JPH0752125B2 - Irradiometer - Google Patents
IrradiometerInfo
- Publication number
- JPH0752125B2 JPH0752125B2 JP61051102A JP5110286A JPH0752125B2 JP H0752125 B2 JPH0752125 B2 JP H0752125B2 JP 61051102 A JP61051102 A JP 61051102A JP 5110286 A JP5110286 A JP 5110286A JP H0752125 B2 JPH0752125 B2 JP H0752125B2
- Authority
- JP
- Japan
- Prior art keywords
- pyroelectric
- light
- detection element
- radiation detection
- shutter
- 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 - Lifetime
Links
- 230000005855 radiation Effects 0.000 claims description 43
- 238000001514 detection method Methods 0.000 claims description 25
- 230000035945 sensitivity Effects 0.000 claims description 13
- 230000003287 optical effect Effects 0.000 claims description 7
- 238000009792 diffusion process Methods 0.000 description 8
- 230000005540 biological transmission Effects 0.000 description 4
- 238000005259 measurement Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 230000010354 integration Effects 0.000 description 2
- 230000002123 temporal effect Effects 0.000 description 2
- 230000001052 transient effect Effects 0.000 description 2
- 238000003491 array Methods 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 238000010408 sweeping Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J1/00—Photometry, e.g. photographic exposure meter
- G01J1/02—Details
- G01J1/04—Optical or mechanical part supplementary adjustable parts
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J1/00—Photometry, e.g. photographic exposure meter
- G01J1/02—Details
- G01J1/04—Optical or mechanical part supplementary adjustable parts
- G01J1/0407—Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings
- G01J1/044—Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings using shutters
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J1/00—Photometry, e.g. photographic exposure meter
- G01J1/02—Details
- G01J1/04—Optical or mechanical part supplementary adjustable parts
- G01J1/0407—Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings
- G01J1/0474—Diffusers
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】 産業上の利用分野 本発明は、紫外波長域から赤外波長域に至る広い範囲の
放射パワーの定量的検出が精度よく行なえ、かつ携帯用
装置として小形,軽量に構成された放射照度計に関する
ものである。TECHNICAL FIELD The present invention is capable of accurately quantitatively detecting radiation power in a wide range from the ultraviolet wavelength range to the infrared wavelength range, and is compact and lightweight as a portable device. Irradiance meter which was made.
従来の技術 これまで放射パワー(例えばmW・cm-2単位)の検出には
古くから、受光面を金黒などでブラッキングした感度の
波長依存性がない熱電対や熱電対列(サーモパイル)が
用いられていたが、これらはゼロ点ドリフトが大きく、
また応答時間(時定数)も大きい。さらに十分な感度が
得られないため実用上使用しにくい面があった。Conventional technology It has been a long time for detecting radiation power (for example, mW · cm -2 unit), and thermocouples and thermopile arrays (thermopile) that have black sensitivity on the light-receiving surface and have no wavelength dependence of sensitivity have been used. It was used, but these have a large zero point drift,
The response time (time constant) is also large. In addition, it was difficult to practically use because sufficient sensitivity could not be obtained.
最近これらに替わるものとして焦電効果を利用した放射
検出素子が開発された。しかし焦電型の放射検出素子
は、入射する放射の微分的変動にのみ応答して、定常的
な(一定の強さで時間的に変化しない)入射には感度が
ない。そのため焦電型放射検出素子は、火災の発生や侵
入者による放射の変動のような一過性の変化現象の探知
に使用されることが多かった。Recently, a radiation detection element utilizing the pyroelectric effect has been developed as an alternative to these. However, pyroelectric radiation detection elements are insensitive to steady (non-time-varying, constant intensity) incidence, responding only to the differential variation of the incident radiation. Therefore, the pyroelectric radiation detecting element is often used for detecting a transient change phenomenon such as a fire occurrence or a change in radiation by an intruder.
発明が解決しようとする問題点 焦電型放射検出素子で定常光の光量を測定しようとする
場合、通常は回転セクターをモータなどで駆動して入力
放射を断続する必要がある。これに受光器の受光角感度
特性を余弦則に近似せしめる透過拡散構造物を組み合わ
せて放射照度計を構成した場合、回転セクターは受光面
の端部から受光面を掃引するかたちで放射をさえぎるた
め、受光器の入射角特性が時間的に変化するという問題
点が生ずる。Problems to be Solved by the Invention In order to measure the amount of stationary light with a pyroelectric radiation detection element, it is usually necessary to drive the rotating sector with a motor or the like to interrupt the input radiation. When a irradiance meter is constructed by combining this with a transmission diffusion structure that approximates the light receiving angle sensitivity characteristic of the receiver to the cosine law, the rotating sector blocks the radiation by sweeping the light receiving surface from the edge of the light receiving surface. However, there is a problem that the incident angle characteristic of the light receiver changes with time.
また、装置が複雑,精密かつ大がかりなものになるため
携帯用の放射照度計には不適当であった。In addition, the device is complicated, precise, and large-scale, and thus is not suitable for a portable irradiometer.
本発明は上記従来の問題を解消し、紫外域から赤外域に
いたる広い波長範囲の放射照度を定量的に精度よく検出
する、小形軽量で携帯可能な放射照度計を提供すること
を目的とする。SUMMARY OF THE INVENTION It is an object of the present invention to solve the above conventional problems and to provide a small, lightweight and portable irradiance meter that quantitatively and accurately detect irradiance in a wide wavelength range from the ultraviolet region to the infrared region. .
問題点を解決するための手段 本発明の放射照度計は、焦電型放射検出素子と、その受
光角感度特性を余弦則に近似せしめる透過拡散構造物
と、前記焦電型放射検出素子への入力放射を前記焦電型
放射検出素子受光面の中心に対して、同心円状に開閉し
断続する光シャッターと、前記焦電型放射検出素子から
の光電出力を入射光量に比例した直流出力に変換し表示
する回路から構成される。Means for Solving the Problems The irradiance meter of the present invention is a pyroelectric radiation detection element, a transmissive diffusion structure that approximates its light-receiving angle sensitivity characteristic to a cosine law, and the pyroelectric radiation detection element An optical shutter that opens and closes the input radiation concentrically with respect to the center of the light receiving surface of the pyroelectric radiation detection element, and converts the photoelectric output from the pyroelectric radiation detection element into a DC output proportional to the amount of incident light. It is composed of a circuit for displaying.
作用 上記構成によれば、光シャッター一回の開閉によって紫
外域から赤外域にいたる広い波長範囲の放射照度を定量
的に精度よく検出できる。Operation According to the above configuration, irradiance in a wide wavelength range from the ultraviolet region to the infrared region can be quantitatively and accurately detected by opening and closing the optical shutter once.
実施例 以下に、本発明の一実施例として光シャッターにソレノ
イドコイルで電気的に同心円状に開閉する虹彩シャッタ
ーを使った放射照度計の実施例を図面を使用して示す。Example An example of an irradiance meter using an iris shutter that opens and closes electrically concentrically with a solenoid coil as an optical shutter will be described below as an example of the present invention with reference to the drawings.
第1図に本実施例の放射照度計の受光部を示す。図にお
いて1は焦電型放射検出素子、2は焦電型放射検出素子
1の入射角感度特性を余弦則に近似せしめる透過拡散構
造物、3は電気的に同心円状に開閉する虹彩シャッタ
ー、4は虹彩シャッター3を開閉するソレノイドコイル
である。FIG. 1 shows the light receiving part of the irradiance meter of this embodiment. In the figure, 1 is a pyroelectric type radiation detection element, 2 is a transmissive diffusion structure that approximates the incident angle sensitivity characteristic of the pyroelectric type radiation detection element 1 to a cosine law, 3 is an iris shutter that opens and closes electrically in concentric circles, 4 Is a solenoid coil for opening and closing the iris shutter 3.
以下に上記の装置の動作原理を示す。第2図のような時
間的に変化の少ない光E(t)を、透過拡散構造物2に
入射させる。このとき虹彩シャッター3をQ(t)なる
時間特性で開閉するとq(t)なる光が前記焦電型放射
検出素子1に入射する。このとき入射光の変化q(t)
は第3図のようになり次式で表わされる。The operating principle of the above device is shown below. Light E (t), which has a small temporal change as shown in FIG. 2, is made incident on the transmissive diffusion structure 2. At this time, when the iris shutter 3 is opened and closed with a time characteristic of Q (t), light of q (t) is incident on the pyroelectric radiation detection element 1. At this time, the change in incident light q (t)
Is as shown in FIG. 3 and is expressed by the following equation.
q(t)=E(t)・Q(t) ……(1) 焦電型放射検出素子1は、第4図(a)に示すように入
射光q(t)の微分に比例した出力電圧R(t)を発生
する。R(t)は次式で表わされる。q (t) = E (t) · Q (t) (1) The pyroelectric radiation detection element 1 outputs an output proportional to the derivative of the incident light q (t) as shown in FIG. 4 (a). Generate a voltage R (t). R (t) is represented by the following equation.
R(t)=dq/dt ……(2) この出力の振れは一過性のもので、しかも微分値である
から電圧の振幅と入射の強さは比例しないので、この電
圧値を測定しても入射光量の測定にはならない。ここで
この微分電圧R(t)を積分回路で積分すると、積分に
よって入射光q(t)に比例する出力S(t)が得られ
る。すなわち、 これを第4図(b)に示す。この復元信号の振幅はE
(t)(第2図のt1〜t2間の値の平均)に比例するよう
になる。実際には、この積分値はコンデンサ等への充電
で行なうが、そのチャージは次第に放電し減衰するの
で、積分終了時(t2)直後にサンプルホールド回路でホ
ールドする。R (t) = dq / dt (2) This output fluctuation is transient, and since it is a differential value, the amplitude of the voltage and the intensity of the incident are not proportional, so measure this voltage value. However, it does not measure the amount of incident light. Here, when the differential voltage R (t) is integrated by the integrating circuit, the output S (t) proportional to the incident light q (t) is obtained by the integration. That is, This is shown in FIG. 4 (b). The amplitude of this restored signal is E
(T) (average of values between t 1 and t 2 in FIG. 2 ). In reality, this integrated value is charged by charging a capacitor or the like, but since the charge is gradually discharged and attenuated, it is held by the sample hold circuit immediately after the end of the integration (t 2 ).
この装置で、シャッター開口時間Δt=|t2−t1|は焦電
型放射検出素子1の微分応答の時定数より十分大きくと
る。In this device, the shutter opening time Δt = | t 2 −t 1 | is set sufficiently larger than the time constant of the differential response of the pyroelectric radiation detection element 1.
測定はシャッターの開閉を随時行なうことによって、繰
返し何度でも実行できる。また、シャッターの動作にバ
ラツキがあってもΔtが十分大きければ微分信号は完全
に取り込めるので、積分した値すなわち測定値は変化し
ない。The measurement can be repeated any number of times by opening and closing the shutter at any time. Further, even if there is a variation in the operation of the shutter, if Δt is sufficiently large, the differential signal can be taken in completely, so the integrated value, that is, the measured value does not change.
測定値の校正は、例えば放射量のわかっている電球を用
いて、その前でシャッターを開閉して行なえばよく、ま
た暗入力の測定は、周囲温度と同温の暗幕などの前で行
なえばよい。Calibration of measured values may be performed, for example, by using a light bulb of known radiation amount and opening and closing the shutter in front of it, and measurement of dark input may be performed in front of a dark curtain at the same temperature as the ambient temperature. Good.
受光器の受光角感度特性は、透過拡散構造物2によって
余弦則に近似させる。透過拡散構造物2からの拡散光は
虹彩シャッター3によって断続され、焦電型放射検出素
子1の受光面に入射する。虹彩シャッター3は焦電型放
射検出素子1の受光面近くに配置する。このとき虹彩シ
ャッター3はソレノイドコイル4で電気的に同心円状に
開閉する。この虹彩シャッター3の同心円状の開閉の中
心と、透過拡散構造物2の中心および焦電型放射検出素
子1の受光面の中心を一致させることによって、虹彩シ
ャッター3の開口が時間的にどのような状態にあって
も、受光器の受光角感度特性は余弦則に近似する。した
がって、虹彩シャッターの開閉によって時間的に受光器
の受光角感度特性は変化せず、その余弦則近似を損なう
ことはない。The light receiving angle sensitivity characteristic of the light receiver is approximated to the cosine law by the transmissive diffusion structure 2. The diffused light from the transmission / diffusion structure 2 is interrupted by the iris shutter 3 and enters the light-receiving surface of the pyroelectric radiation detection element 1. The iris shutter 3 is arranged near the light receiving surface of the pyroelectric type radiation detection element 1. At this time, the iris shutter 3 is electrically opened and closed by the solenoid coil 4 in a concentric pattern. By aligning the center of the concentric opening / closing of the iris shutter 3 with the center of the transmission / diffusion structure 2 and the center of the light-receiving surface of the pyroelectric radiation detection element 1, how the opening of the iris shutter 3 is temporally changed. Even in such a state, the light receiving angle sensitivity characteristic of the light receiver approximates to the cosine law. Therefore, the opening / closing of the iris shutter does not change the light receiving angle sensitivity characteristic of the light receiver with time, and does not impair the cosine law approximation.
虹彩シャッターは、一般にモータ駆動の回転セクターに
比べて、はるかに軽量,薄形である上に、受光素子であ
る焦電型放射検出素子からの入射の見込み角を回転セク
ターより大きくとることができる。また回転セクターの
ように常時駆動する必要がなく、開閉動作は測定時のみ
に限られるので電力の消耗も少ない。このようなことか
ら焦電型放射検出素子とシャッターを用いた放射照度計
は携帯用としても優れた特性を持つ。The iris shutter is generally much lighter and thinner than a motor-driven rotating sector, and can have a larger angle of incidence from the pyroelectric radiation detection element, which is a light receiving element, than the rotating sector. . Further, unlike the rotating sector, it is not necessary to drive it constantly, and since the opening / closing operation is limited to only during measurement, power consumption is small. Therefore, the irradiance meter using the pyroelectric radiation detection element and the shutter has excellent characteristics even when it is portable.
発明の効果 本発明は、焦電型放射検出素子と、その角感度特性を余
弦則に近似せしめる透過拡散構造物と、前記焦電型放射
検出素子への入力放射を前記焦電型放射検出素子受光面
の中心に対して、同心円状に開閉し断続する光シャッタ
ーと、前記焦電型放射検出素子からの光電出力を入射光
量に比例した直流出力に変換し表示する回路からなり、
以下のような効果がある。EFFECTS OF THE INVENTION The present invention provides a pyroelectric radiation detecting element, a transmissive diffusing structure for approximating its angular sensitivity characteristic to a cosine law, and input radiation to the pyroelectric radiation detecting element, the pyroelectric radiation detecting element. With respect to the center of the light receiving surface, an optical shutter that opens and closes concentrically and is intermittent, and a circuit that converts the photoelectric output from the pyroelectric radiation detection element into a DC output proportional to the amount of incident light and displays the result.
It has the following effects.
(1) 光シャッター一回の開閉によって紫外域から赤
外域にいたる広い波長範囲の放射照度を定量的に精度よ
く検出する放射照度計が構成できる。(1) An irradiance meter that quantitatively and accurately detects irradiance in a wide wavelength range from the ultraviolet region to the infrared region can be configured by opening and closing the optical shutter once.
(2) シャッターは、一般にモータ駆動の回転セクタ
ーに比べて、はるかに軽量,薄型である上に、受光素子
である焦電型放射検出素子からの入射の見込み角を回転
セクターより大きくとることができる。このとき光シャ
ッターは同心円状に開閉するので、シャッターの開閉に
よって時間的に受光器の受光角感度特性の変化は小さ
い。したがって受光角感度特性が余弦則に近似した放射
照度計が得られる。(2) The shutter is generally much lighter and thinner than a motor-driven rotating sector, and the angle of incidence from the pyroelectric radiation detection element, which is a light receiving element, can be set larger than that of the rotating sector. it can. At this time, since the optical shutter is opened and closed concentrically, the change in the light receiving angle sensitivity characteristic of the light receiver is small with time due to the opening and closing of the shutter. Therefore, it is possible to obtain the irradiance meter whose light-receiving angle sensitivity characteristic is close to the cosine law.
(3) シャッターは、回転セクターのように常時駆動
する必要がなく、開閉動作は測定時のみに限られるので
電力の消耗も少ない。このようなことから焦電型放射検
出素子とシャッターを用いた放射照度計は小形軽量とな
り、携帯用としても優れた特性を持つ。(3) The shutter does not need to be constantly driven like a rotating sector, and the opening / closing operation is limited to only during measurement, so power consumption is small. For this reason, the irradiance meter using the pyroelectric radiation detection element and the shutter is small and lightweight, and has excellent characteristics for portable use.
第1図は本発明の一実施例における放射照度計の受光部
の断面図、第2図は放射照度計に入射する光の時間的変
化を示す図、第3図は焦電型放射検出素子に入射する光
の時間的変化を示す図、第4図(a)は焦電型放射検出
素子の応答出力を示す図、第4図(b)は焦電型放射検
出素子の応答出力を積分回路で積分した波形を示す図で
ある。 1……焦電型放射検出素子、2……透過拡散構造物、3
……虹彩シャッター、4……ソレノイドコイル。FIG. 1 is a cross-sectional view of a light receiving portion of an irradiance meter in one embodiment of the present invention, FIG. 2 is a view showing a temporal change of light incident on the irradiance meter, and FIG. 3 is a pyroelectric radiation detecting element. FIG. 4 (a) shows the response output of the pyroelectric type radiation detection element, and FIG. 4 (b) shows the integrated response output of the pyroelectric type radiation detection element. It is a figure which shows the waveform integrated by the circuit. 1 ... Pyroelectric radiation detection element, 2 ... Transmission / diffusion structure, 3
...... Iris shutter, 4 ... Solenoid coil.
Claims (1)
出素子の受光角感度特性を余弦則に近似せしめる透過拡
散構造物と、前記焦電型放射検出素子への入力放射を前
記焦電型放射検出素子受光面の中心に対して、同心円状
に開閉し断続する光シャッターと、前記焦電型放射検出
素子からの光電出力を入射光量に比例した直流出力に変
換し表示する回路からなる放射照度計。1. A pyroelectric radiation detecting element, a transmissive diffusing structure for approximating a light-receiving angle sensitivity characteristic of the pyroelectric radiation detecting element to a cosine law, and an input radiation to the pyroelectric radiation detecting element. An optical shutter that opens and closes concentrically with respect to the center of the light receiving surface of the pyroelectric radiation detection element, and a circuit that converts the photoelectric output from the pyroelectric radiation detection element into a direct current output proportional to the amount of incident light and displays it. Irradiometer consisting of.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61051102A JPH0752125B2 (en) | 1986-03-07 | 1986-03-07 | Irradiometer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61051102A JPH0752125B2 (en) | 1986-03-07 | 1986-03-07 | Irradiometer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62207919A JPS62207919A (en) | 1987-09-12 |
| JPH0752125B2 true JPH0752125B2 (en) | 1995-06-05 |
Family
ID=12877445
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61051102A Expired - Lifetime JPH0752125B2 (en) | 1986-03-07 | 1986-03-07 | Irradiometer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0752125B2 (en) |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5323113B2 (en) * | 1972-12-19 | 1978-07-12 | ||
| JPS5767828A (en) * | 1980-10-15 | 1982-04-24 | Kureha Chem Ind Co Ltd | Photodetector |
| JPS58178649U (en) * | 1982-05-25 | 1983-11-29 | 日本遠赤外線株式会社 | infrared detection device |
| JPS59112235A (en) * | 1982-12-18 | 1984-06-28 | Sharp Corp | Temperature sensor |
-
1986
- 1986-03-07 JP JP61051102A patent/JPH0752125B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62207919A (en) | 1987-09-12 |
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