JPS6130728A - Measurement of infrared radiation temperature - Google Patents
Measurement of infrared radiation temperatureInfo
- Publication number
- JPS6130728A JPS6130728A JP15352484A JP15352484A JPS6130728A JP S6130728 A JPS6130728 A JP S6130728A JP 15352484 A JP15352484 A JP 15352484A JP 15352484 A JP15352484 A JP 15352484A JP S6130728 A JPS6130728 A JP S6130728A
- Authority
- JP
- Japan
- Prior art keywords
- temp
- circuit
- temperature
- measured
- amplifier
- 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
Links
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
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/02—Constructional details
- G01J5/08—Optical arrangements
- G01J5/0803—Arrangements for time-dependent attenuation of radiation signals
- G01J5/0805—Means for chopping radiation
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Radiation Pyrometers (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、熱容量の少ない物体、遠方物体、移動物体等
の温度を非接触で測定する赤外線放射温度の測定方法に
関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an infrared radiation temperature measuring method for non-contactly measuring the temperature of an object with low heat capacity, a distant object, a moving object, etc.
従来例の構成とその問題点
第1図は従来の赤外線放射温度の測定方法を示す図であ
シ、同図で、1は測定系に到来する被測定物体の赤外線
エネルギー、2は赤外線エネルギー1を集光するだめの
光学系、3はモータ、4はモータ3により回転駆動され
る複数のスリノトヲ有するチョッパ、6は測定温度の基
準値を与える基準黒体、6は赤外線の検出器で、焦電効
果を利用したパイロ素子等が使用される。7.8は増幅
器、9はサーミスタ等の測温素子、10はホトインタラ
プタ等のチョッパの回転数検出器、11はデータ処理機
、12は温度等の表示器、13はモータの回転速度を精
密にコントロールするモ〜り制御回路である。Configuration of the conventional example and its problems Figure 1 is a diagram showing the conventional method for measuring infrared radiation temperature. 3 is a motor, 4 is a chopper having a plurality of slots rotated by the motor 3, 6 is a reference black body that provides a reference value for the measured temperature, 6 is an infrared detector, and 6 is an infrared detector. A pyro element or the like that utilizes the electric effect is used. 7.8 is an amplifier, 9 is a temperature measuring element such as a thermistor, 10 is a chopper rotation speed detector such as a photointerrupter, 11 is a data processor, 12 is a display for temperature, etc., and 13 is a precision sensor for measuring the rotational speed of the motor. This is a motor control circuit that controls the
上記構成で温度を検出するには、被測定物の赤外線エネ
ルギー1を光学系2により検出器6上に焦点を結ばせる
一方で、基準黒体6からの赤外線エネルギーをチョッパ
4により交流に直した上で検出器らにより検出している
。チョッパ4には羽根の一部にスリットが設けられてい
るので、スリットを通過する赤外線量は被測定物体の温
度TMに比例し、またスリノ)・が無い状態ではチョッ
パ4の表面で反射した基準黒体の温度T。に比例するこ
とになる。但し、検出器6としてパイロ型の検出素子を
用いた時には出力は温度T、とT。の差TB に依存す
る。To detect the temperature with the above configuration, the infrared energy 1 of the object to be measured is focused on the detector 6 by the optical system 2, while the infrared energy from the reference black body 6 is converted into alternating current by the chopper 4. It is detected by the detectors above. Since the chopper 4 has a slit in a part of the blade, the amount of infrared rays passing through the slit is proportional to the temperature TM of the object to be measured. Blackbody temperature T. It will be proportional to. However, when a pyro-type detection element is used as the detector 6, the output is the temperature T. depends on the difference TB.
一般に、検出器にパイロ型の検出素子を用いた時には出
力IVIは下記(1)式のように与えられることが知ら
れている。Generally, it is known that when a pyro-type detection element is used as a detector, the output IVI is given as shown in equation (1) below.
ここでkは定数(−1)、Cは検出器の容量、ω′は検
出器の比熱、ρは検出器の密度、hは検出器の厚さ、ω
はチ”!7パの周波数(2πf)、εfd放射L σは
ステファンボルツマン定?(−5,673X10 W
−a*deg’)、TB は被測定物と基準黒体の温度
差、Abはパイロ定数(=T
6、OX 10 coul/z 0K )。where k is a constant (-1), C is the capacitance of the detector, ω' is the specific heat of the detector, ρ is the density of the detector, h is the thickness of the detector, ω
Hachi”! 7P frequency (2πf), εfd radiation L σ is Stefan Boltzmann constant? (-5,673X10 W
-a*deg'), TB is the temperature difference between the measured object and the reference black body, and Ab is the pyro constant (=T 6, OX 10 coul/z 0K).
従って、出力Vから基準黒体6の温度(To)が既知で
あるとして被測定物の温度(TM)が求まることになる
。この場合、検出器6の出力は増幅器7を経由してデー
タ処理機11に、入力される。増幅器7の出力はチョッ
パ4により交流に変換され、れているので、回転数検出
器10の出力で前記交流出力を同期整流すると共に、測
温素子9による基準黒体6の温度情報を増幅器8を介し
て同様にデータ処理機11に入力し、前述のように(1
)式の関係から被測定物の温度TM(i7演算により求
め表示器12に表示することが出来る。しかしながら、
被測定物の温度TMとToの差に比例して変化するため
に、例えば300’Cの時の検出器の電圧は2000’
Cになると、約10倍になるため、増幅器のダイナミッ
クレンジ内に入れることが出来ず測定範囲が狭くなって
しまう欠点があった。Therefore, the temperature (TM) of the object to be measured can be determined from the output V assuming that the temperature (To) of the reference black body 6 is known. In this case, the output of the detector 6 is input to the data processor 11 via the amplifier 7. Since the output of the amplifier 7 is converted into alternating current by the chopper 4, the alternating current output is synchronously rectified by the output of the rotation speed detector 10, and the temperature information of the reference black body 6 from the temperature measuring element 9 is sent to the amplifier 8. is similarly input to the data processor 11 via , and as described above (1
) The temperature of the object to be measured TM (i7 calculation) can be determined and displayed on the display 12. However,
Since it changes in proportion to the difference between the temperature TM and To of the object to be measured, for example, the voltage of the detector when the temperature is 300'C is 2000'C.
When it comes to C, it becomes about 10 times as large, so it has the disadvantage that it cannot be placed within the dynamic range of the amplifier, resulting in a narrow measurement range.
発明の目的
本発明は、上記従来例の欠点を除去するもので、測定範
囲が増加しても温度分解能を低下させることなく、測定
可能とする赤外線放射温度の測定方法を提供することを
目的とするものである。Purpose of the Invention The present invention eliminates the drawbacks of the conventional examples described above, and aims to provide a method for measuring infrared radiation temperature that can be measured without reducing temperature resolution even if the measurement range increases. It is something to do.
発明の構成
本発明は、上記目的を達成するために、検出器の感度が
、チョッパの周波数に依存される事を利用するもので、
検出器からの出力が予め定められた範囲を越えると、チ
ラッパの周波数を高くして増幅器のダイナミックレンジ
内に納めるものであシ、範囲の広い温度を測定する効果
を得ることができる。 □
実施例の説明
以下に本発明の測定方法について図面を参照して説明す
る。第2図で、16は増幅器7からの測定値と増幅器8
からの基準黒体温度情報を選択合成するだめのマルチプ
レクサ(MPX)、16はアナログデジタルコンバータ
(ム/D )、1−rはA/D16とフォトインタラプ
タ等の回転数検出器10の出力を入力して被測定物の温
度TMを求めるための演算を行なうデータ処理機であり
、内部に演算回路18.補正量発生回路19を備えてお
り、必要によりマイクロコンピュータを使用して処理し
ても良い。他の第1図と同様の符号は同一の名称を表わ
すものである。Structure of the Invention In order to achieve the above object, the present invention utilizes the fact that the sensitivity of the detector depends on the frequency of the chopper.
When the output from the detector exceeds a predetermined range, the frequency of the chipper is raised to stay within the dynamic range of the amplifier, making it possible to measure temperatures over a wide range. □ Description of Examples The measurement method of the present invention will be described below with reference to the drawings. In FIG. 2, 16 indicates the measured value from amplifier 7 and amplifier 8.
16 is an analog-to-digital converter (MU/D), 1-r is an input of the output of A/D 16 and a rotation speed detector 10 such as a photointerrupter. This is a data processing machine that performs calculations to determine the temperature TM of the object to be measured, and has an internal calculation circuit 18. A correction amount generation circuit 19 is provided, and a microcomputer may be used for processing if necessary. The same reference numerals as in other FIG. 1 represent the same names.
次に動作を説明する。演算回路18は前記(1)式の逆
演算によシ、基準黒体を使用して、被測定物の温度T、
を求める点では従来例と同様であるが、゛(1)式にお
いて従来測定温度が変化してもチョッパの周波数ωを一
定に保とうとしたのに対し、本実施例の方法では、演算
回路18の出力から得られる測定温度情報と基準黒体温
度情報により、測定温度が変化した場合にモータ3の回
転数をこれに追従して変化するように補正量発生回路1
9により段階的に数通りの補正信号(ω′)を発生させ
る。Next, the operation will be explained. The arithmetic circuit 18 calculates the temperature T of the object to be measured,
However, in the method of this embodiment, the frequency ω of the chopper was kept constant even if the measured temperature changed in the conventional example (1), but in the method of the present example, the calculation circuit 18 Based on the measured temperature information and reference blackbody temperature information obtained from the output of
9, several types of correction signals (ω') are generated in stages.
この場合測定温度が変化しても演算回路18の出力は一
定に保たれることになるが、補正信号(ω′)の値を演
算回路18の演算時の入力情報として利用して、測定値
を求め、表示器12により表示すれば良い。In this case, even if the measured temperature changes, the output of the arithmetic circuit 18 will be kept constant, but the value of the correction signal (ω') is used as input information for the arithmetic operation of the arithmetic circuit 18, and the measured value What is necessary is to find it and display it on the display 12.
なお、上記構成においてデータ処理機17の構成自体は
公知の技術を用いて容易に行ない得る。In addition, in the above configuration, the configuration of the data processor 17 itself can be easily performed using a known technique.
また、A/D16はデータ処理機17に扱えるようにア
ナログデータをデジタル変換するためのものである。Further, the A/D 16 is for converting analog data into digital data so that it can be handled by the data processor 17.
発明の効果
以上の説明から明らかなように本発明によれば増幅器よ
シ得られる電圧は、例えば3o○°Cの場合と2000
’Cの場合では、約10倍となり、従ってチョッパの周
波数を約10倍とすれば増幅器の増幅度を変える事無く
測定温度範囲を拡大する事ができる。又チョッパの周波
数は例えばフメトインタラグタで測定する事により、多
少の誤差が有っても演算する事により、測定誤差を生じ
ない利点が有る。Effects of the Invention As is clear from the above explanation, according to the present invention, the voltage obtained from the amplifier is different from that at 3°C and 2000°C.
In the case of 'C, it becomes about 10 times, and therefore, by increasing the chopper frequency about 10 times, the measurement temperature range can be expanded without changing the amplification degree of the amplifier. Furthermore, by measuring the frequency of the chopper using, for example, a fumetointerlager, there is an advantage that no measurement error occurs because the calculation is performed even if there is some error.
第1図は従来の赤外線放射温度の測定方法を説明するだ
めのブロック図、第2図は本発明の赤外線放射温度の測
定方法を説明するだめの一実施例のブロック図である。
4・・・・・・チョッパ、5・・・・・基準黒体、6・
・・・・・検出器、18・・・・・演算回路、19・・
・・・・補正量発生回路。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
第2図FIG. 1 is a block diagram for explaining a conventional method for measuring infrared radiation temperature, and FIG. 2 is a block diagram for explaining an embodiment of the method for measuring infrared radiation temperature according to the present invention. 4...Chopper, 5...Reference black body, 6...
...Detector, 18...Arithmetic circuit, 19...
...Correction amount generation circuit. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2
Claims (1)
外線エネルギーをモータにより回転するチョッパを介し
て検出器に交互に導入し、前記検出器の出力と前記基準
黒体の温度測定値から前記被測定物体の温度を演算によ
り算出するに際し、前記モータの回転数を変化して前記
演算結果が被測定物の温度変化に対し一定値になるよう
に補正することを特徴とする赤外線放射温度の測定方法
。Infrared energy from the object to be measured and infrared energy from the reference blackbody are alternately introduced into the detector via a chopper rotated by a motor, and the output of the detector and the temperature measurement value of the reference blackbody are used to calculate the temperature of the object to be measured. A method for measuring infrared radiation temperature, characterized in that when calculating the temperature of an object by calculation, the rotation speed of the motor is changed to correct the calculation result so that it becomes a constant value with respect to temperature changes of the object to be measured. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15352484A JPS6130728A (en) | 1984-07-24 | 1984-07-24 | Measurement of infrared radiation temperature |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15352484A JPS6130728A (en) | 1984-07-24 | 1984-07-24 | Measurement of infrared radiation temperature |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6130728A true JPS6130728A (en) | 1986-02-13 |
Family
ID=15564410
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15352484A Pending JPS6130728A (en) | 1984-07-24 | 1984-07-24 | Measurement of infrared radiation temperature |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6130728A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5169234A (en) * | 1990-02-13 | 1992-12-08 | Ultrakust Electronic Gmbh | Infrared temperature sensor |
| JP2017500565A (en) * | 2013-12-13 | 2017-01-05 | ブレイン・テンプ,インコーポレーテッド | Error reduction in radiation-based temperature measurement systems |
-
1984
- 1984-07-24 JP JP15352484A patent/JPS6130728A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5169234A (en) * | 1990-02-13 | 1992-12-08 | Ultrakust Electronic Gmbh | Infrared temperature sensor |
| JP2017500565A (en) * | 2013-12-13 | 2017-01-05 | ブレイン・テンプ,インコーポレーテッド | Error reduction in radiation-based temperature measurement systems |
| US9958343B2 (en) | 2013-12-13 | 2018-05-01 | Brain Temp, Inc. | Error reduction in radiation-based temperature measurement systems |
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