photometry. You can always check the image of the subject as it is, and you can measure the light at the same time as focusing. Since you can operate while checking the brightness of each part in the viewfinder to ensure that the illuminance of the entire focus plate is the same, you can feel confident and you can operate in the same way no matter where the main subject is on the screen. . Conventional light receiving elements can be used, and there is no particular need to increase the number of them. A conventional photometric circuit can be used. It has many advantages such as.

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

第1図はこの発明の測光装置を組込んだ1眼レ
フカメラの測光装置の概念図、第2図はこの発明
に使用されるピント板の区分例を示す図、第3図
は測光法の説明図、第4図は作動回路の説明図で
あり、図中の符号はそれぞれ 1:ピント板、2:ペンタプリズム、3:アイ
ピース、4,P:受光素子、5:反射鏡、6:撮
影レンズ、O:演算増幅器、AC:露出制御回路、
S:スイツチ、D:デコーダ、A:アナログスイ
ツチ、OC:基準パルス発振器、G:ゲートを示
す。
Fig. 1 is a conceptual diagram of a photometric device for a single-lens reflex camera incorporating the photometric device of the present invention, Fig. 2 is a diagram showing an example of classification of a focusing plate used in this invention, and Fig. 3 is a diagram showing a photometric method of a single-lens reflex camera. The explanatory diagram and Fig. 4 are explanatory diagrams of the operating circuit, and the symbols in the diagram are respectively 1: focusing plate, 2: pentaprism, 3: eyepiece, 4, P: light receiving element, 5: reflecting mirror, 6: photographing. Lens, O: operational amplifier, AC: exposure control circuit,
S: switch, D: decoder, A: analog switch, OC: reference pulse oscillator, G: gate.

Claims (1)

【特許請求の範囲】[Claims] 1 焦点板の後方に受光素子を配置した測光装置
において、前記焦点板の全面を適宜のパターンに
区分した電気光学拡散板により構成すると共に、
前記電気光学拡散板の各区分それぞれの透過率を
それぞれ独立に変化させるための、電気的制御手
段を設け、測光に先立ち、前記電気的制御手段に
より、主要被写体以外の区分における前記電気光
学拡散板の透過率を変化させて、主要被写体の区
分と主要被写体以外の区分との輝度をほぼ等しく
しうるように構成したことを特徴とする測光装
置。
1. A photometric device in which a light-receiving element is arranged behind a focus plate, in which the entire surface of the focus plate is constituted by an electro-optic diffuser plate divided into appropriate patterns,
An electric control means is provided for independently changing the transmittance of each section of the electro-optic diffuser, and prior to photometry, the electric control means controls the electro-optic diffuser in sections other than the main subject. 1. A photometry device characterized in that the luminance of a main subject section and a section other than the main subject can be made almost equal by changing the transmittance of the photometer.
JP55152157A 1980-10-31 1980-10-31 Photometric device Granted JPS5776533A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55152157A JPS5776533A (en) 1980-10-31 1980-10-31 Photometric device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55152157A JPS5776533A (en) 1980-10-31 1980-10-31 Photometric device

Publications (2)

Publication Number Publication Date
JPS5776533A JPS5776533A (en) 1982-05-13
JPH0346809B2 true JPH0346809B2 (en) 1991-07-17

Family

ID=15534262

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55152157A Granted JPS5776533A (en) 1980-10-31 1980-10-31 Photometric device

Country Status (1)

Country Link
JP (1) JPS5776533A (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55161221A (en) * 1979-06-04 1980-12-15 Canon Inc Photometric device
JPS5689027A (en) * 1979-12-21 1981-07-20 Fuji Photo Film Co Ltd Photometry device

Also Published As

Publication number Publication date
JPS5776533A (en) 1982-05-13

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