JPS6231844Y2 - - Google Patents

Info

Publication number
JPS6231844Y2
JPS6231844Y2 JP510981U JP510981U JPS6231844Y2 JP S6231844 Y2 JPS6231844 Y2 JP S6231844Y2 JP 510981 U JP510981 U JP 510981U JP 510981 U JP510981 U JP 510981U JP S6231844 Y2 JPS6231844 Y2 JP S6231844Y2
Authority
JP
Japan
Prior art keywords
light
light source
distance
receiving element
subject
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
JP510981U
Other languages
Japanese (ja)
Other versions
JPS57118312U (en
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 filed Critical
Priority to JP510981U priority Critical patent/JPS6231844Y2/ja
Publication of JPS57118312U publication Critical patent/JPS57118312U/ja
Application granted granted Critical
Publication of JPS6231844Y2 publication Critical patent/JPS6231844Y2/ja
Expired legal-status Critical Current

Links

Landscapes

  • Measurement Of Optical Distance (AREA)

Description

【考案の詳細な説明】 本考案は距離検出装置に関するもので、特に赤
外発光ダイオード等の発光素子の光を被写体に投
射し、その反射光量が被写体距離の二乗に反比例
することに着目し、受光素子に入射する反射光の
強弱により被写体距離を検知し、撮影レンズの焦
点合せを行う方式の距離検出装置に関するもので
ある。
[Detailed description of the invention] The present invention relates to a distance detection device, and focuses on the fact that light from a light emitting element such as an infrared light emitting diode is projected onto a subject, and the amount of reflected light is inversely proportional to the square of the subject distance. The present invention relates to a distance detection device that detects a subject distance based on the intensity of reflected light incident on a light receiving element and focuses a photographic lens.

上記の様な距離検出装置は、反射光量が被写体
距離によつて変ることは前述の通りであるが被写
体自身の反射率によつても左右されるため精度の
よい測距を行うことが出来ないと云う欠点を有し
ていた。この欠点を補うため基線距離計方式の考
え方を併用して測距精度の向上を計つたものも提
案されている。
As mentioned above, the amount of reflected light varies depending on the distance to the subject, but it also depends on the reflectance of the subject itself, so distance detection devices such as the one described above cannot perform accurate distance measurements. It had the following drawbacks. In order to compensate for this drawback, some methods have been proposed that combine the idea of the baseline distance meter method to improve distance measurement accuracy.

しかしながらこの様な装置を小型カメラに内蔵
する場合、あまり長い基線距離を取ることは出来
ないため、受光素子面における反射光の結像位置
のずれが被写体距離の変化に応じて顕著に現われ
ず充分な基線効果を挙げることが出来なかつた。
However, when such a device is built into a small camera, it is not possible to have a very long baseline distance, so it is sufficient that the shift in the imaging position of the reflected light on the light receiving element surface does not become noticeable as the subject distance changes. No significant baseline effect could be found.

このため光源の大きさを小さくすると共に受光
素子面積も小さくして基線効果を上げ、更に発光
強度の高い素子を用い、僅かな位置ずれでも受光
量に明確な差が出る様にする必要があるが、この
様な素子は価格が高いだけでなく消費電気量も多
く、小型カメラ等に内蔵する距離検出装置には適
さないものであつた。
For this reason, it is necessary to reduce the size of the light source and the area of the light-receiving element to increase the baseline effect, and to use elements with high emission intensity so that even a slight positional shift can make a clear difference in the amount of light received. However, such an element is not only expensive but also consumes a large amount of electricity, making it unsuitable for a distance detection device built into a small camera or the like.

本考案は上記の様な欠点を解消し、正確な測距
を行い得る距離検出装置を提供することを目的と
し、光源の発光部の周辺に反射面を斜設して、被
写体上に投射される光源の像の周辺部におけるエ
ネルギー密度を高めると共に、受光素子の周辺部
形状を光源の周辺部形状に一致させて受光面上の
結像位置の僅かなずれによつても受光量に明確な
差が生じ基線効果を高め得る様に構成した。
The purpose of this invention is to eliminate the above-mentioned drawbacks and provide a distance detection device that can perform accurate distance measurement.The purpose of this invention is to provide a distance detection device that can perform accurate distance measurement. In addition to increasing the energy density at the periphery of the image of the light source, the shape of the periphery of the light-receiving element is made to match that of the light source, so that even a slight shift in the image formation position on the light-receiving surface can result in a clear change in the amount of light received. It was designed so that a difference could be generated and the baseline effect could be enhanced.

以下本考案を実施例について説明する。 The present invention will be described below with reference to embodiments.

第1図は本考案装置の配置を示すもので、1は
例えばSPCの様な受光素子、2は赤外発光ダイオ
ード等の発光光源、3は受光素子の前面に配置さ
れた受光用集光レンズ、4は光源2の前面に配置
された投光用集光レンズで、受光用集光レンズ3
とは基線距離L隔てて配置され、これらは投光用
光軸と受光用光軸とがある距離(例えば2m)で
交差する様固定配置されているものとする。
Figure 1 shows the arrangement of the device of the present invention, where 1 is a light receiving element such as an SPC, 2 is a light emitting source such as an infrared light emitting diode, and 3 is a light receiving condenser lens placed in front of the light receiving element. , 4 is a condensing lens for projecting light arranged in front of the light source 2, and condensing lens 3 for receiving light is arranged in front of the light source 2.
are arranged at a baseline distance L apart from each other, and these are fixedly arranged so that the light emitting optical axis and the light receiving optical axis intersect at a certain distance (for example, 2 m).

5は距離aにおける受光範囲、6は同距離にあ
る被写体上に投光された光源の像で、51,5
2,53及び61,62,63は各距離において
変化する状態を示すものである。
5 is the light receiving range at distance a, 6 is the image of the light source projected onto the subject at the same distance, 5 1 , 5
2 , 5 3 and 6 1 , 6 2 , 6 3 indicate states that change at each distance.

第2図は光源の一例を示すもので第3図はその
詳細を示す断面図である。図に於て24は発光ダ
イオードのN型層、25はP型層で、金属ステム
部21に設けた凹みの底部にN型層が接して設け
られ、その周囲は底面に対し約45゜傾いた斜面2
1aによつて囲まれており、該ダイオードからの
光は矢印で示す様に斜面21aで反射して前方へ
向う様になつている。22はP型層25とリード
線23を介して接続されたリードフレームを示
す。
FIG. 2 shows an example of the light source, and FIG. 3 is a sectional view showing its details. In the figure, 24 is an N-type layer of the light emitting diode, and 25 is a P-type layer.The N-type layer is provided in contact with the bottom of the recess provided in the metal stem portion 21, and the periphery thereof is inclined at approximately 45 degrees with respect to the bottom surface. slope 2
1a, and the light from the diode is reflected by the slope 21a and directed forward as shown by the arrow. Reference numeral 22 indicates a lead frame connected to the P-type layer 25 via lead wires 23.

第4図は上記光源2からの光が集光レンズ4に
よつて投射された時の被写体上の像を示すもの
で、発光部の像6aの周りに前記反射面により高
照度の像6bが出来る。この時の照射エネルギー
の強度分布は第5図の線図の様になる。図におい
てハツチングを施した部分は反射面を持たない発
光ダイオードのエネルギーの強度分布を参考のた
めに示したものである。
FIG. 4 shows an image on the subject when the light from the light source 2 is projected by the condensing lens 4, and a high-intensity image 6b is formed by the reflective surface around the image 6a of the light emitting part. I can do it. The intensity distribution of the irradiation energy at this time is as shown in the diagram in FIG. The hatched area in the figure shows the energy intensity distribution of a light emitting diode without a reflective surface for reference.

第6図は上記投光像6からの反射光が集光レン
ズ3によつて受光素子1の受光面上に結像した状
態を示す。
FIG. 6 shows a state in which the reflected light from the projected image 6 is imaged on the light-receiving surface of the light-receiving element 1 by the condenser lens 3.

図に於て1aは受光面、6は該受光面上の光源
の像を示す。
In the figure, 1a indicates a light receiving surface, and 6 indicates an image of a light source on the light receiving surface.

第1図に61で示す様な極めて近い距離に被写
体がある時は像6からの反射光は受光面1aの外
にあるが、被写体が僅か遠距離側へ移動すると、
受光素子上の像6′は第6図矢印A方向に移動
し、受光面1aの一部に像6′が入る。この時
6′Aとして示す様に受光面積は小さいが前記の
様に照射エネルギー密度の高い周辺部分が近距離
で反射するため受光量としては極めて高い。被写
体が更に遠距離になると像6′が6′Bで示す様に
受光面1a内に入り受光面積は増大するが、反射
光量が距離の自乗に反比例して減少するため像
6′が受光面の右端に一致するまで受光量は徐々
に減少する。被写体が更に遠距離側へ移動すると
6′Cで示す様に像6′の外周部が受光面1aから
外れる。この時距離の二乗に反比例する反射光量
の減少と相俟つて高照度部からの光が入射しなく
なるため受光素子の受光量は急激に低下する。こ
の距離を境にして近距離と遠距離とを受光素子の
出力から判別する様に構成することにより被写体
の反射率等の差に拘らず距離の検出は明確に行わ
れる。
When the subject is at a very close distance as shown by 61 in Figure 1, the reflected light from the image 6 is outside the light receiving surface 1a, but when the subject moves slightly to the far side,
The image 6' on the light-receiving element moves in the direction of arrow A in FIG. 6, and the image 6' enters a part of the light-receiving surface 1a. At this time, as shown by 6'A, the light-receiving area is small, but the amount of light received is extremely high because the peripheral portion where the irradiation energy density is high is reflected at a short distance as described above. When the subject becomes further away, the image 6' enters the light-receiving surface 1a as shown by 6'B, and the light-receiving area increases, but the amount of reflected light decreases in inverse proportion to the square of the distance, so the image 6' becomes the light-receiving surface. The amount of received light gradually decreases until it matches the right edge of . When the subject moves further away, the outer periphery of the image 6' moves away from the light-receiving surface 1a, as shown by 6'C. At this time, the amount of reflected light decreases in inverse proportion to the square of the distance, and the light from the high-illuminance area no longer enters, so the amount of light received by the light receiving element rapidly decreases. By configuring the camera to distinguish between short distance and long distance based on the output of the light-receiving element using this distance as a boundary, distance can be clearly detected regardless of the difference in reflectance of the subject.

この様な急激な変化を生じさせるために境界に
於て投光線と受光範囲の輪廓とが一致する様に発
光素子と受光素子の形状寸法及び集光レンズの焦
点距離を定める。
In order to produce such a rapid change, the dimensions of the light emitting element and the light receiving element and the focal length of the condensing lens are determined so that the light emitting line and the contour of the light receiving range coincide at the boundary.

本実施例に於ては光源の外形を円形にし、受光
面の端部は該光源の像に適合する円弧状にした
が、第7図及び第8図は、光源の外形を直線状に
した実施例を示す。第7図に於て24′,25′は
前述と同様発光ダイオードでその両側には斜面2
1′aが設けられている。21′は金属ステム部、
22′はリードフレーム、23′はリード線を示
す。第8図は被写体上の投光像を示すもので、発
光部像6″aの両側には高照度部6bが生ずる。
In this embodiment, the light source had a circular shape, and the end of the light receiving surface was shaped like an arc to fit the image of the light source, but in FIGS. 7 and 8, the light source had a straight shape. An example is shown. In Fig. 7, 24' and 25' are light emitting diodes as mentioned above, and on both sides there are two slopes.
1'a is provided. 21' is a metal stem part,
22' is a lead frame, and 23' is a lead wire. FIG. 8 shows a projected image on a subject, in which high-illuminance areas 6b appear on both sides of the light-emitting part image 6''a.

この場合受光範囲5′が二点鎖線で示す形状と
なる様に受光面の形状寸法を設定することは前述
の実施例と同様である。
In this case, the shape and dimensions of the light-receiving surface are set so that the light-receiving range 5' has the shape shown by the two-dot chain line, as in the previous embodiment.

本考案は上述の様に光源からの光を集光レンズ
を介して被写体に照射し、その反射光を一定の基
線距離隔てて配置された集光レンズを介して受光
素子で受けて、その光量により距離を検出する方
式の距離検出装置に於て、光源の発光部の近傍に
該発光部からの光を被写体側へ向わせる反射面を
設けて被写体上に投射される光源の像の端部に高
照度部を生じさせ、受光面端部を前記集光レンズ
によつて再結像する光源の像と一致する様に形成
したので、受光面上の像の僅かなずれによつて受
光量に急激な変化を生じさせ精確な距離検出が可
能となる。
As mentioned above, the present invention irradiates light from a light source onto a subject through a condensing lens, and receives the reflected light by a light receiving element through a condensing lens placed a certain baseline distance apart. In a distance detection device that detects distance by A high-illuminance area is created in the area, and the edge of the light-receiving surface is formed to match the image of the light source that is re-imaged by the condensing lens. Accurate distance detection is possible by causing a sudden change in the amount.

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

第1図は本考案装置の光学的配置図、第2図は
光源の一例を示す斜視図、第3図は同光源の断面
図、第4図は被写体上に投射された光源の像を示
す説明図、第5図は光源の照射エネルギー分布を
示す線図、第6図は受光面と光源像との関係を示
す説明図、第7図は光源の他の実施例を示す斜視
図、第8図は同光源の投射像を示す説明図であ
る。 1;受光素子、1a;受光面、2;光源、3,
4;集光レンズ、21a,21′a;反射面、2
4,25;発光部。
Fig. 1 is an optical layout diagram of the device of the present invention, Fig. 2 is a perspective view showing an example of a light source, Fig. 3 is a sectional view of the same light source, and Fig. 4 is an image of the light source projected onto a subject. 5 is a diagram showing the irradiation energy distribution of the light source, FIG. 6 is an explanatory diagram showing the relationship between the light receiving surface and the light source image, and FIG. 7 is a perspective view showing another embodiment of the light source. FIG. 8 is an explanatory diagram showing a projected image of the same light source. 1; Light receiving element, 1a; Light receiving surface, 2; Light source, 3,
4; Condenser lens, 21a, 21'a; Reflective surface, 2
4,25; Light emitting part.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 一定の基線距離隔てて配置された光源と受光素
子とを有し、集光レンズを介して被写体に投射さ
れた光源像からの反射光を集光レンズを介して受
光素子で受けて、その受光量により距離を検出す
る方式の距離検出装置において、光源の発光部の
側方に反射面を斜設して被写体上の光源像の端部
に高照度部を生じさせる様にすると共に、受光素
子の受光面の端部を該受光素子上に再結像する上
記光源像の高照度部と一致する形状にしたことを
特徴とする距離検出装置。
It has a light source and a light-receiving element arranged at a certain baseline distance apart, and the light-receiving element receives the reflected light from the light source image projected onto the subject through the condenser lens, and receives the light. In a distance detection device that detects distance based on the amount of light, a reflective surface is provided obliquely on the side of the light emitting part of the light source to create a high-illuminance area at the end of the light source image on the subject, and a light receiving element A distance detecting device characterized in that an end of the light receiving surface of the light receiving element is shaped to match a high illuminance part of the light source image re-imaged onto the light receiving element.
JP510981U 1981-01-17 1981-01-17 Expired JPS6231844Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP510981U JPS6231844Y2 (en) 1981-01-17 1981-01-17

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP510981U JPS6231844Y2 (en) 1981-01-17 1981-01-17

Publications (2)

Publication Number Publication Date
JPS57118312U JPS57118312U (en) 1982-07-22
JPS6231844Y2 true JPS6231844Y2 (en) 1987-08-15

Family

ID=29803495

Family Applications (1)

Application Number Title Priority Date Filing Date
JP510981U Expired JPS6231844Y2 (en) 1981-01-17 1981-01-17

Country Status (1)

Country Link
JP (1) JPS6231844Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0711624B2 (en) * 1990-11-13 1995-02-08 チノン株式会社 Ranging device

Also Published As

Publication number Publication date
JPS57118312U (en) 1982-07-22

Similar Documents

Publication Publication Date Title
JPS6130689B2 (en)
JPH0714810Y2 (en) Rangefinder
JPS62174607A (en) Optical system for measuring instrument
JP2764121B2 (en) Automatic focusing device
JPS6247508A (en) Optical device for range finding
JPH046298Y2 (en)
JPH0167517U (en)
JPH0333389U (en)
JPH0325106U (en)
JPH07112050B2 (en) Optical semiconductor device
JPH0161610U (en)
JPS63105007U (en)
JPS6215511A (en) Light emitting element for automatic focus adjusting device
JPH01267601A (en) Condenser lens
JPH0360011U (en)
JPH01104507U (en)
JPH01131108U (en)
JPS6397957U (en)
JPS58138010U (en) Dimension measuring device
JPS60165855U (en) Surface inspection device for cylindrical objects
JPH0459832U (en)
JPS6323867U (en)
JPS61137006A (en) Range finder in camera
JPH01321390A (en) Detector
JPS63115746U (en)