JPS58154625A - Sensor for detecting illumination of whole sky - Google Patents

Sensor for detecting illumination of whole sky

Info

Publication number
JPS58154625A
JPS58154625A JP3841182A JP3841182A JPS58154625A JP S58154625 A JPS58154625 A JP S58154625A JP 3841182 A JP3841182 A JP 3841182A JP 3841182 A JP3841182 A JP 3841182A JP S58154625 A JPS58154625 A JP S58154625A
Authority
JP
Japan
Prior art keywords
light
cylinder
sky
sensor
whole sky
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
JP3841182A
Other languages
Japanese (ja)
Inventor
Masato Oki
沖 允人
Kazutoshi Nakao
中尾 一俊
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP3841182A priority Critical patent/JPS58154625A/en
Priority to DE19833308429 priority patent/DE3308429A1/en
Priority to FR8304339A priority patent/FR2523301A1/en
Publication of JPS58154625A publication Critical patent/JPS58154625A/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
    • G01J1/0403Mechanical elements; Supports for optical elements; Scanning arrangements
    • 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
    • G01J1/06Restricting the angle of incident light
    • 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
    • G01J1/0214Constructional arrangements for removing stray light

Landscapes

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

Abstract

PURPOSE:To detect the illumination of thw whole sky even in a densely built-up area, by fitting separators forming light passing holes between a light collecting hole and a photosensor to prevent the reflected light from the inwall surface of a light shielding cylinder from being made incident to the photosensor. CONSTITUTION:The light collecting hole H1 with radius r1 is formed on the upper surface of the light shielding cylinder 1 having square sections of which the whole inside and outside surfaces are coated with delustering black paint and an illuminometer 2 having the photodetecting area of radius r2 (r2<r1) is attached to the bottom of the cylinder 1. In order to prevent the light from the light collecting hole H1 from being reflected by the inwall of the cylinder 1 and irradiated to the iluminometer 2, the separators 3-6 are fitted between the upper surface of the cylinder 1 and the illuminometer 2. When the whole sky luminance E' around the periphery of the zenith is to be measured by turning the cylinder 1 upwards, the whole sky illumination E is found from E=K.E' when a constant fixed by the shape of the whole sky illumination sensor ODS, a measuring time band and the weather at the time band is defined as K.

Description

【発明の詳細な説明】 零発鳩は住宅の凰光照明環境に対応し九2光率、即ち、
住宅内任意の受wA面上の凰光照度とそれと同ti#j
に生ずる直射日光を除いえ水平面上の全天空照度との比
の測定に使用する全天空照度検出センサに関するもので
ある。
[Detailed description of the invention] The zero-lighting pigeon corresponds to the residential lighting environment and has a light rate of 92, that is,
The illuminance of the phoenix light on any receiving surface in the house and the same ti#j
The present invention relates to a sensor for detecting total sky illuminance, which is used to measure the ratio of total sky illuminance on a horizontal plane, excluding direct sunlight.

従来、思光率測定に際しては、2光率が家内照度と全天
゛空照度との比であることから、2つの照度針のうちの
一方は被測定住宅内任意の部屋のほぼ中央にセットされ
て太陽光1sIcよる部屋の明るさを検出するとともに
、他方の照度針は当該住宅地域の屋外にセフ)されて直
射日光を除いた水平面上の全天空照度を検出するが、全
天空照度を正確に検出するためには水平面上に光を遺る
一切の建造物、樹木等のないことが必要である。
Conventionally, when measuring luminous index, one of the two illuminance hands is set approximately in the center of any room in the house to be measured, since the luminous index is the ratio of the illuminance inside the house and the total sky illuminance. The other illuminance needle is set outside the residential area to detect the brightness of the room due to 1sIc of sunlight, and the other illuminance needle is set outside the residential area to detect the total sky illuminance on the horizontal plane excluding direct sunlight. For accurate detection, it is necessary that there be no buildings, trees, etc. that would leave light on the horizontal plane.

しかるに、現実問題として、住宅が建てられるほとんど
の場所には水平面上の視界を遮る何らかの建造物等があ
るため、全天空照度を正確に測定することができず、従
って、全天空照度検出用層ンサは比較的広い場所の中央
部IC−にフトされても、周辺に建造物等があって水平
面上の視界が遮られることには変わりはなく、また、視
界が遮られる程度は各測定地域によってそれぞれ異なる
ことから、全天空照度の検出111度も一定せず、その
結果、駅光率測定値に対する信頼性は乏しく、2光率測
定結果は単なる目安としてでしか用いられないという欠
点があった。
However, as a practical matter, most places where houses are built have some type of structure that obstructs the view on the horizontal plane, making it impossible to accurately measure the total sky illuminance. Even if the sensor is moved to a central IC in a relatively wide area, there will still be buildings in the surrounding area that will obstruct the view on the horizontal plane, and the extent to which the view will be obstructed will vary depending on each measurement area. Since the total sky illuminance is different for each, the detection of total sky illuminance (111 degrees) is not constant.As a result, the reliability of the station light rate measurement is poor, and the two light rate measurement results can only be used as a guide. Ta.

本発明の目的は住宅密集地11NICおいても、精度の
高い検出が可能な限られ九範囲の天頂輝度から全天空照
度を求める全天空照度検出センナを提供することによっ
て、前記従来の欠点を除去することにある。
An object of the present invention is to eliminate the above-mentioned drawbacks of the conventional art by providing an all-sky illuminance detection sensor that detects all-sky illuminance from a limited nine ranges of zenith brightness and is capable of highly accurate detection even in densely populated residential areas (11 NICs). It's about doing.

次に、本発明の一実施例の構成を図面によって餠、明す
る。
Next, the configuration of an embodiment of the present invention will be explained with reference to the drawings.

内外全面をつや消黒艷塗装をした断面正方形状遮光筒1
上面に社半径r1の光採入孔H1が形成され、かつ、そ
の底面には半径r2(r2(rl)の受光面積の照度針
2が取付けられるとともに、遮光筒1の上面と底面との
間には光採入孔H1からの光が通光f[113内壁面に
反射して照度計2eC照射されるのを防止するためのセ
パレータ6〜6が予め規定された間隔で取付けられ、各
セパレータ5〜6に形成された光通過孔H2〜H5の寸
法は、前記WA度計2中心と光採入孔H1円鳩とを直線
で結ぶ角度aと、照度計2受光面積の半径r2円周位曹
から光採入孔H1内周の最大、最小位瞳とを直線で結ぶ
角度θ1、θ2とのそれぞれが予め規定した特定関係に
なるように定められ、全大空照度センサODSがこれら
各条件に従って形成された扶助において、この遮光筒1
を上に向けて天頂周辺の天空輝度E′を測定すると、全
天空照度Eは前記全天空照度センサ○D8の形状、測定
時間帯とそのときの天候等tこよって定まる定数なXと
すると、 1=に一1’ で求められるときもに、全天空照度E測定時において図
示省略室内照度センサよりaによって測定された任意の
室内の照度がEsのと趣、当u、家内の賦光率りは a D = 、 (%) で表わされ、この測定を天候、測定時間帯等によっても
変動しないように、任意の時間間隔でnll測測定た累
積平均tli[D’で求めると、で表わされる。
Shade tube 1 with a square cross section with matte black paint on the entire inside and outside.
A light intake hole H1 with a radius r1 is formed on the top surface, and an illuminance needle 2 with a light receiving area of a radius r2 (r2 (rl) is attached to the bottom surface of the hole H1, and a light receiving hole H1 with a light receiving area of radius r2 (rl) is attached to the bottom surface of the hole H1. Separators 6 to 6 are installed at predetermined intervals to prevent the light from the light intake hole H1 from being reflected on the inner wall surface of the light passage f[113 and irradiated with the illumination meter 2eC, and each separator The dimensions of the light passing holes H2 to H5 formed in 5 to 6 are the angle a connecting the center of the WA meter 2 and the light intake hole H1 with a straight line, and the radius r2 of the light receiving area of the illumination meter 2. The angles θ1 and θ2 connecting the maximum and minimum pupils of the inner periphery of the light intake hole H1 with a straight line are determined to have a specific predetermined relationship, and the total sky illuminance sensor ODS is set under each of these conditions. In the aid formed according to
When measuring the sky brightness E' around the zenith with the sensor facing upward, the total sky illuminance E is a constant X determined by the shape of the total sky illuminance sensor ○D8, the measurement time period, the weather at that time, etc. When 1 = 1', when measuring the total sky illuminance E, the illuminance in any room measured by a by an indoor illuminance sensor (not shown) is Es, and u is the light absorption rate in the house. The rate is expressed as a D = , (%), and the cumulative average tli [D' of nll measurements taken at arbitrary time intervals so as not to fluctuate due to weather, time of day, etc. expressed.

なお、この全天空照度センサOD8は測定M度を高める
ために、原則としてCIE欅準標準空、即ち、水平から
の高度θの天空輝度Lθと天頂輝度Lwとの比が で表される完全な曇天空またはこれに準する状態で用い
られ、この場合において全天空照度センナODSを例え
ば第1図のように三脚7に直接取付けて水平に竜ットし
、あるいは、嬉5図のように自在回転体8とブラケット
9とを介して取付けて自動的に水平に竜ットし、このと
き、全天空照度センサOD8の照度計2で求められ九測
定値をIzとすると、全天空照度Eは、 1=に・ Ex で求められ、この定数には第1図に示す関係の遮光筒1
において、光採入孔H1より照度針2受光面(2r2)
への入射光束rは 照良計29光面(2r2)の平均開度Exはl  W 
K 、g z 天頂部分を測定し、測定範囲における天頂輝度Lmは一
定とすると、 とおくと、 ここで例として、 θ1=14.26@ 02ニー5.0” rm ”0.0205 従って r+”0.0100 d−0,120 El ”= 5.0 とすると K””47.5 一様大空とすると、 K =x K’= 149.5 同様に θ1=10.0゜ θまた5、0@ r2zO,012 従って r1冨o、 o 3 b d=0.270 α=7.6 とすると、 x’z18.3 一様天空とすると、 K=rK’=57.4 このように全天空照度センサOD8の形状寸法で定まる
定数Xを照度針2の測定値に乗することによって、全天
空照度を措定値として高精度に求めることができ、これ
によって住宅密集地においても駅光率を高精度に求める
ことかで―る効果がある。
In order to increase the measurement M degree, this all-sky illuminance sensor OD8 is used as a general rule in accordance with the CIE Keyaki semi-standard sky, that is, the complete sky illuminance sensor OD8, where the ratio of the sky brightness Lθ at an altitude θ from the horizontal to the zenith brightness Lw is expressed as It is used under cloudy skies or similar conditions, and in this case, the all-sky illuminance sensor ODS can be directly attached to the tripod 7 as shown in Figure 1 and mounted horizontally, or it can be used freely as shown in Figure 5. It is attached via the rotating body 8 and the bracket 9 and is automatically set horizontally. At this time, if the measured value obtained by the illuminance meter 2 of the all-sky illuminance sensor OD8 is Iz, the all-sky illuminance E is , 1=Ex
, from the light intake hole H1 to the light receiving surface of the illumination needle 2 (2r2)
The incident luminous flux r is the illumination meter, and the average opening Ex of the 29 light surface (2r2) is l W
K , g z If the zenith part is measured and the zenith brightness Lm in the measurement range is constant, then as an example, θ1 = 14.26 @ 02 knee 5.0" rm "0.0205 Therefore r+" 0.0100 d-0,120 If El "= 5.0, K""47.5 If it is a uniform sky, K = x K' = 149.5 Similarly, θ1 = 10.0° θ and 5,0 @ r2zO,012 Therefore, r1 Tomio, o 3 b d=0.270 α=7.6, x'z18.3 Assuming a uniform sky, K=rK'=57.4 In this way, the total sky illuminance By multiplying the measured value of the illuminance needle 2 by a constant There are different effects depending on what you are looking for.

次に本発明の効果ンこついて説明する。Next, the effects of the present invention will be explained.

本発明は内面を黒色仕上した遮光筒の上面に大空輝度に
対応した太陽光線採光用先様入孔を形成するとともに、
前記遮光筒の先様入孔直下の予め設定した一定深さ位置
に光量に対応した電束信号を発生させる光センナを取付
け、かつ、前記遮光筒内壁面からの反射光が前記光セン
ナに入射するのを防止するため前記先様入孔と前記光セ
ンナとの間の任意間隔付蓋に光通過孔を形成したセパレ
ータを取付けた全天空照度検出センサにある。
In the present invention, a hole is formed on the top surface of the light-shielding tube whose inner surface is finished black, and a hole is formed at the top for letting in sunlight that corresponds to the brightness of the sky.
An optical sensor that generates an electric flux signal corresponding to the amount of light is installed at a predetermined depth position directly below the tip entrance hole of the light-shielding tube, and the reflected light from the inner wall surface of the light-shielding tube enters the optical sensor. In order to prevent this, the all-sky illuminance detection sensor is provided with a separator having a light passage hole formed in a lid with an arbitrary distance between the entrance hole and the optical sensor.

これによって、本発明は住宅密集地斌においても、精度
の高い検出が可能な限られた範囲の天頂輝度から全天空
照度を容易かつ高精度に求めることがで亀るとともに思
光率測定値の精度と信軸性を著しく向上させることがで
きる効果がある。
As a result, the present invention makes it possible to easily and accurately determine the total sky illuminance from a limited range of zenith brightness that can be detected with high precision even in densely populated residential areas, and to improve the spectral rate measurement value. This has the effect of significantly improving accuracy and reliability.

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

81図は本発明の一実施例の破断偽面図、第2図はその
破断平面図、第6図はその使用杖すの一例を示す斜視図
である。 1・・・遮光I@2・・・照度計 3〜6・・・セパvX′−タ   Hl・・・先様入孔
H2〜H5・・・光通過孔
FIG. 81 is a cutaway false sectional view of an embodiment of the present invention, FIG. 2 is a cutaway plan view thereof, and FIG. 6 is a perspective view showing an example of the cane used. 1... Light shielding I@2... Illuminance meter 3-6... Separator vX'-ta Hl... Previous entry hole H2-H5... Light passing hole

Claims (1)

【特許請求の範囲】[Claims] 内面を黒色仕上し丸遮光簡の上面IC天空輝度に対応し
九太陽光線採光用光採入孔を形成するとともに、前記遮
光筒の光挿入孔直下の予め設定した一定深さ位曹に光量
に対応した電気信号を発生させる光センサを取付け、か
つ、前記゛′遺先光筒内壁面らの反射光が前記光センナ
に入射するのを防止する丸め前記光採入孔と前記光セン
ナとの間の任意間隔位l1lIc光通過孔を形成したセ
パレータを取付けることを特徴とする全天空照度検出セ
ンサ。
The inner surface is finished black, and a light intake hole for nine solar rays is formed on the top surface of the round light shielding tube to correspond to the sky brightness. A light sensor that generates a corresponding electric signal is attached, and the rounded light intake hole and the light sensor prevent reflected light from the inner wall surface of the trailing light tube from entering the light sensor. An all-sky illuminance detection sensor comprising a separator having light passage holes formed at arbitrary intervals between l1lIc.
JP3841182A 1982-03-10 1982-03-10 Sensor for detecting illumination of whole sky Pending JPS58154625A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP3841182A JPS58154625A (en) 1982-03-10 1982-03-10 Sensor for detecting illumination of whole sky
DE19833308429 DE3308429A1 (en) 1982-03-10 1983-03-07 Sensor which can be mounted in the open in order to measure the brightness of the uncovered sky
FR8304339A FR2523301A1 (en) 1982-03-10 1983-03-09 OUTDOOR DETECTOR FOR DETECTING ILLUMINATION OF AN OBSTACLE-FREE SKY

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3841182A JPS58154625A (en) 1982-03-10 1982-03-10 Sensor for detecting illumination of whole sky

Publications (1)

Publication Number Publication Date
JPS58154625A true JPS58154625A (en) 1983-09-14

Family

ID=12524552

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3841182A Pending JPS58154625A (en) 1982-03-10 1982-03-10 Sensor for detecting illumination of whole sky

Country Status (3)

Country Link
JP (1) JPS58154625A (en)
DE (1) DE3308429A1 (en)
FR (1) FR2523301A1 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007038597A (en) * 2005-08-05 2007-02-15 Seiko Epson Corp Printer and lens detection method
JP2008116463A (en) * 2007-11-16 2008-05-22 Mitsubishi Cable Ind Ltd Sunshine sensor
JP2009109315A (en) * 2007-10-30 2009-05-21 Sony Corp Light measuring device and scanning optical system
JP2009250705A (en) * 2008-04-03 2009-10-29 Fujitsu Ltd Light guiding mechanism for illumination sensor and mobile phone

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10065732B2 (en) * 2012-08-21 2018-09-04 Technology For Energy Corporation Systems and methods of tracking rotor blades

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5110512A (en) * 1974-07-15 1976-01-28 Tokyo Shibaura Electric Co JODENDOJIKIFUJOSEIGYOHOHO

Family Cites Families (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1546264A (en) * 1921-12-31 1925-07-14 Gen Electric Radiation-measuring device
DE1759212U (en) * 1957-11-05 1958-01-02 Friedrich Dipl Phys Dr Volz SMALL PHOTOMETER TO MEASURE THE DIRECT SUNLIGHT.
US3648056A (en) * 1970-01-12 1972-03-07 Honeywell Inc Optical detector with radiant energy absorbing chamber
DE2355033A1 (en) * 1973-11-03 1975-05-07 Franz Ummen Universal optical electronic sensor - reacts to both increasing and decreasing light intensities
US4040751A (en) * 1976-01-13 1977-08-09 Polaroid Corporation Unicell photometer device
US4217026A (en) * 1978-08-25 1980-08-12 The United States Of America As Represented By The Secretary Of The Air Force Elliptic cylindrical baffle assembly
DE2924125C2 (en) * 1979-06-15 1982-10-28 Bodenseewerk Perkin-Elmer & Co GmbH, 7770 Überlingen Device for suppressing stray light in grating monochromators

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5110512A (en) * 1974-07-15 1976-01-28 Tokyo Shibaura Electric Co JODENDOJIKIFUJOSEIGYOHOHO

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007038597A (en) * 2005-08-05 2007-02-15 Seiko Epson Corp Printer and lens detection method
JP2009109315A (en) * 2007-10-30 2009-05-21 Sony Corp Light measuring device and scanning optical system
JP2008116463A (en) * 2007-11-16 2008-05-22 Mitsubishi Cable Ind Ltd Sunshine sensor
JP2009250705A (en) * 2008-04-03 2009-10-29 Fujitsu Ltd Light guiding mechanism for illumination sensor and mobile phone

Also Published As

Publication number Publication date
FR2523301A1 (en) 1983-09-16
DE3308429A1 (en) 1983-09-29

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