JPH076844B2 - Temperature measurement method - Google Patents
Temperature measurement methodInfo
- Publication number
- JPH076844B2 JPH076844B2 JP308488A JP308488A JPH076844B2 JP H076844 B2 JPH076844 B2 JP H076844B2 JP 308488 A JP308488 A JP 308488A JP 308488 A JP308488 A JP 308488A JP H076844 B2 JPH076844 B2 JP H076844B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- calculated
- color
- camera
- theoretical
- 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 - Fee Related
Links
- 238000000034 method Methods 0.000 title claims description 10
- 238000009529 body temperature measurement Methods 0.000 title description 4
- 230000003595 spectral effect Effects 0.000 claims description 8
- 230000005457 Black-body radiation Effects 0.000 claims description 6
- 238000011088 calibration curve Methods 0.000 claims description 2
- 238000012937 correction Methods 0.000 description 12
- 238000004364 calculation method Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 238000005259 measurement Methods 0.000 description 4
- 238000002485 combustion reaction Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000012544 monitoring process Methods 0.000 description 3
- 239000003086 colorant Substances 0.000 description 1
- 230000000295 complement effect Effects 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 238000011002 quantification Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
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- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は画像情報が得られ、温度測定が必要とされるあ
らゆる対象物、例えばボイラ火炉の火炎温度等の温度測
定法に関する。Description: TECHNICAL FIELD The present invention relates to a method for measuring temperature of any object for which image information is obtained and for which temperature measurement is required, for example, the flame temperature of a boiler furnace.
従来の光学的温度測定法の二色温度計による完全黒体の
温度測定を例に説明する。The temperature measurement of a perfect black body by a conventional two-color thermometer of the optical temperature measurement method will be described as an example.
第5図は、温度をパラメータにとりその黒体からの放射
エネルギを波長に対して表わした、プランクの式による
黒体放射の理論曲線である。FIG. 5 is a theoretical curve of blackbody radiation according to Planck's equation in which the radiant energy from the blackbody is expressed with respect to wavelength with temperature as a parameter.
この式は、各温度に対し一本決まるので、例えばこの図
において、波長Gの700℃の曲線との交点G1、波長Rの
700℃との交点R1との比R1/G1、同様にして750℃曲線
上の比R2/G2、800℃曲線上の比R3/G3は一義的に決定
される。従って逆に対象物の波長GおよびRの放射エネ
ルギを測定すれば、対象物の温度が測定できる。Since one equation is determined for each temperature, for example, in this figure, the intersection point G 1 of the wavelength G with the 700 ° C. curve and the wavelength R
The ratio R 1 / G 1 with the intersection R 1 with 700 ° C., the ratio R 2 / G 2 on the 750 ° C. curve, and the ratio R 3 / G 3 on the 800 ° C. curve are uniquely determined. Therefore, conversely, the temperature of the object can be measured by measuring the radiant energy of the wavelengths G and R of the object.
この曲線は完全黒体に対するものであるが、その放射
が、係数ε(0<ε≦1)の倍率で異なる灰色体におい
ても、例えばこのR,Gの二波長を用いれば、係数εの影
響なく温度が測定できる。このように二波長における放
射エネルギを測定しその比から温度を求める方法を二色
温度計と云い、工業的にも広く利用されている。This curve is for a perfect black body, but even for a gray body whose emission varies with the magnification of the coefficient ε (0 <ε ≦ 1), if the two wavelengths of R and G are used, the effect of the coefficient ε is affected. The temperature can be measured without. The method of measuring the radiant energy at two wavelengths and obtaining the temperature from the ratio is called a two-color thermometer and is widely used industrially.
第6図は二色温度計の構成を示す。FIG. 6 shows the structure of a two-color thermometer.
測定対象物1からの光を波長Rのみを通過させる狭帯域
フィルタ2及び波長Gのみを通過させる狭帯域フィルタ
3で受け、それらの背後に置れた光‐電変換器4を通し
て演算回路5に入力し、両入力比、すなわち二色比より
測定対象物の温度が演算々出されていた。The light from the measurement object 1 is received by a narrow band filter 2 that allows only the wavelength R to pass and a narrow band filter 3 that allows only the wavelength G to pass, and is passed to a calculation circuit 5 through a photoelectric converter 4 placed behind them. The temperature of the measurement object was calculated and calculated from both input ratios, that is, the two-color ratio.
上記従来の二色温度計は、ごく狭い部分の温度を計測す
るには適している。例えば、ボイラ火炉内を二色温度計
で計測すると、所望の1点の温度は判るものの、全体の
温度分布は判らなかった。The above conventional two-color thermometer is suitable for measuring the temperature of a very narrow portion. For example, when the inside of the boiler furnace was measured by a two-color thermometer, the temperature at a desired point was known, but the entire temperature distribution was not known.
本発明は上記課題を解決するため次の手段を講ずる。 The present invention takes the following means in order to solve the above problems.
測定対象物に向けられたカラーテレビジョンカメラの、
各映像点毎の各カラー出力をデコーダでR(赤)、G
(緑)及びB(青)信号に分解し、同R(赤)、G
(緑)及びB(青)の出力にγ逆補正を施し、R/G等の
二色比の複数組を計算するとともに温度をパラメータと
した黒体放射の理論曲線をカラーテレビジョンカメラの
分光特性で補正して得られる較正曲線により予め求めた
理論R(赤)、G(緑)及びB(青)信号の二色比の複
数組を計算し、これら二組の二色比を用いて上記測定対
象物の温度を上記各映像点毎に算出することを特徴とす
る温度計測方法。Of a color television camera aimed at the object to be measured,
Decoder for each color output for each video point R (red), G
Separated into (green) and B (blue) signals, the same R (red), G
Γ inverse correction is applied to the outputs of (green) and B (blue), multiple sets of dichroic ratios such as R / G are calculated, and the theoretical curve of black body radiation with temperature as a parameter is used to analyze the spectrum of a color television camera. A plurality of sets of dichroic ratios of theoretical R (red), G (green) and B (blue) signals obtained in advance by a calibration curve obtained by correcting the characteristics are calculated, and the dichroic ratios of these two sets are used. A temperature measuring method, characterized in that the temperature of the measuring object is calculated for each of the image points.
上記の方法により、計測対象物に向けられたカラーテレ
ビジョンカメラの信号から各映像点毎にデコーダでR,G
及びB信号が算出され、γ逆補正された後、二色比が計
算されるとともに予め黒体放射の理論曲線を、カラーテ
レビジョンカメラの分光特性で補正を行なった理論R,G
及びB信号の二色比が計算され、これらの二組の二色比
から上記各映像点毎の温度が計算出力される。By the above method, the R, G is detected by the decoder for each video point from the signal of the color television camera aimed at the measurement object.
And B signals are calculated, and γ is inversely corrected, then the dichroic ratio is calculated, and the theoretical curves of black body radiation are corrected in advance with the theoretical characteristics of the color characteristics of the color television camera R, G.
And the dichroic ratio of the B signal is calculated, and the temperature for each image point is calculated and output from these two sets of dichroic ratios.
このようにして、計測対象物の温度分布が容易に得られ
る。In this way, the temperature distribution of the measurement object can be easily obtained.
本発明の方法を適用した一実施例を第1図ないし第4図
により説明する。An embodiment to which the method of the present invention is applied will be described with reference to FIGS.
第1図は同実施例の構成図、第2図は第1図のカラーテ
レビジョンカメラのγ特性説明図、第3図は第1図のカ
ラーテレビジョンカメラの分光特性図、第4図は上記実
施例のカラーテレビカメラの分光特性による補正法説明
図である。FIG. 1 is a configuration diagram of the same embodiment, FIG. 2 is an explanatory diagram of .gamma. Characteristics of the color television camera of FIG. 1, FIG. 3 is a spectral characteristic diagram of the color television camera of FIG. 1, and FIG. It is explanatory drawing of the correction method by the spectral characteristic of the color television camera of the said Example.
第1図にてカラーテレビジョンカメラ(以後カメラと略
記する)10の各映像点毎の出力はデコーダ11に入力され
る。同デコーダ11のR(赤)、G(緑)及びB(青)の
出力はγ逆補正回路12を経て二色比温度演算手段13へ入
力される。さらに同二色比温度演算手段13は補正付理論
曲線手段14の出力を受けて演算し温度を出力する。In FIG. 1, an output for each image point of a color television camera (hereinafter abbreviated as a camera) 10 is input to a decoder 11. The R (red), G (green) and B (blue) outputs of the decoder 11 are input to the dichroic ratio temperature calculation means 13 via the γ inverse correction circuit 12. Further, the two-color-ratio temperature calculating means 13 receives the output of the corrected theoretical curve means 14 and calculates and outputs the temperature.
以上の構成において、カメラの信号は、一般に日本にお
ける標準テレビ方式であるNTSC方式に従って信号処理さ
れ、デコーダに送られこゝで、R(赤)、G(緑)、B
(青)の三色に分解された信号が取り出される。In the above configuration, the camera signal is generally processed according to the NTSC system, which is a standard television system in Japan, and sent to the decoder, where R (red), G (green) and B
The signal decomposed into the three colors of (blue) is extracted.
テレビジョン受像機のブラウン管は、その入力電圧に対
して第2図の受像機曲線に示されるように、その出力即
ち画面の明るさは直線的に変化しない特性を有してい
る。そこで、カメラ側では、光の入力に対し、カメラ曲
線に示されるように、受像機曲線の補完をするように低
い入力のとき実際より大きな電圧を出力するような特性
を持たせ、カメラと受像機両方の特性が相補的に働らい
て受像機の画面には、カメラに入力した明るさと同じ明
るさが再現される、この曲線対がギリシャ文字γに似て
いることからこの補正をγ補正という。The cathode ray tube of a television receiver has a characteristic that its output, that is, the brightness of the screen, does not change linearly with respect to its input voltage, as shown in the receiver curve of FIG. Therefore, on the camera side, as shown in the camera curve, the camera side has a characteristic that a voltage larger than the actual voltage is output at the time of a low input so as to complement the receiver curve, and the camera and the image The characteristics of both units work complementarily, and the same brightness as the brightness input to the camera is reproduced on the screen of the receiver.Since this curve pair is similar to the Greek letter γ, this correction is γ correction Say.
又カメラは、人間に画像を再現して示すことが主たる目
的であるから、第3図の如き人の眼の視感度に近い分光
特性を有しており、単一波長の光のみを選択的にとりこ
むようにはなっていない。Further, since the camera is mainly intended to reproduce and show an image to a human, it has a spectral characteristic close to the luminosity of the human eye as shown in FIG. 3 and selectively selects light of a single wavelength. I'm not supposed to take in.
そこで温度を測定するために、このカメラの出力信号を
用いようとすると、二色温度計の例えばR,Gの信号に対
し波長幅が拡がっている分のエネルギがカメラに入り出
力されていると考え、理論曲線上にこの分光特性をのせ
それぞれの波長に対する入射エネルギの積分としてカメ
ラの出力を考える。Therefore, when trying to use the output signal of this camera to measure the temperature, it is said that the energy corresponding to the wavelength width expanded with respect to the R, G signals of the dichroic thermometer is output to the camera. Considering this, the spectral output is placed on the theoretical curve, and the output of the camera is considered as the integral of the incident energy for each wavelength.
さて、第1図の構成で、γ逆補正によりR,G,及びBに戻
された信号は、この次にγの逆補正を設け初めて入力に
忠実に比例した信号となる。次に二色温度演算手段で二
色比の複数組が計算され、あらかじめ計算されていた補
正付の理論曲線手段から得られる理論出力の同二色比と
照合され前記映像点毎の温度がこれら二種類の二色比か
ら計算され出力される。Now, in the configuration of FIG. 1, the signal returned to R, G, and B by the γ inverse correction becomes a signal that is faithfully proportional to the input only after the γ inverse correction is provided next. Next, a plurality of sets of dichroic ratios are calculated by the dichroic temperature calculation means, and the calculated dichroic ratios of theoretical outputs obtained from the theoretical curve means with correction, which have been calculated in advance, are collated and the temperatures at the respective image points are calculated as follows. It is calculated from two types of two-color ratio and output.
上記補正付の理論曲線手段の計算法を以下に述べる。The calculation method of the above theoretical curve means with correction will be described below.
第4図において、パラメータT=T0の黒体放射理論曲
線上で、例えば中心波長Rのカメラの赤成分出力は、カ
メラの分光特性のRの値を1として、(1)式のように表
わしこれを二色法における一つの波長の出力とする。In FIG. 4, on the black body radiation theoretical curve with the parameter T = T 0 , for example, the red component output of the camera with the center wavelength R is given by the equation (1), where R is the spectral characteristic of the camera. This is the output of one wavelength in the dichroic method.
S′R=W0・y0+W1・y1+W2・y2……Wn・yn …
(1) さらに、分光特性上Rのピークの値を乗じ、最終的な温
度T0におけるRのカメラの理論出力は(2)式で表され
る。S ′ R = W 0 · y 0 + W 1 · y 1 + W 2 · y 2 …… W n · y n・ ・ ・
(1) Further, the theoretical output of the R camera at the final temperature T 0 is expressed by the equation (2) by multiplying the R peak value on the spectral characteristic.
S′R=CRS′R ………(2) 以上のようにして、カメラの信号から各映像点毎の温度
データが容易に得られるため、火炎等の温度分布が把握
でき、燃焼の監視及び制御手段として極めて役立つもの
となる。S ′ R = C R S ′ R (2) As described above, since temperature data for each image point can be easily obtained from the camera signal, the temperature distribution of flames and the like can be grasped and combustion It is extremely useful as a monitoring and control means.
〔発明の効果〕 本発明は次の効果を奏する。[Effects of the Invention] The present invention has the following effects.
従来、人が火炎を肉眼で監視することを目的として、設
置されていたテレビカラーカメラの信号(映像)から、
物理的定量性を有する温度データが計測できることによ
り、その分布等を含めて、燃焼の定量的把握あるいは他
火炎との比較が可能となり、より正確な燃焼の監視ある
いは、制御センサとしての情報が得られるようになる。Conventionally, from the signal (video) of the TV color camera that was installed for the purpose of monitoring the flame with human eyes,
By being able to measure temperature data with physical quantification, it is possible to quantitatively grasp combustion, including its distribution, and compare it with other flames, and obtain more accurate combustion monitoring or information as a control sensor. Will be available.
第1図は本発明の構成図、第2図は従来のカラーテレビ
ジョンカメラのγ特性説明図、第3図は従来のカメラの
分光特性、第4図は第1図の補正付理論曲線手段の計算
説明図、第5図は従来の黒体放射理論曲線、第6図は従
来の二色式温度計の原理図。 図中、 1……測定対象物、2……Rフィルタ、 3……Gフィルタ、4……光‐電変換器、 5……演算回路、 10……カラーテレビジョンカメラ、 11……デコーダ、12……γ逆補正回路、 13……二色比温度演算手段、 14……補正付理論曲線手段。FIG. 1 is a block diagram of the present invention, FIG. 2 is an explanatory view of .gamma. Characteristics of a conventional color television camera, FIG. 3 is a spectral characteristic of a conventional camera, and FIG. 4 is a theoretical curve means with correction of FIG. Fig. 5 shows the conventional black body radiation theoretical curve, and Fig. 6 shows the principle of the conventional two-color thermometer. In the figure, 1 ... Object to be measured, 2 ... R filter, 3 ... G filter, 4 ... Photoelectric converter, 5 ... Operation circuit, 10 ... Color television camera, 11 ... Decoder, 12 …… γ reverse correction circuit, 13 …… two-color ratio temperature calculation means, 14 …… correction theoretical curve means.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 高比良 幸美 長崎県長崎市飽の浦町1番1号 三菱重工 業株式会社長崎造船所内 (72)発明者 佐藤 康彦 長崎県長崎市飽の浦町1番1号 三菱重工 業株式会社長崎研究所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Yukiko Takahira 1-1, Atsunoura Town, Nagasaki City, Nagasaki Prefecture Mitsubishi Heavy Industries Ltd. Nagasaki Shipyard (72) Inventor Yasuhiko Sato 1-1, Atsunoura Town, Nagasaki City, Nagasaki Prefecture Mitsubishi Heavy Industry Co., Ltd. Nagasaki Research Institute
Claims (1)
ンカメラの、各映像点毎の各カラー出力をデコーダでR
(赤)、G(緑)及びB(青)信号に分解し、同R
(赤)、G(緑)及びB(青)の出力にγ逆補正を施
し、R/G等の二色比の複数組を計算するとともに温度を
パラメータとした黒体放射の理論曲線をカラーテレビジ
ョンカメラの分光特性で補正して得られる較正曲線によ
り予め求めた理論R(赤)、G(緑)及びB(青)信号
の二色比の複数組を計算し、これら二組の二色比を用い
て上記測定対象物の温度を上記各映像点毎に算出するこ
とを特徴とする温度計測方法。1. A decoder outputs each color output of each image point of a color television camera directed to an object to be measured.
(Red), G (green) and B (blue) signals
The outputs of (red), G (green) and B (blue) are inversely corrected by γ, multiple sets of dichroic ratios such as R / G are calculated, and the theoretical curve of blackbody radiation with temperature as a parameter is colored. Plural sets of dichroic ratios of theoretical R (red), G (green) and B (blue) signals obtained in advance by a calibration curve obtained by correcting the spectral characteristics of the television camera are calculated, and two sets of these two sets are calculated. A temperature measuring method, wherein the temperature of the measuring object is calculated for each of the image points by using a color ratio.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP308488A JPH076844B2 (en) | 1988-01-12 | 1988-01-12 | Temperature measurement method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP308488A JPH076844B2 (en) | 1988-01-12 | 1988-01-12 | Temperature measurement method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01180430A JPH01180430A (en) | 1989-07-18 |
| JPH076844B2 true JPH076844B2 (en) | 1995-01-30 |
Family
ID=11547475
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP308488A Expired - Fee Related JPH076844B2 (en) | 1988-01-12 | 1988-01-12 | Temperature measurement method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH076844B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6814484B2 (en) | 2001-01-17 | 2004-11-09 | Noritake Co., Limited | Temperature distribution measuring method and apparatus |
| US6817758B2 (en) | 2001-04-04 | 2004-11-16 | Noritake Co., Limited | Temperature distribution measuring method and apparatus |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3639701B2 (en) * | 1997-09-24 | 2005-04-20 | キヤノン株式会社 | Measuring device, light source characteristic value calculating device and calculating method thereof |
| JP2013152194A (en) * | 2012-01-26 | 2013-08-08 | Buriizu:Kk | Infrared camera and temperature detection method of infrared emission source |
-
1988
- 1988-01-12 JP JP308488A patent/JPH076844B2/en not_active Expired - Fee Related
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6814484B2 (en) | 2001-01-17 | 2004-11-09 | Noritake Co., Limited | Temperature distribution measuring method and apparatus |
| US6817758B2 (en) | 2001-04-04 | 2004-11-16 | Noritake Co., Limited | Temperature distribution measuring method and apparatus |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01180430A (en) | 1989-07-18 |
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