JPH0547815B2 - - Google Patents
Info
- Publication number
- JPH0547815B2 JPH0547815B2 JP56190711A JP19071181A JPH0547815B2 JP H0547815 B2 JPH0547815 B2 JP H0547815B2 JP 56190711 A JP56190711 A JP 56190711A JP 19071181 A JP19071181 A JP 19071181A JP H0547815 B2 JPH0547815 B2 JP H0547815B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- signal
- view
- distance
- distance measurement
- 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
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B7/00—Mountings, adjusting means, or light-tight connections, for optical elements
- G02B7/28—Systems for automatic generation of focusing signals
- G02B7/30—Systems for automatic generation of focusing signals using parallactic triangle with a base line
- G02B7/32—Systems for automatic generation of focusing signals using parallactic triangle with a base line using active means, e.g. light emitter
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Focusing (AREA)
- Automatic Focus Adjustment (AREA)
Description
【発明の詳細な説明】
本発明は、投光素子より被写体に光を投射し、
被写体からの反射光を計測し、被写体までの距離
を測定する装置の改良に関するものである。[Detailed description of the invention] The present invention projects light onto a subject from a light projecting element,
The present invention relates to an improvement of a device that measures reflected light from a subject and measures the distance to the subject.
従来、光を被写体に投射して、被写体上を走査
し、距離を測定する測距システムに於いては、測
距視野を大きくすると測距精度が悪くなり、精度
を上げるためには投光部と受光部間の基線長を増
さなければならず、又受光素子側から見ると視野
が広くなり、外部の明るさ、あるいは、蛍光灯等
の光源によるノイズの影響が出てくるので、実際
には大きくすることはできず、なるべく絞つて使
つているのが現状で、投光角度として1〜2°位で
ある。、このため、被写体を撮影する時、普通測
距視野は撮影用フアインダーフレームの中心にあ
るが、この狭い測距視野を被写体に向けて合わさ
なければならず、構図に限定があり、シヤツター
チヤンスを逃す恐れがあり、被写体が人物2人の
時の撮影ではプリフオーカスを使用せざるを得な
かつた。 Conventionally, in distance measurement systems that project light onto a subject, scan it, and measure distance, increasing the field of view reduces the accuracy of distance measurement, and in order to increase accuracy, it is necessary to It is necessary to increase the baseline length between the light receiving element and the light receiving element, and the field of view becomes wider when viewed from the light receiving element side, which increases the influence of noise from external brightness or light sources such as fluorescent lights. Currently, it is not possible to increase the angle of light, so we are currently using it as narrowly as possible, and the projection angle is about 1 to 2 degrees. For this reason, when photographing a subject, the distance-measuring field of view is normally located at the center of the photographic viewfinder frame, but this narrow distance-measuring field of view must be aligned toward the subject, which limits the composition of the shot. Because of the risk of missing the subject, I had to use pre-focus when shooting two people.
本発明は上記の点に鑑み、上記欠点を解消する
ためになされたもので、撮影の構図に気を使わず
に、近距離から遠距離まで高精度に測距できる測
距装置を提供するもので、目標に向けて光源から
光を投射し、その反射光を前記光源から所定の基
線長離れた位置にある受光素子にて受光し、該受
光信号に基づいて距離に依存する測距信号を得る
測距装置において、方向の異なる複数の目標に向
けて光を順次走査させて投射する投光手段と、複
数の異なる測距視野からの前記投光手段により投
射された光の反射光を受光し、各視野からの上記
反射光に応じた受光信号をそれぞれ独立に出力す
る受光手段と、各受光信号をそれぞれ測距視野に
対応して、それぞれ異なる時間遅延させて出力す
る遅延回路と、各受光信号に対する前記遅延出力
のうち最も早く出力された遅延出力に基づいてピ
ント調定を行なうピント調定手段とを有するもの
である。 The present invention has been made in view of the above points and in order to eliminate the above drawbacks, and provides a distance measuring device that can measure distances with high accuracy from short distances to long distances without worrying about the composition of the photograph. A light source projects light toward a target, the reflected light is received by a light receiving element located a predetermined baseline length away from the light source, and a distance-dependent distance measurement signal is generated based on the received light signal. A distance measuring device that obtains a distance measuring device includes a light projecting means for sequentially scanning and projecting light toward a plurality of targets in different directions, and receiving reflected light of the light projected by the light projecting means from a plurality of different ranging fields of view. a light-receiving means for independently outputting a light-receiving signal corresponding to the reflected light from each field of view; a delay circuit for outputting each light-receiving signal with a different time delay corresponding to each distance-measuring field of view; and a focus adjustment means for performing focus adjustment based on the earliest output of the delayed outputs for the received light signal.
以下、本発明の一実施例を図面に従つて詳細に
説明する。 Hereinafter, one embodiment of the present invention will be described in detail with reference to the drawings.
第1図は本発明に関わる測距の原理を示す図面
であつて、LEDは赤外発光ダイオードや半導体
レーザー等の投光素子で矢印aのように振られ、
レンズL1を通して被写体OBの方を至近から無限
遠の方向に走査する。DはレンズL1とレンズL2
の間隔で基線長である。SPC1,SPC2,SPC
3,SPC4は受光素子で、レンズL2の矢印bの
方向の動きによつてLEDによる被写体OBに投射
された像のレンズL2による光像を受けるように
なつている。従つてレンズL2の動きは、投光素
子LEDが被写体側の至近から無限遠迄可変する
時に、LEDの光線がレンズL2の光軸に交わると
して、交点に像ができるとすると、その交点の像
が受光素子SPC1〜SPC4のいずれかの面上にレ
ンズL2を通して結像するように動く。たとえば、
本発明の測距装置をカメラの自動焦点に用いる場
合は、レンズL2の後方に配置されたフイルム面
と共役な位置に受光素子SPC1〜SPC4を配置す
るか、撮影レンズとは別個にレンズL2を設けて、
前記せるようにレンズL2を移動させれば良い。
第1図の状態では、被写体OBの同一面上(レン
ズL2の光軸に直角な面上)に受光素子SPC1〜
SPC4の光像がレンズL2を通して結像されてい
る。その像がSPC1′〜SPC4′である(この像
は、実際は受光素子から光束がでてないので形成
されていない)。逆に言えば、投光素子LEDが
SPC1′〜SPC4′の範囲を走査して、被写体OB
上に投射された像は全てレンズL2により受光素
子SPC1〜SPC4上に結像する。従つて被写体
OBの位置ではSPC1′〜SPC4′の像の範囲が測
距視野となる。このようにして投光素子LEDの
投射光により被写体OBが走査され、走査された
像はレンズL2を介して受光素子SPC1〜SPC4
に結像されて、該受光素子からの信号を処理する
ことにより測距する。 FIG. 1 is a diagram showing the principle of distance measurement related to the present invention, in which the LED is a light emitting element such as an infrared light emitting diode or a semiconductor laser, and is swung in the direction of arrow a.
The object OB is scanned from close range to infinity through lens L1 . D is lens L 1 and lens L 2
The baseline length is the interval of . SPC1, SPC2, SPC
3. SPC4 is a light-receiving element, which receives the light image of the image projected onto the object OB by the LED by the lens L2 by movement of the lens L2 in the direction of arrow b. Therefore, the movement of the lens L2 is such that when the light emitting element LED changes from close to the subject side to infinity, the light beam of the LED intersects the optical axis of the lens L2 , and an image is formed at the intersection point. moves so that the image thereof is formed on one of the surfaces of the light receiving elements SPC1 to SPC4 through the lens L2 . for example,
When using the distance measuring device of the present invention for automatic focusing of a camera, the light receiving elements SPC1 to SPC4 are placed at positions conjugate to the film surface placed behind the lens L2 , or the light receiving elements SPC1 to SPC4 are placed at positions conjugate to the film surface placed behind the lens L2, or the lens L2 is placed separately from the photographic lens. 2 ,
All you have to do is move the lens L2 as described above.
In the state shown in Fig. 1, the light receiving elements SPC1 to
The light image of SPC4 is focused through lens L2 . The images are SPC1' to SPC4' (this image is not actually formed because no light beam is emitted from the light receiving element). Conversely, if the light emitter LED
Scan the range from SPC1' to SPC4' to capture the object OB.
All the images projected above are formed on the light receiving elements SPC1 to SPC4 by the lens L2 . Therefore, the subject
At the OB position, the range of images of SPC1' to SPC4' becomes the distance measurement field of view. In this way, the object OB is scanned by the projection light of the light emitting element LED, and the scanned image is sent to the light receiving elements SPC1 to SPC4 via the lens L2 .
The distance is measured by processing the signal from the light receiving element.
第2図は受光素子からの信号を処理する評価回
路の一例を示す回路図で、OP1〜OP4は演算増
幅器で、受光素子SPC1〜SPC4の光電流を帰還
抵抗1〜4で電圧に各々変換する。投光素子
LEDはパルス駆動されるのでOP1〜OP4の出力
は交流信号となる。5〜8は交流増幅器でOP1
〜OP4からの交流信号を各々増幅する。9〜1
2は同期検波回路で、投光素子LEDの駆動パル
スと同期したパルスにより同期検波し、交流増幅
器5〜8からの交流信号を各々直流化する。29
〜32は同期検波回路9〜12とピーク検出回路
13〜16を各々接続するラインである。33〜
36は同期検波回路9〜12とANDゲート21
〜24の入力端子を各々接続するラインで、投光
素子LEDで走査され、同期検波回路9〜12に
より直流化された信号成分がある検出レベルを越
えた時から投光素子LEDの走査が終了する迄、
“ハイ”レベルの信号を伝え、その他の時は、“ロ
ー”レベルの信号を伝える。13〜16はピーク
検出回路で17〜20のタイマー回路と組み合せ
て信号のピークの正確なタイミングを決定する。
37〜40はタイマー回路17〜20とANDゲ
ート21〜24の入力端を各々接続するライン
で、ピーク信号を伝える。ANDゲート21〜2
4の出力はNORゲート25の入力として与えら
れるよう各々接続されている。その出力は電流制
限用抵抗26を介してトランジスタ27のベース
に入力されるよう接続されている。28は、第4
図に示されている撮影レンズ等を保持している鏡
筒の駆動を係止するストツプ爪を動かすためのマ
グネツトのコイルである。マグネツトのコイル2
8は、電源Vbatとトランジスタ27に接続され
ている。 Figure 2 is a circuit diagram showing an example of an evaluation circuit that processes signals from photodetectors. OP1 to OP4 are operational amplifiers, and the photocurrents of photodetectors SPC1 to SPC4 are converted into voltages by feedback resistors 1 to 4, respectively. . Light emitting element
Since the LEDs are pulse driven, the outputs of OP1 to OP4 are AC signals. 5 to 8 are AC amplifiers OP1
~ Amplify each AC signal from OP4. 9-1
Reference numeral 2 denotes a synchronous detection circuit, which performs synchronous detection using a pulse synchronized with the driving pulse of the light projecting element LED, and converts the AC signals from the AC amplifiers 5 to 8 into DC signals. 29
32 are lines connecting the synchronous detection circuits 9 to 12 and the peak detection circuits 13 to 16, respectively. 33~
36 is the synchronous detection circuit 9 to 12 and the AND gate 21
The scanning of the light projector LED ends when the signal component, which is scanned by the light projector LED and converted into DC by the synchronous detection circuits 9 to 12, exceeds a certain detection level on the line connecting each of ~24 input terminals. Until
It transmits a "high" level signal, and at other times transmits a "low" level signal. 13 to 16 are peak detection circuits which are combined with timer circuits 17 to 20 to determine the exact timing of the signal peak.
Lines 37 to 40 connect the input terminals of the timer circuits 17 to 20 and the AND gates 21 to 24, respectively, and transmit peak signals. AND gate 21-2
The outputs of 4 are connected to each other so as to be provided as inputs to a NOR gate 25. Its output is connected to be input to the base of a transistor 27 via a current limiting resistor 26. 28 is the fourth
This is a magnet coil for moving a stop pawl that locks the lens barrel that holds the photographic lens shown in the figure. magnet coil 2
8 is connected to the power supply Vbat and the transistor 27.
第3図はライン29〜32の各々の信号波形図
を示している図面である。 FIG. 3 is a drawing showing signal waveform diagrams of each of lines 29-32.
第4図は撮影レンズ等を保持している鏡筒の動
きを、測距完了時に係止する鏡筒係止装置の一実
施例の図面である。TLは撮影レンズ等を中に保
持している鏡筒で、紙面と垂直方向にスプリング
SP2の力によつて駆動される。スプリングSP2
は鏡筒TLを矢印c方向に駆動し、鏡筒TLは、紙
面と垂直方向にネジが切つてあり、固定部(図示
せず)と螺合しているので、矢印cの方向の駆動
で紙面と垂直方向に移動する。鏡筒TLの側面に
ギアGRがきざんである。STは鏡筒TLの動きを
止めるためのストツプ爪で、軸41により回動可
能に軸支され、ストツプ爪の先端がギアGRに食
い込むことにより鏡筒TLを係止する。SP1はス
プリングでストツプ爪の先端をギアGRに向かせ
るためのものである。42はマグネツトでマグネ
ツトのコイル28が巻回され、マグネツトのコイ
ル28に電流が流れた時、ストツプ爪STの先端
を鏡筒TLのギアGRから離すようにする。 FIG. 4 is a drawing of an embodiment of a lens barrel locking device that locks the movement of a lens barrel holding a photographic lens etc. upon completion of distance measurement. TL is a lens barrel that holds a photographic lens, etc. inside, and a spring is attached perpendicular to the plane of the paper.
Driven by the force of SP2. Spring SP2
The lens barrel TL is driven in the direction of arrow c, and since the lens barrel TL is threaded in a direction perpendicular to the page and is screwed into a fixed part (not shown), it can be driven in the direction of arrow c. Move perpendicular to the page. A gear GR is notched on the side of the lens barrel TL. ST is a stop pawl for stopping the movement of the lens barrel TL, which is rotatably supported by a shaft 41, and the tip of the stop pawl bites into the gear GR to lock the lens barrel TL. SP1 is a spring used to direct the tip of the stop pawl toward gear GR. Numeral 42 is a magnet around which a magnet coil 28 is wound, and when a current flows through the magnet coil 28, the tip of the stop claw ST is separated from the gear GR of the lens barrel TL.
次に、以上の如く構成される本発明の実施例の
動作を説明する。 Next, the operation of the embodiment of the present invention configured as above will be explained.
今、例えば、均一反射率の被写体を考えると、
投光素子LEDはパルス駆動されて、前述したよ
うに、至近から無限遠の方向に走査される。
LEDのパルス駆動は評価回路のS/Nを良くし
て高精度に測距できるようにするためのものであ
る。被写体に投射した反射光が受光素子SPC1〜
SPC4に入射し、演算増幅器OP1〜OP4と抵抗
1〜4で交流電流が交流電圧に変換され、変換さ
れた信号は交流増幅器5〜8で増幅され、同期検
波回路9〜12を経て信号成分を直流化する。直
流化された信号は、例えば、ライン29に出る信
号の場合、ピーク検出器13とタイマー回路17
により、第3図に示されているように、そのピー
クの時点からT1時間後に、ピークを示すピーク
信号がライン37に出力される。同様にライン3
0に出る信号波形はピーク検出器14とタイマー
回路18とにより、ライン31に出る信号波形は
ピーク検出器15とタイマー回路19とにより、
ライン32に出る信号波形はピーク検出器16と
タイマー回路20とにより、各々ピーク時点から
T2,T3,T4時間後にピーク信号が各々ライン3
8,39,40に出力される。故に、同一距離に
ある被写体のピーク信号は第3図ではQ〜Q′の
タイミングで出力され同時点となる。このライン
37〜40に出力されるピーク信号は、始めは
“ロー”レベルで、ピーク信号が出た時“ハイ”
レベルとなる。従つてピーク信号がこない間は、
ANDゲート21〜24の出力は“ロー”レベル
となり、NORゲート25の出力は“ハイ”レベ
ルとなるので、抵抗26を介してベースに接続さ
れているトランジスタ27は導通状態となり、マ
グネツトのコイル28は通電状態になつている。
ところが、ピーク信号がたとえばライン37に出
力された時は、同期検波回路9の検出レベルを信
号は越えており、ライン33は“ハイ”レベルと
なつているので、ANDゲート21の出力は“ハ
イ”レベルとなり、NORゲート25の出力は
“ロー”レベルとなり、トランジスタ27を非導
通状態とし、マグネツトのコイル28への通電を
断つ。すると、第4図に示されているように、マ
グネツト42により引きつけられていたストツプ
爪STがスプリングSP1により引張られ、その先
端がスプリングSP2の力により矢印c方向に回
転している鏡筒TLの側面にきざんであるギア
GRに飛び込むことによつて鏡筒は係止されて測
距が完了し、最も近い被写体、すなわち主被写体
にピントが合うことになる。そして撮影等が始ま
る。このように分割された受光素子のいずれか
に、被写体からの投光素子LEDの投射像が存在
すれば、正確な測距ならびに焦点調節が行われる
ことになる。 For example, if we consider an object with uniform reflectance,
The light projecting element LED is driven in pulses and scanned in the direction from close range to infinity, as described above.
The purpose of pulse driving of the LED is to improve the S/N ratio of the evaluation circuit and enable highly accurate distance measurement. The reflected light projected onto the subject is detected by light receiving elements SPC1~
The AC current enters the SPC 4, and is converted into an AC voltage by operational amplifiers OP1 to OP4 and resistors 1 to 4. The converted signal is amplified by AC amplifiers 5 to 8, and passes through synchronous detection circuits 9 to 12 to extract signal components. Convert to direct current. For example, in the case of a signal output on line 29, the DC signal is passed through the peak detector 13 and the timer circuit 17.
As a result, as shown in FIG. 3, a peak signal indicating the peak is output on line 37 at T 1 hours after the peak. Similarly line 3
The signal waveform that appears on line 31 is detected by the peak detector 14 and timer circuit 18, and the signal waveform that appears on line 31 is detected by the peak detector 15 and timer circuit 19.
The signal waveform appearing on the line 32 is detected by the peak detector 16 and the timer circuit 20 from the respective peak points.
T 2 , T 3 , T 4 hours later, the peak signal is on line 3, respectively.
8, 39, and 40. Therefore, the peak signals of objects located at the same distance are output at timings Q to Q' in FIG. 3, and are at the same time. The peak signals output to these lines 37 to 40 are initially at "low" level, and when the peak signal is output, they become "high".
level. Therefore, while the peak signal does not arrive,
The outputs of the AND gates 21 to 24 become "low" level, and the output of the NOR gate 25 becomes "high" level, so the transistor 27 connected to its base via the resistor 26 becomes conductive, and the magnet coil 28 becomes conductive. is in a energized state.
However, when the peak signal is output to line 37, for example, the signal exceeds the detection level of synchronous detection circuit 9, and line 33 is at a "high" level, so the output of AND gate 21 is "high". " level, and the output of the NOR gate 25 becomes a "low" level, making the transistor 27 non-conductive and cutting off the current to the magnet coil 28. Then, as shown in FIG. 4, the stop claw ST, which had been attracted by the magnet 42, is pulled by the spring SP1, and the tip of the stop claw ST is pulled toward the lens barrel TL, which is rotating in the direction of arrow c by the force of the spring SP2. gear notched on the side
By jumping into the GR, the lens barrel is locked, distance measurement is completed, and the closest subject, the main subject, is brought into focus. And then filming begins. If the projected image of the light projecting element LED from the subject is present in any of the light receiving elements divided in this way, accurate distance measurement and focus adjustment will be performed.
上述した実施例において、投光素子LEDおよ
びレンズL1が本発明の投光手段に相当し、以下
同様に、受光素子SPC1〜SPC4、レンズL2、
演算増幅器OP1〜OP4、帰還抵抗1〜4、交流
増幅器5〜8、同期検波回路9〜12、ピーク検
出回路13〜16、タイマー回路17〜20、
ANDゲート21〜24およびライン29〜40
が受光手段に相当し、NORゲート25、電流制
限用抵抗26およびトランジスタ27が評価回路
に相当する。 In the above embodiment, the light projecting element LED and the lens L1 correspond to the light projecting means of the present invention, and the light receiving elements SPC1 to SPC4, the lens L2 ,
Operational amplifiers OP1 to OP4, feedback resistors 1 to 4, AC amplifiers 5 to 8, synchronous detection circuits 9 to 12, peak detection circuits 13 to 16, timer circuits 17 to 20,
AND gates 21-24 and lines 29-40
corresponds to a light receiving means, and the NOR gate 25, current limiting resistor 26 and transistor 27 correspond to an evaluation circuit.
本発明は、上記せるように構成、動作すること
によつて、測距視野を広げたため、撮影者は自由
な構図を取り易くなり、性能上からも投光手段の
ビーム径が小さくでき、このため単位面積当りの
パワーを高くでき、S/Nがあがり、低反射率の
被写体まで測距できる。更に、基線長も短くでき
ることになるので、測距装置の小型化が可能とな
るという効果を有する。なお、今後安価になると
思われる半導体レーザーを投光素子に使用すれ
ば、この効果は絶大である。さらに、受光手段も
CCDアレイ等を使用すれば、自由な測距視野が
構成できる。 The present invention is configured and operated as described above to widen the field of view for distance measurement, making it easier for the photographer to take a free composition, and from the viewpoint of performance, the beam diameter of the light projecting means can be made small. Therefore, the power per unit area can be increased, the S/N ratio can be increased, and distance measurement can be performed even to objects with low reflectance. Furthermore, since the base line length can be shortened, there is an effect that the distance measuring device can be downsized. Note that this effect will be tremendous if a semiconductor laser, which is expected to become cheaper in the future, is used for the light projecting element. Furthermore, the light receiving means
By using a CCD array, etc., it is possible to configure any distance measurement field of view.
第1図は本発明に関わる測距の原理を示す図
面、第2図は受光素子で受けた信号を処理する、
本発明の評価回路の一実施例の回路図、第3図は
ライン29〜32の各々の信号波形図、第4図は
鏡筒係止装置の一実施例の図面である。
1〜4……帰還抵抗、5〜8……交流増幅器、
9〜12……同期検波回路、13〜16……ピー
ク検出回路、17〜20……タイマー回路、21
〜24……ANDゲート、25……NORゲート、
26……電流制限用抵抗、27……トランジス
タ、28……マグネツトのコイル。
Fig. 1 is a diagram showing the principle of distance measurement related to the present invention, and Fig. 2 is a diagram showing the processing of the signal received by the light receiving element.
FIG. 3 is a circuit diagram of an embodiment of the evaluation circuit of the present invention, FIG. 3 is a signal waveform diagram of each of lines 29 to 32, and FIG. 4 is a diagram of an embodiment of the lens barrel locking device. 1-4...Feedback resistor, 5-8...AC amplifier,
9-12... Synchronous detection circuit, 13-16... Peak detection circuit, 17-20... Timer circuit, 21
~24...AND gate, 25...NOR gate,
26... Current limiting resistor, 27... Transistor, 28... Magnet coil.
Claims (1)
光を前記光源から所定の基線長離れた位置にある
受光素子にて受光し、該受光信号に基づいて距離
に依存する測距信号を得る測距装置において、 方向の異なる複数の目標に向けて光を順次走査
させて投射する投光手段と、複数の異なる測距視
野からの前記投光手段により投射された光の反射
光を受光し、各視野からの上記反射光に応じた受
光信号をそれぞれ独立に出力する受光手段と、各
受光信号をそれぞれ測距視野に対応して、それぞ
れ異なる時間遅延させて出力する遅延回路と、各
受光信号に対する前記遅延出力のうち最も早く出
力された遅延出力に基づいてピント調定を行なう
ピント調定手段とを有することを特徴とする測距
装置。[Scope of Claims] 1. Light is projected from a light source toward a target, the reflected light is received by a light receiving element located a predetermined baseline length away from the light source, and distance dependent based on the received light signal. A distance measuring device that obtains a distance measurement signal that includes a light projection means that sequentially scans and projects light toward a plurality of targets in different directions, and a light projection means that projects light from a plurality of different distance measurement fields of view. a light receiving means for receiving the reflected light from each field of view and independently outputting a light reception signal corresponding to the reflected light from each field of view, and outputting each light reception signal with a different time delay corresponding to the distance measurement field of view. 1. A distance measuring device comprising: a delay circuit; and a focus adjustment means for performing focus adjustment based on the earliest output of the delay outputs for each light reception signal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19071181A JPS5893040A (en) | 1981-11-30 | 1981-11-30 | Range finder for camera |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19071181A JPS5893040A (en) | 1981-11-30 | 1981-11-30 | Range finder for camera |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5893040A JPS5893040A (en) | 1983-06-02 |
| JPH0547815B2 true JPH0547815B2 (en) | 1993-07-19 |
Family
ID=16262557
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19071181A Granted JPS5893040A (en) | 1981-11-30 | 1981-11-30 | Range finder for camera |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5893040A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0616147B2 (en) * | 1986-03-26 | 1994-03-02 | チノン株式会社 | camera |
| US5249013A (en) * | 1990-07-23 | 1993-09-28 | Ricoh Company, Ltd. | Distance measuring device of camera |
| JP3091243B2 (en) * | 1991-02-04 | 2000-09-25 | オリンパス光学工業株式会社 | Multi-point distance measuring device |
| JPH0886641A (en) * | 1994-09-16 | 1996-04-02 | Olympus Optical Co Ltd | Light emitting and receiving type focus detector |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55146425A (en) * | 1979-05-01 | 1980-11-14 | Kyocera Corp | Automatic focus control unit |
| JPS5657012A (en) * | 1979-10-16 | 1981-05-19 | Canon Inc | Distance detecting optical system |
-
1981
- 1981-11-30 JP JP19071181A patent/JPS5893040A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5893040A (en) | 1983-06-02 |
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