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JP3284325B2 - Camera ranging device - Google Patents
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JP3284325B2 - Camera ranging device - Google Patents

Camera ranging device

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Publication number
JP3284325B2
JP3284325B2 JP21156893A JP21156893A JP3284325B2 JP 3284325 B2 JP3284325 B2 JP 3284325B2 JP 21156893 A JP21156893 A JP 21156893A JP 21156893 A JP21156893 A JP 21156893A JP 3284325 B2 JP3284325 B2 JP 3284325B2
Authority
JP
Japan
Prior art keywords
light
projecting
distance
circuit
receiving
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 - Fee Related
Application number
JP21156893A
Other languages
Japanese (ja)
Other versions
JPH0763983A (en
Inventor
顕 伊藤
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.)
Seiko Precision Inc
Original Assignee
Seiko Precision 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 Seiko Precision Inc filed Critical Seiko Precision Inc
Priority to JP21156893A priority Critical patent/JP3284325B2/en
Publication of JPH0763983A publication Critical patent/JPH0763983A/en
Application granted granted Critical
Publication of JP3284325B2 publication Critical patent/JP3284325B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Automatic Focus Adjustment (AREA)
  • Measurement Of Optical Distance (AREA)
  • Focusing (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】この発明は、被写体に照射光を投
光して距離信号を得る、いわゆるアクティブ型のカメラ
用測距装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a so-called active type camera distance measuring device for projecting irradiation light onto a subject to obtain a distance signal.

【0002】[0002]

【従来の技術】三角測量法を用いた測距装置において、
被写体上の反射強度のムラや、被写体の縁に投光ビーム
の一部が当たっているときに生じる受光スポットの重心
位置のずれ(以下これを不均一照射という)による距離
検出誤差を補正する方法として、たとえば特開昭63−
235909号公報や特開平5−52557号公報に開
示されているように、投光素子を1つ、受光素子を2つ
使ったいわゆる3眼方式が知られている。
2. Description of the Related Art In a distance measuring apparatus using a triangulation method,
A method for correcting a distance detection error due to uneven reflection intensity on a subject or a shift in the center of gravity of a light-receiving spot caused when a part of a projected light beam hits an edge of the subject (hereinafter, referred to as non-uniform irradiation). For example, JP-A-63-
As disclosed in JP-A-235909 and JP-A-5-52557, a so-called trinocular system using one light projecting element and two light receiving elements is known.

【0003】[0003]

【発明が解決しようとする課題】3眼方式のアクティブ
式測距装置では2つの受光素子が1つの投光素子の両脇
に配置されるため、通常の2眼方式の測距装置の2倍の
幅を必要とし、小型を旨とするコンパクトカメラに搭載
するにはスペース的に非常に不利になってしまう。本発
明のカメラ用測距装置では、2眼方式と同様な大きさで
3眼方式と同様な効果をあげることを目的とする。
In a three-lens type active distance measuring device, two light receiving elements are arranged on both sides of one light projecting element, so that it is twice as large as a normal two-lens type distance measuring device. This is very disadvantageous in terms of space when it is mounted on a compact camera that requires a small size. The object of the present invention is to provide a camera distance measuring apparatus having the same size as the twin-lens system and the same effect as the three-lens system.

【0004】[0004]

【課題を解決するための手段】以上の課題を解決するた
めに、本発明のカメラ用測距装置では、被写体に対し照
射光を投光する第1の投光手段と、前記投光素子から一
定の基線長を隔てて配置され前記第1の投光手段の照射
光が被写体で反射した光を受光する第1の受光手段と、
前記第1の受光手段の近傍に配置され被写体に対し照射
光を投光する第2の投光手段と、前記第1の投光手段の
近傍に配置され前記第2の投光手段の照射光が被写体で
反射した光を受光する第2の受光手段と、前記第1およ
び第2の受光手段の出力信号に基づいて被写体までの距
離信号を生成する距離信号生成手段とを有している。
In order to solve the above-mentioned problems, in a camera distance measuring apparatus according to the present invention, a first light projecting means for projecting irradiation light to an object and a light projecting device are provided. A first light receiving unit that is arranged at a fixed base line distance and receives light reflected by the subject from irradiation light of the first light projecting unit;
A second light projecting means disposed near the first light receiving means for projecting light to a subject, and an irradiation light of the second light projecting means arranged near the first light projecting means; Has a second light receiving means for receiving light reflected by the object, and a distance signal generating means for generating a distance signal to the object based on output signals of the first and second light receiving means.

【0005】また、前記距離信号生成手段は前記第1の
受光手段および前記第2の受光手段の出力信号を平均し
て距離信号を得る。
Further, the distance signal generating means obtains a distance signal by averaging output signals of the first light receiving means and the second light receiving means.

【0006】[0006]

【作用】アクティブ式の2眼の測距装置において、各レ
ンズの焦点位置に投光素子を配置し、その外側の近傍に
1次元半導体受光素子を配置する。それぞれの受光素子
は互いに他のレンズを通じて投光された投射光を受光
し、その入射位置に応じた電流をそれぞれの受光回路に
出力する。演算回路はそれぞれの受光回路の出力から距
離情報を得る。
In an active type two-lens distance measuring device, a light projecting element is arranged at a focal position of each lens, and a one-dimensional semiconductor light receiving element is arranged near the outside of the lens. Each light receiving element receives the projected light projected through another lens, and outputs a current corresponding to the incident position to each light receiving circuit. The arithmetic circuit obtains distance information from the output of each light receiving circuit.

【0007】[0007]

【実施例】本発明の一実施例を図1から図4に基づいて
説明する。測距動作に先だって演算回路(以下CPUと
いう)1は投光回路2および受光回路10、20の電源
をオンし、続いて投光回路2にデジタルパルス列からな
る投光信号を出力する。投光回路2はこの投光信号に従
って、2つの近赤外発光素子(以下IREDという)1
1、21とを所定の条件(たとえば周期2ミリ秒、発光
デューティー5%)で交互に駆動する。IRED11と
1次元半導体受光素子(以下PSDという)13、IR
ED21とPSD23はそれぞれ図3のように2つの発
光部が同一のプラスチックパッケージ14にモールドさ
れているのがもっとも望ましいが、IRED11とPS
D13とを近接して配置してもよい。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described with reference to FIGS. Prior to the distance measurement operation, an arithmetic circuit (hereinafter referred to as a CPU) 1 turns on the power of the light emitting circuit 2 and the light receiving circuits 10 and 20, and subsequently outputs a light emitting signal composed of a digital pulse train to the light emitting circuit 2. The light emitting circuit 2 receives two near-infrared light emitting elements (hereinafter referred to as IRED) 1 according to the light emitting signal.
1 and 21 are alternately driven under predetermined conditions (for example, a cycle of 2 milliseconds and a light emission duty of 5%). IRED 11, one-dimensional semiconductor light receiving element (hereinafter referred to as PSD) 13, IR
It is most desirable that the ED 21 and the PSD 23 each have two light emitting parts molded in the same plastic package 14 as shown in FIG.
D13 may be arranged in close proximity.

【0008】IRED21から投光された赤外光はレン
ズ22で集められ、被写体3に投光される。被写体3に
よって反射された光はレンズ12で再び集められPSD
13上でビーム像13aとして結像する。PSD13は
入射光の結像位置に対応した信号光電流IN1およびI
F1を出力する。信号光電流IN1は定常光電流抜き取
り回路15aで定常光電流成分を抜き取られ、対数圧縮
回路16aで対数圧縮され、電流増幅回路17aで増幅
された後、演算器18に入力される。信号光電流IF1
も定常光電流抜き取り回路15b、電流増幅回路17
b、対数圧縮回路16bにおいて同様な処理を施され演
算器18に入力される。演算器18は信号光電流IN1
とIF1とから式(1)に示される電圧V1を平均化回
路4に出力する。ここでVcは所定の電圧である。
The infrared light projected from the IRED 21 is collected by the lens 22 and projected on the subject 3. The light reflected by the subject 3 is collected again by the lens 12 and
An image is formed on the light beam 13 as a beam image 13a. The PSD 13 has signal light currents IN1 and I1 corresponding to the imaging position of the incident light.
Output F1. The signal light current IN1 is extracted from the stationary light current extracting circuit 15a by the stationary light current component, is logarithmically compressed by the logarithmic compression circuit 16a, is amplified by the current amplifier circuit 17a, and is input to the arithmetic unit 18. Signal light current IF1
Also the steady photocurrent extraction circuit 15b and the current amplification circuit 17
(b) Similar processing is performed in the logarithmic compression circuit 16b, and the result is input to the arithmetic unit 18. The arithmetic unit 18 outputs the signal light current IN1
And IF1 to output the voltage V1 shown in equation (1) to the averaging circuit 4. Here, Vc is a predetermined voltage.

【0009】 V1=Vc・IF1/(IN1+IF1) (1) 電圧V1は、図5に示したように、PSDの基線長方向
の長さをL、隣接PSD方向の一端からビーム像の中心
までの距離をX1、端子TC1から供給される電流を電
流I1とすると、次の式(2)で表される。ここでcは
電気抵抗の次元をもつ比例定数である。
V1 = Vc · IF1 / (IN1 + IF1) (1) As shown in FIG. 5, the voltage V1 is L, the length of the PSD in the base line length direction, and from one end in the adjacent PSD direction to the center of the beam image. Assuming that the distance is X1 and the current supplied from the terminal TC1 is the current I1, it is expressed by the following equation (2). Here, c is a proportional constant having a dimension of electric resistance.

【0010】 V1=c・(X1/L)・I1 (2) 以上はIRED21から赤外光を投光した場合である
が、IRED11から投光した場合もまったく同様で、
PSD23でビーム像23aのように結像し、信号光電
流IN2およびIF2として出力され、信号光電流IN
2は定常光電流抜き取り回路25aで定常光電流成分を
抜き取られ、対数圧縮回路26aで対数圧縮され、電流
増幅回路27aで増幅された後、演算器28に入力され
る。信号光電流IF2も定常光電流抜き取り回路25
b、電流増幅回路27b、対数圧縮回路26bにおいて
同様な処理を施され演算器28に入力される。演算器2
8は信号光電流IN2とIF2とから式(3)に示され
るとなる電圧V2を平均化回路4に出力する。
V1 = c · (X1 / L) · I1 (2) The above is the case where the infrared light is projected from the IRED 21, but the case where the infrared light is projected from the IRED 11 is exactly the same.
The image is formed by the PSD 23 as a beam image 23a, and is output as the signal light current IN2 and IF2.
2, the stationary photocurrent component is extracted by a stationary photocurrent extraction circuit 25a, logarithmically compressed by a logarithmic compression circuit 26a, amplified by a current amplification circuit 27a, and input to an arithmetic unit 28. The signal light current IF2 is also a steady light current extraction circuit 25.
b, the same process is performed in the current amplification circuit 27b and the logarithmic compression circuit 26b, and the result is input to the arithmetic unit 28. Arithmetic unit 2
8 outputs to the averaging circuit 4 a voltage V2 represented by Expression (3) from the signal light currents IN2 and IF2.

【0011】 V2=Vc・IF2/(IN2+IF2) (3) 電圧V2もまた電圧V1と同様に、隣接PSD方向の一
端からビーム像の中心までの距離をX2、端子TC2か
ら供給される電流を電流I2として、次の式(4)のよ
うに表される。
V2 = Vc · IF2 / (IN2 + IF2) (3) Similarly to the voltage V1, the voltage V2 is the distance from one end in the adjacent PSD direction to the center of the beam image, and the current supplied from the terminal TC2 is the current. I2 is represented by the following equation (4).

【0012】 V2=c・(X2/L)・I2 (4) 平均化回路4は電圧V1とV2とを式(5)のように平
均する回路である。
V2 = c · (X2 / L) · I2 (4) The averaging circuit 4 is a circuit for averaging the voltages V1 and V2 as in equation (5).

【0013】 V0=(V1+V2)/2 (5) 投光回路2はIRED11とIRED21とを交互に駆
動し、その度にCPU1はA/Dコンバータ(以下AD
Cという)5で平均化回路4の出力電圧V0を検出す
る。この電圧V0によって一義的に定まるメモリ1aの
距離テーブルから、被写体までの距離Dを求めることが
できる。もし不均一照射が生じていなければ電圧V1と
V2はほぼ同じ電圧であり、これらの平均電圧V0もま
た電圧V1およびV2にほぼ等しいと考えてよい。
V0 = (V1 + V2) / 2 (5) The light projecting circuit 2 drives the IRED 11 and the IRED 21 alternately, and each time the CPU 1 operates the A / D converter (hereinafter referred to as an AD converter).
At C5, the output voltage V0 of the averaging circuit 4 is detected. From the distance table in the memory 1a uniquely determined by the voltage V0, the distance D to the subject can be obtained. If non-uniform irradiation has not occurred, the voltages V1 and V2 are substantially the same voltage, and the average voltage V0 may also be considered to be substantially equal to the voltages V1 and V2.

【0014】ここで不均一照射の生じていた場合につい
て、図6および図7に従って説明する。図4および図5
と同一物には同一の符号を付してある。図6ではIRE
Dからの投射光が被写体となっている人物の一部分にし
か照射されず、従って被写体からの反射光も円弧の一部
のみの状態である。以下この状態を「ビーム欠け」とい
う。ビーム欠けを生じるとPSD上の像も円弧の一部と
なり、光重心が移動して誤測距の原因となる。図7は図
6のPSD13とPSD23の部分を拡大したもので、
PSD13では値Δx1だけ遠距離側に、PSD23で
は値Δx2だけ近距離側にビームがずれていることがわ
かる。つまり、式(6)と式(7)とが成り立つ。
Here, the case where uneven irradiation has occurred will be described with reference to FIGS. 4 and 5
The same components as those described above are denoted by the same reference numerals. In FIG. 6, IRE
The projection light from D is radiated only to a part of the person who is the subject, so that the reflected light from the subject is also only a part of the arc. Hereinafter, this state is referred to as “beam missing”. When the beam is chipped, the image on the PSD also becomes a part of the arc, and the center of gravity of the light shifts to cause erroneous distance measurement. FIG. 7 is an enlarged view of PSD13 and PSD23 in FIG.
It can be seen that the beam is shifted to the far side by the value Δx1 in the PSD 13 and to the near side by the value Δx2 in the PSD 23. That is, Expression (6) and Expression (7) hold.

【0015】 V1=c・(X−ΔX1)/L・I1 (6) V2=c・(X+ΔX2)/L・I2 (7) これらを平均した電圧V0は、式(8)のようになる。V1 = c · (X−ΔX1) / L · I1 (6) V2 = c · (X + ΔX2) / L · I2 (7) A voltage V0 obtained by averaging these is given by equation (8).

【0016】 V0=c・((X−ΔX1)・I1+(X+ΔX2)・I2)/L (8) ここで、基線長Bに対して被写体が十分に大きい場合、
被写体へのビームの照射量はおよそ等しく、PSD13
とPSD23上にはほぼ同じ強度、ほぼ同じ形状の像が
描かれることになる。したがって値Δx1と値Δx2と
はほぼ等しく、また光強度がほぼ同じという点から電流
I1と電流I2もほぼ等しい。以上から式(8)の値Δ
x1と値Δx2の項が相殺されるため、式(8)は式
(5)とほぼ等しく、ビーム欠けの影響は消えることが
わかる。
V0 = c · ((X−ΔX1) · I1 + (X + ΔX2) · I2) / L (8) Here, when the subject is sufficiently large with respect to the base line length B,
The beam irradiation amount to the subject is approximately equal, and PSD13
Thus, an image having substantially the same intensity and substantially the same shape is drawn on the PSD 23. Therefore, the value Δx1 is substantially equal to the value Δx2, and the currents I1 and I2 are also substantially equal in that the light intensity is substantially the same. From the above, the value Δ of equation (8)
Since the term of x1 and the value Δx2 are canceled out, Expression (8) is almost equal to Expression (5), and it can be seen that the influence of the beam missing disappears.

【0017】以上に示すように、本発明のカメラ用測距
装置は1つの投光素子と1つの受光素子からなる一対の
光学系を2つ持った、2組の投受光素子の系から構成さ
れており、一方の光学系の投光素子がオンする時は他方
の光学系の受光素子はオフするように駆動される。2つ
の投光素子を所定回数にわたって交互に駆動し、平均化
回路4に式(5)の演算を行わせることでビーム欠けの
影響を取り除き、正しく被写体までの距離Dを求めるこ
とができる。この距離Dに従ってCPU1はモータ6を
駆動し撮影レンズ鏡筒7を適正な位置まで移動させる。
As described above, the range finder for a camera according to the present invention comprises two pairs of light emitting and receiving elements having two optical systems each including one light emitting element and one light receiving element. When the light emitting element of one optical system is turned on, the light receiving element of the other optical system is driven to be turned off. By driving the two light emitting elements alternately a predetermined number of times and causing the averaging circuit 4 to perform the calculation of the equation (5), the influence of the beam missing can be removed, and the distance D to the subject can be correctly obtained. The CPU 1 drives the motor 6 according to the distance D to move the photographing lens barrel 7 to an appropriate position.

【0018】この例ではビーム欠けの場合についてのみ
示したが、一般的な不均一照射の場合でも同様にその影
響を少なくできることは自明である。
In this example, only the case where the beam is missing is shown. However, it is obvious that the influence can be similarly reduced in the case of general non-uniform irradiation.

【0019】また、本実施例では不均一照射の発生を撮
影者が知ることはできないが、ブザーやランプなどの報
知手段を付加して不均一照射の発生を撮影者に対し報知
するようにしてもよい。
Further, in this embodiment, the photographer cannot know the occurrence of the non-uniform irradiation. However, a notifying means such as a buzzer or a lamp is added to notify the photographer of the occurrence of the non-uniform irradiation. Is also good.

【0020】さらに本実施例では常に不均一照射の補正
を行うようになっているが、不均一照射の影響がわずか
な場合に、補正演算の誤差によってかえって測距結果の
誤差を増やしてしまうのを避けるために、不均一照射の
影響が所定値以下の場合に測距結果の補正を禁止するよ
うにしてもよい。
Further, in the present embodiment, the correction of the non-uniform irradiation is always performed. However, when the influence of the non-uniform irradiation is slight, the error of the distance measurement result is increased by the error of the correction calculation. In order to avoid this, correction of the distance measurement result may be prohibited when the influence of the non-uniform irradiation is equal to or less than a predetermined value.

【0021】[0021]

【発明の効果】不均一照射時の対策を2眼方式で実現し
たため、3眼方式のように基線長を長くする必要がな
く、もってカメラの小型化に寄与する。
According to the present invention, since the countermeasure for non-uniform irradiation is realized by the two-lens system, it is not necessary to increase the base line length unlike the three-lens system, thereby contributing to downsizing of the camera.

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

【図1】本発明の実施例を示すブロック図である。FIG. 1 is a block diagram showing an embodiment of the present invention.

【図2】従来例を示すブロック図である。FIG. 2 is a block diagram showing a conventional example.

【図3】本発明の実施例に使用される投光素子と受光素
子の配置の一例である。
FIG. 3 is an example of an arrangement of a light emitting element and a light receiving element used in an embodiment of the present invention.

【図4】本発明の実施例においてビーム欠けが生じてい
ない場合の説明図である。
FIG. 4 is an explanatory diagram in a case where a beam is not chipped in the embodiment of the present invention.

【図5】図4において受光素子の部分の拡大図である。FIG. 5 is an enlarged view of a light receiving element in FIG.

【図6】本発明の実施例においてビーム欠けが生じた場
合の説明図である。
FIG. 6 is an explanatory diagram in a case where a beam break occurs in the embodiment of the present invention.

【図7】図6において受光素子の部分の拡大図である。FIG. 7 is an enlarged view of a light receiving element in FIG.

【符号の説明】[Explanation of symbols]

11 IRED(第1の投光手段) 13 PSD(第1の受光手段) 21 IRED(第2の投光手段) 23 PSD(第2の受光手段) 1 CPU(距離信号生成手段) 11 IRED (first light emitting means) 13 PSD (first light receiving means) 21 IRED (second light emitting means) 23 PSD (second light receiving means) 1 CPU (distance signal generating means)

───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) G02B 7/32 G03B 13/36 ──────────────────────────────────────────────────続 き Continued on front page (58) Field surveyed (Int.Cl. 7 , DB name) G02B 7/32 G03B 13/36

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 被写体に対し照射光を投光する第1の投
光素子と、前記投光素子から一定の基線長を隔てて配置
され前記第1の投光素子の照射光が被写体で反射した光
を受光する第1の受光素子と、前記第1の受光素子の近
傍に配置され被写体に対し照射光を投光する第2の投光
素子と、前記第1の投光素子の近傍に配置され前記第2
の投光素子の照射光が被写体で反射した光を受光する第
2の受光素子と、前記第1および第2の受光素子の出力
信号に基づいて被写体までの距離信号を生成する距離信
号生成手段とを有することを特徴とするカメラ用測距装
置。
1. A first light projecting element for projecting irradiation light to a subject, and a light projecting element disposed at a predetermined base length from the light projecting element and reflected by the first projecting element. A first light-receiving element for receiving the light, a second light-emitting element disposed near the first light-receiving element and projecting irradiation light to a subject, and a second light-emitting element near the first light-emitting element. Placed in the second
A second light receiving element for receiving the light reflected by the object from the light emitted from the light projecting element, and a distance signal generating means for generating a distance signal to the object based on the output signals of the first and second light receiving elements And a distance measuring device for a camera.
【請求項2】 前記距離信号生成手段は前記第1の受光
回路および前記第2の受光回路の出力信号を平均して距
離信号を得ることを特徴とするカメラ用測距装置。
2. A distance measuring apparatus for a camera, wherein said distance signal generating means obtains a distance signal by averaging output signals of said first light receiving circuit and said second light receiving circuit.
JP21156893A 1993-08-26 1993-08-26 Camera ranging device Expired - Fee Related JP3284325B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21156893A JP3284325B2 (en) 1993-08-26 1993-08-26 Camera ranging device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21156893A JP3284325B2 (en) 1993-08-26 1993-08-26 Camera ranging device

Publications (2)

Publication Number Publication Date
JPH0763983A JPH0763983A (en) 1995-03-10
JP3284325B2 true JP3284325B2 (en) 2002-05-20

Family

ID=16607942

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21156893A Expired - Fee Related JP3284325B2 (en) 1993-08-26 1993-08-26 Camera ranging device

Country Status (1)

Country Link
JP (1) JP3284325B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2779347B2 (en) * 1996-08-05 1998-07-23 大日本印刷株式会社 Injection molding method of molded article having concave part and pictured film on the surface

Also Published As

Publication number Publication date
JPH0763983A (en) 1995-03-10

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