JPH01316618A - Optical sensor - Google Patents
Optical sensorInfo
- Publication number
- JPH01316618A JPH01316618A JP15071088A JP15071088A JPH01316618A JP H01316618 A JPH01316618 A JP H01316618A JP 15071088 A JP15071088 A JP 15071088A JP 15071088 A JP15071088 A JP 15071088A JP H01316618 A JPH01316618 A JP H01316618A
- Authority
- JP
- Japan
- Prior art keywords
- light
- angle
- incident
- incidence
- optical sensor
- 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.)
- Granted
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 20
- 230000000903 blocking effect Effects 0.000 claims description 2
- 238000005259 measurement Methods 0.000 abstract description 5
- 230000007423 decrease Effects 0.000 abstract 1
- 230000005540 biological transmission Effects 0.000 description 15
- 238000010586 diagram Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 238000001514 detection method Methods 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、各Wi機器の動作を制御したり、環境の測定
のために用いる可視光センサーや赤外線を含む光センサ
ーに関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a visible light sensor and an infrared light sensor used to control the operation of each Wi device and to measure the environment.
従来の技術
従来のこの種の光センサーは、特開昭62−26102
5号広報に示されているように、第9図のような構造に
なっていた。第9図において1は集光レンズ、2は光検
出器、3は光透過窓、4は光検出素子である。集光レン
ズ1は、光検出器2に対し垂直に入射する光はほとんど
屈折せずに透過させ、入射角の大きな光に対しては大き
く屈折させ、光検出器2に全方位からの光を入射させる
ようになっている。Prior art A conventional optical sensor of this type is disclosed in Japanese Patent Application Laid-Open No. 62-26102.
As shown in the No. 5 bulletin, the structure was as shown in Figure 9. In FIG. 9, 1 is a condenser lens, 2 is a photodetector, 3 is a light transmission window, and 4 is a photodetector element. The condensing lens 1 transmits light incident perpendicularly to the photodetector 2 without refracting it, greatly refracts light with a large angle of incidence, and transmits light from all directions to the photodetector 2. It is designed to be incident.
発明が解決しようとする課題
しかし、上記のような構成では、光透過窓3の垂直方向
から入射する光はほとんど検出される。Problems to be Solved by the Invention However, in the above configuration, most of the light incident from the vertical direction of the light transmission window 3 is detected.
−力水平方向から入射する光は集光レンズ1で曲げられ
その一部が光透過窓3に達するがその量はご(わずかし
かない。第10図は照射光量が一定のときの入射角によ
る検出光量の変化を示した図である。入射角が0度、す
なわち集光レンズの光軸上の光の検出量を100とした
場合、入射角が90度、すなわち光透過窓3の水平方向
から入射する場合は0に近い値となる。すなわち、従来
の球面で構成される凹レンズを集光レンズとして用いた
場合、検出光量の入射角依存性が高(、正確な光量測定
は極めて困難であった。本発明は上記課題に鑑み、検出
光量の入射角依存性を小さくし、より正確な測定を行え
る光センサーを提供するものである。- Light incident from the horizontal direction is bent by the condenser lens 1, and a portion of it reaches the light transmission window 3, but the amount is very small. Figure 10 shows detection based on the incident angle when the amount of irradiated light is constant. FIG. 2 is a diagram showing changes in light amount. When the incident angle is 0 degrees, that is, the detected amount of light on the optical axis of the condensing lens is 100, the incident angle is 90 degrees, that is, from the horizontal direction of the light transmission window 3. When it is incident, the value is close to 0.In other words, when a conventional concave lens composed of a spherical surface is used as a condenser lens, the amount of detected light is highly dependent on the angle of incidence (and accurate measurement of the amount of light is extremely difficult). In view of the above problems, the present invention provides an optical sensor that can reduce the dependence of the detected light amount on the angle of incidence and perform more accurate measurements.
課題を解決するための手段
上記目的を達成するために本発明の光センサーは、集光
レンズの一部に入射光を遮蔽もしくは全反射させる手段
を設けたものである。Means for Solving the Problems In order to achieve the above object, the optical sensor of the present invention is provided with means for blocking or totally reflecting incident light in a part of the condensing lens.
作 用
この構成により入射光量の多い箇所は光が遮蔽もしくは
反射されて光量が均一に光検出器に到達することとなる
。Effect: With this configuration, light is blocked or reflected at locations where there is a large amount of incident light, so that the amount of light reaches the photodetector uniformly.
実施例
以下本発明の一実施例について図面を参照しながら説明
する。第1図は本発明の第1の実施例における光センサ
ーの断面図である。同図において5は集光レンズ、6は
光検出器、7は光透過窓、8は光検出素子である。集光
レンズ5の光軸上に軸対称形をした光線遮蔽部9が位置
しており、第2図(a)に示すように、入射角が零度の
時、光線はその大部分が遮蔽部9により遮蔽され光検出
器6の光透過窓7に達しない。また、第2図(b)に示
すように45度の入射角の光線は、光透過窓7に到達す
る光線のうちの一部が遮蔽される。さらに、第2図(C
)に示すように入射角が90度の時は光線は集光レンズ
5の光源側の面で大きく屈折するため、そのほとんどが
遮蔽部9に当たらずに光透過窓7に到達する。この結果
、低入射角の光の検出量は小さ(なり、高入射角の光の
検出量は相対的に大きくなる。すなわち、入射角による
検出光量の差を小さくすることができる。EXAMPLE An example of the present invention will be described below with reference to the drawings. FIG. 1 is a sectional view of an optical sensor in a first embodiment of the present invention. In the figure, 5 is a condenser lens, 6 is a photodetector, 7 is a light transmission window, and 8 is a photodetector element. An axially symmetrical light shielding part 9 is located on the optical axis of the condensing lens 5, and as shown in FIG. 9 and does not reach the light transmission window 7 of the photodetector 6. Furthermore, as shown in FIG. 2(b), a portion of the light rays that reach the light transmission window 7 are blocked at an incident angle of 45 degrees. Furthermore, Figure 2 (C
), when the incident angle is 90 degrees, the light rays are largely refracted by the light source side surface of the condenser lens 5, so most of them reach the light transmission window 7 without hitting the shielding part 9. As a result, the detected amount of light at a low incident angle becomes small (and the detected amount of light at a high incident angle becomes relatively large). In other words, the difference in the detected light amount depending on the incident angle can be made small.
以下本発明の第2の実施例について図面を参照しながら
説明する。第3図は本発明の第2の実施例を示す光セン
サーの集光レンズの構成図である。同図において、第1
図と異なる点は集光レンズを同一の材料で作り、全反射
を利用して遮蔽物と同等の効果を得ている点である。同
図において10は集光レンズの光源側の面、11は集光
レンズの像面側の面内に位置する全反射部、12は集光
レンズの像面側の球面部である。上記のように構成され
た光センサーの集光レンズについてその機能を説明する
。第4図(a)、(b)、(c)に各入射角における光
線が光透過窓7に到達する様子を示している。入射角が
小さい時は全反射部11により光線は光透過窓7に達せ
ず、球面部12から入射した光線のみが光透過窓7に達
する。A second embodiment of the present invention will be described below with reference to the drawings. FIG. 3 is a configuration diagram of a condensing lens of an optical sensor showing a second embodiment of the present invention. In the same figure, the first
The difference from the figure is that the condenser lens is made of the same material and uses total internal reflection to achieve the same effect as a shield. In the figure, 10 is a surface of the condensing lens on the light source side, 11 is a total reflection part located within the plane of the condensing lens on the image plane side, and 12 is a spherical part on the image plane side of the condensing lens. The functions of the condensing lens of the optical sensor configured as described above will be explained. FIGS. 4(a), (b), and (c) show how light rays reach the light transmission window 7 at each incident angle. When the incident angle is small, the light rays do not reach the light transmission window 7 due to the total reflection section 11, and only the light rays incident from the spherical surface section 12 reach the light transmission window 7.
入射角が中以上の光線は第4図(b)、(c)に示すよ
うに、全反射部11と球面部12に入射する光線ともそ
のほとんどが、光透過窓7に到達する。しかも、全反射
部から入射する光線は、光透過窓7に対し球面部12か
ら入射する光線と比較して小さな入射角となって到達す
る為、検出効率が向上する。この結果、同一の材料で作
られた簡素な構造の一部レンズで入射角依存性の小さな
光センサーを実現することができる。本実施においては
、全反射部11を光軸上の一ケ所のみに設けたが、光軸
上でなくても、また、複数箇所に設けてもよい。As shown in FIGS. 4(b) and 4(c), most of the light rays having an incident angle of medium or higher reach the light transmitting window 7, including the light rays incident on the total reflection section 11 and the spherical surface section 12. Moreover, since the light beam incident from the total reflection section reaches the light transmission window 7 at a smaller angle of incidence than the light beam incident from the spherical surface section 12, the detection efficiency is improved. As a result, it is possible to realize an optical sensor with small incidence angle dependence using some lenses with a simple structure made of the same material. In this embodiment, the total reflection section 11 is provided only at one location on the optical axis, but it may be provided at multiple locations, even if not on the optical axis.
次に本発明の第3の実施例について図面を参照しながら
説明する。第5図は本発明の第3の実施例を示す光セン
サーの集光レンズである。同図において13は集光レン
ズ、14は集光レンズ13の光源側面、15は集光レン
ズ13の像面側曲面、16は集光レンズ13の像面側何
面である。Next, a third embodiment of the present invention will be described with reference to the drawings. FIG. 5 shows a condensing lens of an optical sensor showing a third embodiment of the present invention. In the figure, 13 is a condenser lens, 14 is a light source side surface of the condenser lens 13, 15 is a curved surface of the condenser lens 13 on the image plane side, and 16 is a surface of the condenser lens 13 on the image plane side.
上記のように構成された光センサーの集光レンズについ
てその機能を説明する。低入射角の光線はそのほとんど
が光源側面14と像面倒曲面15を通過する光源側面1
4と像面倒曲面15は曲率半径の小さな凹レンズを形成
しており、入射光は太き(広がって光透過窓7に当たる
量が減少する。The functions of the condensing lens of the optical sensor configured as described above will be explained. Most of the light rays at low incident angles pass through the light source side surface 14 and the image surface curved surface 15.
4 and the field surface curved surface 15 form a concave lens with a small radius of curvature, and the incident light is thick (spread) and the amount of light hitting the light transmission window 7 is reduced.
一方、高入射角の光線は光源側面14と像面側側面16
でその進行方向を太き(曲げられ、光透過窓7には低入
射角であたるようになり、光線の絶対量は少な(でも効
率よ(光量を検出することが可能となる。On the other hand, light rays with high incident angles
The traveling direction of the light beam is widened (bend) so that it hits the light transmission window 7 at a low angle of incidence, and the absolute amount of light is small (but it is possible to detect the light amount efficiently).
第6図は本発明の第4の実施例における光センサーの要
部断面図である。本実施例は第1の実施例とほぼ同じ構
成であるが、光遮蔽部17を像面側に配置した点が第1
の実施例と異なるところである。第7図、第8図は本発
明の第5.第6の実施例における光センサーの要部断面
図である。本実施例は第2の実施例と構成はほぼ同じで
あるが全反射部11に加えて、光遮蔽部18、低入射角
用平面部19を設けた点が第2の実施例と異なるところ
である。第5.第6の実施例によれば第2の実施例以上
の効果を得ることができる。なお、第8図において、2
0は側面部であり、球面を用いず、複数の面から構成さ
れておりそれぞれが入射角の異なる光線を効率的に光透
過窓7に到達するようにするものである。FIG. 6 is a sectional view of a main part of an optical sensor according to a fourth embodiment of the present invention. This embodiment has almost the same configuration as the first embodiment, but the first difference is that the light shielding part 17 is disposed on the image plane side.
This is different from the embodiment. FIGS. 7 and 8 show the fifth aspect of the present invention. FIG. 7 is a sectional view of a main part of an optical sensor in a sixth embodiment. This embodiment has almost the same configuration as the second embodiment, but differs from the second embodiment in that in addition to the total reflection section 11, a light shielding section 18 and a flat surface section 19 for low incidence angles are provided. be. Fifth. According to the sixth embodiment, more effects than the second embodiment can be obtained. In addition, in Fig. 8, 2
Reference numeral 0 denotes a side surface, which is composed of a plurality of surfaces without using a spherical surface, each of which allows light rays with different incident angles to efficiently reach the light transmission window 7.
発明の効果
以上のように本発明は、集光レンズに光遮蔽もしくは全
反射手段を設けることにより入射光量の入射角度依存性
を少なくできるので、正確な光量測定が行えることにな
る。Effects of the Invention As described above, according to the present invention, the dependence of the incident light amount on the angle of incidence can be reduced by providing a light shielding or total reflection means on the condenser lens, so that accurate light amount measurement can be performed.
第1図は本発明の第1の実施例の光センサーの断面図、
第2図(a)〜(c)は同センサーの集光レンズに入射
する入射光の状態を示す図、第3図は本発明の第2の実
施例における光センサーの要部断面図、第4図(a)〜
(c)は同実施例における集光レンズに入射する入射光
の状態を示す図、第5図〜第8図は本発明の第3〜第6
の実施例における光センサーの要部断面図、第9図は従
来の光センサーの断面図、第10図は同センサーの光量
と入射角との関係を示す図である。
5・・・・・・集光レンズ、6・・・・・・光検出器、
7・・・・・・光遮蔽過窓、8・・・・・・光検出素子
、9・・・・・・光線遮蔽部代理人の氏名 弁理士 中
尾敏男 ほか1名第1図
T−−−丸餞錫
ト涜オ出東英
第2図
第2図
人前斥力。
第3図
第4図
第4図
(C)
褐 e
i−−−
C()FIG. 1 is a sectional view of a photosensor according to a first embodiment of the present invention;
2(a) to 2(c) are diagrams showing the state of incident light entering the condensing lens of the same sensor, and FIG. Figure 4(a)~
(c) is a diagram showing the state of incident light incident on the condensing lens in the same embodiment, and FIGS.
FIG. 9 is a cross-sectional view of a conventional optical sensor, and FIG. 10 is a diagram showing the relationship between the amount of light and the angle of incidence of the same sensor. 5...Condenser lens, 6...Photodetector,
7...Light shielding window, 8...Photodetection element, 9...Name of the attorney for the light shielding department: Patent attorney Toshio Nakao and one other person Figure 1 T-- - Figure 2, Figure 2, Public repulsion. Figure 3 Figure 4 Figure 4 (C) Brown e i--- C()
Claims (3)
集光レンズとを有し、前記集光レンズの一部に光源より
発せられた光を遮蔽する光遮蔽手段を設けた光センサー
。(1) It has a photodetector and a condensing lens provided on the light source side of the photodetector, and a light shielding means for blocking the light emitted from the light source is provided in a part of the condensing lens. light sensor.
面を設けた請求項1記載の光センサー。(2) The optical sensor according to claim 1, wherein a part of the condensing lens is provided with a total reflection surface that totally reflects the incident light.
集光レンズとを有し、前記集光レンズの一部に入射光を
全反射させる全反射面を設けた光センサー。(3) An optical sensor that includes a photodetector and a condensing lens provided on the light source side of the photodetector, and a part of the condensing lens is provided with a total reflection surface that totally reflects incident light.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63150710A JP2668948B2 (en) | 1988-06-17 | 1988-06-17 | Light sensor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63150710A JP2668948B2 (en) | 1988-06-17 | 1988-06-17 | Light sensor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH01316618A true JPH01316618A (en) | 1989-12-21 |
JP2668948B2 JP2668948B2 (en) | 1997-10-27 |
Family
ID=15502715
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63150710A Expired - Fee Related JP2668948B2 (en) | 1988-06-17 | 1988-06-17 | Light sensor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2668948B2 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107314811B (en) * | 2017-08-09 | 2018-10-12 | 江苏日盈电子股份有限公司 | Sunlight sensor |
EP3480570A1 (en) | 2017-11-01 | 2019-05-08 | Eko Instruments Co., Ltd. | Pyranometer and photometric device |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58137859A (en) * | 1982-02-10 | 1983-08-16 | Fuji Xerox Co Ltd | Exposure detecting device |
JPS593334U (en) * | 1982-06-28 | 1984-01-10 | 三菱電機株式会社 | Optical lens device with light source direction detector |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS593334B2 (en) * | 1976-02-12 | 1984-01-24 | 東洋製罐株式会社 | can body |
-
1988
- 1988-06-17 JP JP63150710A patent/JP2668948B2/en not_active Expired - Fee Related
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58137859A (en) * | 1982-02-10 | 1983-08-16 | Fuji Xerox Co Ltd | Exposure detecting device |
JPS593334U (en) * | 1982-06-28 | 1984-01-10 | 三菱電機株式会社 | Optical lens device with light source direction detector |
Also Published As
Publication number | Publication date |
---|---|
JP2668948B2 (en) | 1997-10-27 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
KR920005443B1 (en) | Optical sensor | |
US20210255033A1 (en) | Light Detection using an Aperture | |
US4420261A (en) | Optical position location apparatus | |
US20050083303A1 (en) | Tracking motion using an interference pattern | |
KR0141447B1 (en) | Pyroelectric type infrared sensor | |
KR20010040931A (en) | Laser scanner measurement system | |
JP2589278Y2 (en) | Apparatus for detecting an object in sheet form | |
US5204520A (en) | Avalanche photodiode array integrated with etched silicon divider | |
JPH01316618A (en) | Optical sensor | |
JPS5899712A (en) | Slant angle measuring device | |
JPS6390866A (en) | Semiconductor photodetector device | |
EP1092965A1 (en) | Numerical aperture limiter | |
JP3090336B2 (en) | Optical detector | |
JP3090337B2 (en) | Optical detector | |
JP3015634B2 (en) | Scattered light smoke detector | |
JP2513148B2 (en) | Optical beam position detector | |
JP2919082B2 (en) | Multi-segment lens for optical detector | |
JP2744872B2 (en) | Scattered light smoke detector | |
JP3015633B2 (en) | Scattered light smoke detector | |
JP3008312B2 (en) | Photo interrupter and detection device | |
JP3039623U (en) | Distance measuring device | |
JPS6129745A (en) | Detecting device for pinhole defect | |
JP2534789B2 (en) | Focus detection optical system | |
JPH03223616A (en) | Photoelectric range finder | |
JPH11153407A (en) | Distance and inclination measuring device |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
LAPS | Cancellation because of no payment of annual fees |