JPS6183921A - Illuminometer - Google Patents

Illuminometer

Info

Publication number
JPS6183921A
JPS6183921A JP20581384A JP20581384A JPS6183921A JP S6183921 A JPS6183921 A JP S6183921A JP 20581384 A JP20581384 A JP 20581384A JP 20581384 A JP20581384 A JP 20581384A JP S6183921 A JPS6183921 A JP S6183921A
Authority
JP
Japan
Prior art keywords
light
photo detection
detection angle
cosine law
substrate
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.)
Pending
Application number
JP20581384A
Other languages
Japanese (ja)
Inventor
Rie Otsuka
大塚 利恵
Osamu Yamada
修 山田
Kazuaki Okubo
和明 大久保
Hideo Nishiyama
西山 英夫
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP20581384A priority Critical patent/JPS6183921A/en
Publication of JPS6183921A publication Critical patent/JPS6183921A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • G01J1/0407Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings
    • G01J1/0455Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings having a throughhole enabling the optical element to fulfil an additional optical function, e.g. a mirror or grating having a through-hole for a light collecting or light injecting optical fibre
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • G01J1/0407Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings
    • G01J1/0474Diffusers
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/0204Compact construction
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • G01J2001/0485Cosinus correcting or purposely modifying the angular response of a light sensor

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

PURPOSE:To obtain the photo detection angle characteristic complying with the cosine law, by providing one or more photo detection angle characteristic correcting apertures on the side of a photo detector. CONSTITUTION:Light incident from the top (x) of a light diffusion plate 3 reaches a photoelectric conversion element 7 passing sequentially through a magnifying filter 5 and a view angle correction filter 6 to be converted into electricity. As the photo detection angle grows larger to 90 deg., incident light from the top (x) of the light diffusion plate 3 decreases too much to maintain the photo detection angle characteristic complying with the cosine law. But when provided on the side of the substrate 4, an aperture 8 allows light to reach the BD surface incident from the AC surface so that the photo detection characteristic is corrected with respect to the photo detection angle near 90 deg.. In this manner, the photo detection angle characteristic can be obtained which the light receiving surface composed of the substrate 4 and the light diffusion plate 3 is flat while precisely complying with the cosine law.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、受光角特性補正済みの受光器をもつ照度計に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an illuminance meter having a light receiver whose light receiving angle characteristics have been corrected.

従来列の)1り成と問題点 照度計がもつべき重要な特性は2つあり、1つは受光器
の分光感度特性が標準比視感度に合致していることと、
もう1つは、受光器の受光角特性が余弦則に合致してい
ることである。このうち後者の余弦則は第4図のように
表せる。第4図において受光面の中心に立てた垂線と入
射光とのなす角を受光角θとすると、受光角の変化にと
もなう受光器の感1度がC05θで変化することを余弦
則に従うという。
(Conventional column) 1. Composition and Problems There are two important characteristics that an illuminance meter should have. One is that the spectral sensitivity characteristics of the light receiver match the standard luminous efficiency;
The other is that the light receiving angle characteristics of the light receiver match the cosine law. The latter cosine law can be expressed as shown in Figure 4. In Fig. 4, if the angle between the perpendicular to the center of the light-receiving surface and the incident light is the light-receiving angle θ, then the sensitivity of the light receiver changes by C05θ as the light-receiving angle changes, which is said to follow the cosine law.

照度計の受光器は通常光電変換素子の上に光拡散板をお
くことにより上記受光角特性を余弦則に合致させるよう
にしている。この光拡散板はその形状が(ト面である場
合、第6図のように拡散性のよいものほど余弦則に近似
する。しかし、最も優れた拡散性を用いた場合でも、受
光面の形状が平面であり、また周辺の基板と同一平面ま
たはそれより低い位置にある場合には、受光角が900
に近づくにつれ、受光角特性の余弦則からのはずれが大
きくなる。そこでこれを改善するため、光拡散板および
その周辺の基板の形状に様々な工夫がこらされている。
The light receiver of the illuminance meter usually has a light diffusing plate placed on top of the photoelectric conversion element so that the above-mentioned light receiving angle characteristics match the cosine law. When the shape of this light diffusing plate is (total), the better the diffusivity is, the more it approximates the cosine law as shown in Figure 6. However, even when the best diffusivity is used, the shape of the light-receiving surface is flat and located on the same plane or lower than the surrounding substrate, the acceptance angle is 900°.
As the value approaches , the deviation of the acceptance angle characteristic from the cosine law increases. In order to improve this problem, various improvements have been made to the shape of the light diffusing plate and the substrate around it.

例えば、第6図a、hに示すように光拡散板の形状を平
面から立体状にするとともに、周辺の基板よりも拡散板
を持ち上げることによって、90’付近での受光角特性
の改善をはかっている。しかし、光拡散板を基板より持
ち上げることにより、90°付近での指示値が零になら
ない場合もある。また、光拡散板が立体状である場合、
測定基準面を光拡散板のどの位置にするかによって光源
からの距離が変わるため、その照度1直の信頼性に問題
が生じてくる。また測定時および収納時に光拡散板の表
面に傷がつき、受光角特性に悪影響をおよぼすこともあ
る。
For example, as shown in Figures 6a and 6h, the shape of the light diffusing plate can be changed from a flat surface to a three-dimensional shape, and the light receiving angle characteristics around 90' can be improved by raising the diffusing plate higher than the surrounding substrates. I know. However, by lifting the light diffusing plate above the substrate, the indicated value at around 90° may not become zero. In addition, if the light diffusing plate is three-dimensional,
Since the distance from the light source changes depending on where the measurement reference plane is located on the light diffusing plate, a problem arises in the reliability of the single illuminance. Furthermore, the surface of the light diffusing plate may be scratched during measurement and storage, which may adversely affect the light receiving angle characteristics.

発明の目的 本発明は、このような従来の問題を解消するもので、光
拡散板が基板と同一平面かまたはこれより低い位置にあ
って、余弦則に合致した受光角特性を持つ照度計受光部
を提供するものである。
OBJECTS OF THE INVENTION The present invention solves these conventional problems, and provides an illuminometer light receiving device in which the light diffusing plate is located on the same plane as the substrate or at a position lower than this, and has a receiving angle characteristic that conforms to the cosine law. The purpose of this is to provide the following information.

発明の構成 本発明は、照度計受光部の基板と、この基板と同一平面
かこれより低い平面に位置する光拡散板と前記基板の側
面に設けた1つ以上のアパーチャから構成する照度計受
光器であり、これにより余弦則に正確に合致した受光角
特性が得られるものである。
Structure of the Invention The present invention provides an illumination meter light receiving unit which is composed of a substrate of the illumination meter light receiving section, a light diffusing plate located on the same plane as the substrate or a plane lower than this, and one or more apertures provided on the side surface of the substrate. With this, it is possible to obtain light receiving angle characteristics that exactly match the cosine law.

実施例の説明 第1図は本発明の実施例における照度計受光器の断面構
造を示すものである。第3図において3は光拡散板、4
は照度計受光器の基板、5は倍率フィルタ、6は視感度
補正フィルタ、了は光電変換素子である。また8はアパ
ーチャである。
DESCRIPTION OF EMBODIMENTS FIG. 1 shows a cross-sectional structure of an illuminance meter receiver in an embodiment of the present invention. In Fig. 3, 3 is a light diffusing plate, 4
5 is a magnification filter, 6 is a visibility correction filter, and R is a photoelectric conversion element. Further, 8 is an aperture.

照度計受光器は第4図に示すように、光拡散板の上面X
から入射した光は順次倍率フィルタ5、視感度補正フィ
ルタ6、を通って光電変換素子7に達して光′電変換さ
れる。受光角が大きくなって90’に近づくと、光拡散
板の上面Xからの入射光は減少して、余弦則に従った受
光角特性を維持できなくなるが、基板の側面にアパーチ
ャ8を設けることにより光はAC面から入射して、BD
面に達し、ここから拡散板を通して光電変換素子7に達
し、90’附近での受光角に対する受光角特性の補正の
役割をはたすことができる。第1図のアパーチャ8にお
いて、CBは光拡散板の上面Xと平行に位置する。アパ
ーチャ内面壁は黒色つや消し塗装とする。これにより、
90°の受光角に対する光入射を零としている。また、
Bpに対するACの長さが大きいほど、受光角の小さい
ところかC)の補正ができることになる。
As shown in Figure 4, the illumination meter receiver is
The incident light passes sequentially through a magnification filter 5 and a visibility correction filter 6, reaches a photoelectric conversion element 7, and is photo-electrically converted. As the acceptance angle increases and approaches 90', the incident light from the top surface X of the light diffusing plate decreases, making it no longer possible to maintain acceptance angle characteristics according to the cosine law. However, providing an aperture 8 on the side of the substrate Therefore, the light enters from the AC surface, and the BD
From there, it reaches the photoelectric conversion element 7 through the diffuser plate, and can play the role of correcting the light receiving angle characteristics for the light receiving angle around 90'. In the aperture 8 of FIG. 1, CB is located parallel to the upper surface X of the light diffusing plate. The inner wall of the aperture will be painted matte black. This results in
The light incidence for a light receiving angle of 90° is assumed to be zero. Also,
The larger the length of AC with respect to Bp, the more correction can be made for the small angle of acceptance or C).

第2図は、受光器の外観図を示す0第2図において4は
基板、3は光拡散板、8はアパーチャを示す。このアパ
ーチャは受光器の側面に一列に配置しているが、二列あ
るいはそれ以上をレンガ積みのように配置することもで
きる。また第3図のように、多数個のアパーチャをすべ
て連結して、この部分に透明な光材料9を挿入してもよ
い。これによっても受光角特性の補正は可能である。
FIG. 2 shows an external view of the light receiver. In FIG. 2, 4 is a substrate, 3 is a light diffusing plate, and 8 is an aperture. The apertures are arranged in one row on the side of the receiver, but two or more rows can also be arranged in a brick-like arrangement. Alternatively, as shown in FIG. 3, a plurality of apertures may all be connected and a transparent optical material 9 may be inserted into this portion. This also makes it possible to correct the light receiving angle characteristics.

発明の効果 本発明による照度計受光器は、側面に受光角特性補正用
アパーチャを配備しているため、基板および光拡散板で
構成される受光面が平面にしてかつ余弦則に正確に一致
した受光角特性をもち、照度計用受光器としてその実用
性はまことに大きい0
Effects of the Invention The illumination meter receiver according to the present invention is equipped with an aperture for correcting the angle of acceptance characteristics on the side, so that the acceptance surface made up of the substrate and the light diffusing plate is flat and precisely conforms to the cosine law. It has light receiving angle characteristics and is extremely useful as a light receiver for illumination meters.

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

第1図は本発明による照度計受光部の断面図、第2図は
本発明の一実施例による照度計受光部の外観図、第3図
は本発明の他の実施例による照度計受光部の外i82図
、第4図は余弦則に従う受光角特性の誇明図、第5図は
拡散性の違いによる照度計受光器の受光角特性図、第6
図は従来の照度計受光部のりr面図である。 3・・・・・・光拡散板、4・・・・・・受光器の基板
、7・山・・光電変換素子、8・・印・アパーチャ。 代PII人の氏名 弁理士 中 尾 敏 男 はが1名
第3図 (a、) 受光、1IilliL(θ)
FIG. 1 is a sectional view of an illuminometer light receiving section according to the present invention, FIG. 2 is an external view of an illuminance meter light receiving section according to an embodiment of the present invention, and FIG. 3 is an illuminance meter light receiving section according to another embodiment of the present invention. Figure 4 is an exaggerated diagram of the acceptance angle characteristics according to the cosine law, Figure 5 is a diagram of the acceptance angle characteristics of the illumination meter receiver due to differences in diffusivity, and Figure 6
The figure is an R-side view of a conventional illuminance meter light receiving section. 3... Light diffuser plate, 4... Light receiver substrate, 7... Mountain... Photoelectric conversion element, 8... Mark... Aperture. Name of representative PII Patent attorney Toshio Nakao 1 person Figure 3 (a,) Light reception, 1IilliL (θ)

Claims (1)

【特許請求の範囲】[Claims] 受光器の側面に1つ以上の受光角特性補正用アパーチャ
をもうけた照度計。
An illuminance meter that has one or more apertures on the side of the receiver for correcting the receiving angle characteristics.
JP20581384A 1984-10-01 1984-10-01 Illuminometer Pending JPS6183921A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20581384A JPS6183921A (en) 1984-10-01 1984-10-01 Illuminometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20581384A JPS6183921A (en) 1984-10-01 1984-10-01 Illuminometer

Publications (1)

Publication Number Publication Date
JPS6183921A true JPS6183921A (en) 1986-04-28

Family

ID=16513120

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20581384A Pending JPS6183921A (en) 1984-10-01 1984-10-01 Illuminometer

Country Status (1)

Country Link
JP (1) JPS6183921A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4948969A (en) * 1988-03-29 1990-08-14 Sharp Kabushiki Kaisha Photodetector having convex window for shielding electromagnetic wave and electrostatic induction noises
US5456945A (en) * 1988-12-27 1995-10-10 Symetrix Corporation Method and apparatus for material deposition
US5614252A (en) * 1988-12-27 1997-03-25 Symetrix Corporation Method of fabricating barium strontium titanate

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4948969A (en) * 1988-03-29 1990-08-14 Sharp Kabushiki Kaisha Photodetector having convex window for shielding electromagnetic wave and electrostatic induction noises
US5456945A (en) * 1988-12-27 1995-10-10 Symetrix Corporation Method and apparatus for material deposition
US5614252A (en) * 1988-12-27 1997-03-25 Symetrix Corporation Method of fabricating barium strontium titanate

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