JP2020128981A - Temperature measuring method - Google Patents

Abstract

To more accurately measure the temperature of a measurement object while suppressing a measured temperature difference at an end of a substance.SOLUTION: The present invention pertains to a temperature measuring method for detecting heat radiation light of near-infrared band that is emitted by a measurement object and measuring the temperature of the measurement object on the basis of detection result of the radiance of the heat radiation light. Using a bicolor radiation thermometer comprising a light receiving unit for receiving the heat radiation light of the measurement object, a detection unit for detecting the heat radiation light received by the light receiving unit and a position control mechanism for changing the relative positional relation of the measurement object and the light receiving unit and causing the distribution of the heat radiation light in the widthwise direction of the measurement object to be measured by the light receiving unit, this method detects the heat radiation light of the measurement object and measures a temperature distribution along the widthwise direction of the measurement object.SELECTED DRAWING: Figure 18A

Description

The present invention relates to a temperature measuring method.

Radiation thermometry is a method of knowing the temperature of the target object by detecting the thermal radiation light emitted by the object according to the temperature with a measuring device such as a radiation thermometer, and it is possible to measure the temperature non-contact and at high speed. It is a remote temperature measuring method. Today, many industries, including the steel industry, use such radiation thermometry.

For example, the following Patent Document 1 discloses a technique of measuring the surface temperature of a slab being cast by a continuous casting machine by a radiation temperature measuring method.

JP, 2014-36988, A

The radiation thermometer used in Patent Document 1 is a so-called “monochromatic radiation thermometer” that calculates the temperature of the measurement object based on the energy intensity of the thermal radiation light at one wavelength of interest. However, since the monochromatic radiation thermometer derives the temperature from the energy intensity in the measurement visual field, the measurement visual field is lacking at the end (corner portion) of the object (hereinafter, also simply referred to as “missing visual field”). ), temperature measurement error (more specifically, error due to underestimating the temperature of the corner portion) occurs.

Further, in an actual production line in a steel mill, it is necessary to separate the radiation thermometer from the object by at least about 3 to 4 m, and the circular measurement diameter of the monochromatic radiation thermometer is about 40 to 50 mm. On the other hand, in monitoring the temperature during manufacturing, it is important to correctly measure the temperature of the steel end, and the temperature near the corner will drop in the range of the above measurement diameter, and the steel end The temperature of the part cannot be measured correctly.

Therefore, the present invention has been made in view of the above problems, and an object of the present invention is to measure the temperature of a measurement object more accurately while suppressing the temperature measurement error at the end of the object. An object of the present invention is to provide a temperature measurement method capable of performing the above.

In order to solve the above problems, according to an aspect of the present invention, the thermal radiation of the near infrared band emitted by the measurement object is detected, and the measurement is performed based on the detection result of the radiance of the thermal radiation. A temperature measuring method for measuring the temperature of an object, the light receiving section for receiving the thermal radiation of the measuring object, a detection section for detecting the thermal radiation received by the light receiving section, and the measuring object. Two-color radiation thermometer having a position control mechanism that changes the relative positional relationship between an object and the light-receiving unit, and causes the light-receiving unit to measure the distribution of the thermal radiation light in the width direction of the measurement object. Is used to detect the thermal radiation of the measurement object and measure a temperature distribution along the width direction of the measurement object including the vicinity of the end of the measurement object. ..

The two-color radiation thermometer, the minimum radiant light amount that is the minimum radiant light amount required for temperature calculation in the measurement field of view of the two-color radiation thermometer is specified in advance, the position control mechanism, the two-color It is preferable to change the relative positional relationship between the measurement object and the light receiving unit until the amount of emitted light detected in the measurement field of view of the radiation thermometer becomes less than the minimum amount of emitted light.

The position control mechanism may be an angle control mechanism that changes an angle formed by the surface normal direction of the measurement target and the optical axis of the light receiving unit.

The angle control mechanism, between the measurement object and the light guide optical system that guides the thermal radiation light to the detection unit, a mirror provided obliquely to the surface normal direction, The angle formed by the surface normal direction and the optical axis of the light receiving section may be changed by rotating the measurement object by a predetermined angle with the longitudinal direction as a rotation axis.

The position control mechanism may be a drive mechanism that moves the light receiving unit along the width direction of the measurement target.

The two-color radiation thermometer is a two-color radiation thermometer capable of independently outputting the radiance of the thermal radiation light at each of two types of wavelengths of interest, and the temperature in the width direction of the measurement target. While scanning the distribution, in the range of the measurement field of the radiance in the two-color radiation thermometer, if something other than the measurement object is located, the two-color radiation thermometer, The temperature of the measurement target is measured using the radiance of the thermal radiation at each of the two wavelengths to be measured, and when the measurement target occupies the range of the measurement field of view, The color radiation thermometer may measure the temperature of the measurement object by using the radiance of the thermal radiation light of one of the two types of wavelengths of interest.

The distance from the two-color radiation thermometer to the measurement object is H [mm], the size of the measurement diameter of the two-color radiation thermometer is D _L [mm], and the width of the measurement object is W[ mm], the two-color radiation thermometer is a two-color radiation thermometer capable of independently outputting the radiance of the thermal radiation light at each of the two wavelengths of interest, and As a position control mechanism, the surface normal direction of the measurement object, and has an optical axis of the light receiving unit, and has an angle control mechanism for changing the angle formed, the temperature distribution in the width direction of the measurement object. During scanning, the size of the angle formed by the surface normal direction of the measurement object and the optical axis of the light receiving unit is |φ|=|tan ^-1 [{(W/2)-(D _L 2)}/H]|, the two-color radiation thermometer uses the radiance of the thermal radiation at each of the two wavelengths of interest, The temperature of the measurement target is measured, and the size of the angle formed by the surface normal direction of the measurement target and the optical axis of the light receiving unit is |φ|=|tan ^-1 [{(W/2) -(D _L /2)}/H]|, the two-color radiation thermometer determines whether the thermal radiation light of either one of the two wavelengths of interest is The temperature of the measurement object may be measured using the radiance.

The dichroic thermometer calculates a dichroic ratio obtained by dividing one of the measurement data of the radiance at two types of wavelengths of interest by the other, and using the calculated dichroic ratio, the dichroic ratio is calculated. The temperature of the measurement object may be calculated based on a relational expression between the temperature and the temperature.

The two-color radiation thermometer, in a state in which the absorber having wavelength dependence on the spectral absorption coefficient in the near-infrared band is present in at least part of the optical path, the thermal radiation light of the measurement object. , Measuring data at two wavelengths having the same spectral absorption coefficient of the absorber, and generating measurement data showing a detection result of radiance of the thermal radiation light at the two wavelengths. The temperature of the measurement object may be calculated based on the measured data corresponding to the two types of wavelengths thus obtained and the relational expression between the spectral radiance and the temperature.

The detection unit detects a branching optical element that branches the thermal radiation of the measurement object into two optical paths, and detects the branched thermal radiation at one of the two wavelengths. A detection element, a second detection element that detects the branched thermal radiation light at the other wavelength of the two types of wavelengths, and is provided between the branch optical element and the first detection element, One of the two types of wavelengths is provided between the first optical filter that transmits the heat radiation light of one of the two types of wavelengths, and the branch optical element and the second detection element. A second optical filter that transmits the heat radiation light having the wavelength of.

As the two types of wavelengths, two types of wavelength bands having a predetermined width including wavelengths at which the spectral absorption coefficients of the absorber are the same are selected, and the two types of wavelength bands are spectral absorption coefficients of the absorber. The apparent spectral absorption coefficients calculated by weighted averaging with the spectral radiance of the measurement target temperature may be selected to be equal to each other.

The two-color radiation thermometer calculates a black body radiance at any of the two types of wavelengths calculated using the temperature of the measurement object, the radiance of the measured thermal radiation, and the absorber. The spectral absorption coefficient at the two types of wavelengths, the reflectance of the thermal radiation light at the interface of the absorber on the side of the measurement target, the reflectance of the thermal radiation light at the interface of the absorber, and the measurement The thickness of the absorber may be further calculated using the setting conditions in the section.

The absorber may be at least one of water, oil and fat, solution, glass and resin.

It is preferable that the measurement result of the temperature of the measurement object is output in association with the position of the center of gravity of the region occupied by the measurement object in the measurement visual field of the two-color radiation thermometer.

The near infrared band may be 940 nm to 1350 nm.

As described above, according to the present invention, it is possible to more accurately measure the temperature of the measurement target while suppressing the temperature measurement error at the end portion of the object.

FIG. 5 is a graph showing the relationship between wavelength and spectral radiance. FIG. 6 is a graph showing the relationship between temperature and dichroic ratio. FIG. 6 is a graph showing the relationship between temperature and dichroic ratio. FIG. 6 is a graph showing the relationship between temperature and dichroic ratio. FIG. 6 is a graph showing the relationship between temperature and the attenuation rate of spectral radiance. FIG. 6 is a graph showing the relationship between temperature and the attenuation rate of spectral radiance. It is explanatory drawing for demonstrating the influence of the water in a monochromatic radiation thermometer. It is explanatory drawing which showed the wavelength dependence of the spectral absorption coefficient of water. It is explanatory drawing for demonstrating the influence of the water in a monochromatic thermometer. It is explanatory drawing which showed the relationship between blackbody radiance, wavelength, and temperature. It is explanatory drawing for demonstrating the change of the dichroic ratio by a water film. It is explanatory drawing which showed the spectral absorption coefficient of water which is an example of an absorber. It is explanatory drawing for demonstrating the combination of the wavelength of the two-color radiation thermometer which is not influenced by water. It is explanatory drawing for demonstrating the combination of the wavelength of the two-color radiation thermometer which is not influenced by water. It is explanatory drawing for demonstrating the combination of the wavelength of the two-color radiation thermometer which is not influenced by water. It is explanatory drawing for demonstrating the weighting coefficient according to the spectral absorption coefficient and spectral radiance of water. It is explanatory drawing for demonstrating the weighting coefficient according to the spectral absorption coefficient and spectral radiance of water. It is explanatory drawing which showed the wavelength dependence of the spectral radiance of a high temperature object. It is explanatory drawing which showed the mode of the change of the dichroic ratio by the spectral absorption coefficient of water. It is explanatory drawing for demonstrating the calculation method of the thickness of a water film. It is a graph which showed the relationship between the thickness of a water film, and spectral transmittance. It is explanatory drawing which showed typically an example of a structure of the temperature measuring device which concerns on the same embodiment. It is explanatory drawing which showed typically an example of a structure of the temperature measuring device which concerns on the same embodiment. It is explanatory drawing which showed typically an example of a structure of the measuring part with which the temperature measuring device which concerns on the same embodiment is equipped. It is explanatory drawing which showed typically an example of a structure of the measuring part with which the temperature measuring device which concerns on the same embodiment is equipped. It is a graph which showed an example of the relationship between the center wavelength of an optical filter, and a temperature measurement error. It is explanatory drawing which showed typically an example of a structure of the detection part in the measurement part which concerns on the same embodiment. It is explanatory drawing which showed typically an example of a structure of the detection part in the measurement part which concerns on the same embodiment. It is explanatory drawing which showed typically an example of a structure of the detection part in the measurement part which concerns on the same embodiment. It is a block diagram showing an example of composition of an arithmetic processing unit with which a temperature measuring device concerning the embodiment is provided. It is a block diagram showing another example of composition of an arithmetic processing unit with which a temperature measuring device concerning the embodiment is provided. It is a block diagram showing an example of hardware constitutions of a temperature measuring device concerning the embodiment. It is explanatory drawing for demonstrating the temperature measuring method which concerns on the same embodiment. It is explanatory drawing for demonstrating the temperature measuring method which concerns on the same embodiment. It is explanatory drawing for demonstrating the temperature measuring method which concerns on the same embodiment. It is explanatory drawing for demonstrating the temperature measuring method which concerns on the same embodiment. It is explanatory drawing for demonstrating the temperature measuring method which concerns on the same embodiment. It is explanatory drawing for demonstrating the calculation method of a gravity center position. It is explanatory drawing which showed the temperature measuring method in an Example. It is a graph which showed the temperature measurement result in an Example. It is a graph which showed the temperature measurement result in an Example.

Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the accompanying drawings. In the present specification and the drawings, components having substantially the same functional configuration are designated by the same reference numerals, and duplicate description will be omitted.

(Study by the inventors regarding the radiation thermometer)
<The principle of radiation thermometry and the purpose of the present invention>
Prior to describing the temperature measuring method according to the embodiment of the present invention, the principle of the radiation temperature measuring method of interest in the present invention will be briefly described, and the purpose of the present invention will be described.

As described above, the radiation thermometry is a method of detecting the thermal radiation light emitted by an object according to the temperature and knowing the temperature of the object. The spectral radiance L of a black body, which is an ideal radiator, is expressed by the following equation (1) as a function of temperature and wavelength according to Planck's black body radiation law.

In the above formula (1),
T: Temperature [K]
λ: wavelength [nm]
c ₁ : first constant of black body radiation, 1.19×10 ²⁰ [W·m ⁻² ·nm ⁴ ].
c ₂ : second constant of blackbody radiation, 1.44×10 ⁷ [nm·K]
Is.

Here, if λT is sufficiently smaller than c ₂ such as when the radiator is a red hot steel material or when observing thermal radiation of a short wavelength, the above formula (1) becomes the formula (2) shown below. ) Can be approximated as

The spectral radiance of an actual object is smaller than the spectral radiance of a black body as described above, and the spectral radiance L of an actual object is expressed by the following equation (3) using the spectral emissivity peculiar to a substance. It

Here, in the above formula (3), ε(λ) is the spectral emissivity at the observation wavelength λ [nm], and other character formulas are the same as the above formulas (1) and (2). ..

In the radiation thermometry, since the observation wavelength λ is determined by the detector, the spectral radiance L is a function of the temperature T and the emissivity ε. The relationship between the observed wavelength λ and the spectral radiance L when the temperature T is changed to several temperatures is shown in FIG.

Therefore, the radiant temperature measurement method using a general monochromatic radiation thermometer (also called monochromatic radiation temperature measurement method) is to grasp the spectral emissivity in advance and then measure the spectral radiance of the thermal radiation from the measurement object. Is measured at one observation wavelength to obtain the temperature. In other words, in the general monochromatic radiation thermometry, accurate temperature measurement cannot be performed when the spectral emissivity of the measurement object is unknown. Further, even when the observation light is attenuated due to the presence of the absorber on the optical path from the object to be measured to the radiation thermometer, a temperature measurement error occurs unless the amount of attenuation by the absorber can be quantitatively specified.

On the other hand, in the radiation temperature measurement method, there is a temperature measurement method using a two-color thermometer in addition to the single color radiation temperature measurement method using a single color radiation thermometer. A two-color radiation thermometer (hereinafter, also simply referred to as a two-color thermometer) is a measuring instrument for observing thermal radiation light at two different observation wavelengths. As is apparent from the above formula (3), when the spectral emissivity is the same at the _two wavelengths λ ₁ and λ ₂ , the ratio of the spectral radiance L at the two wavelengths (that is, dichroic ratio) is temperature. Therefore, the temperature can be measured without knowing the spectral emissivity of the object to be measured in advance (the radiation temperature measurement method using a two-color thermometer will be described in detail below). When wavelengths that are close enough to be considered to have the same spectral emissivity (for example, wavelengths λ ₁ =1 μm and λ ₂ =1.2 μm in FIG. 1) are selected, as shown in FIG. Is a function of the temperature T. Such a two-color radiation thermometer is not affected by the obstruction of the field of view of the detector and the dimming due to obstacles on the optical path (for example, floating dust or mist, dirt on the observation window). There is a feature.

On the other hand, as mentioned earlier, in the general monochromatic radiation thermometry, the field of view is lost and the temperature measurement error occurs at the end (corner) of the object. Such a temperature measurement error occurs because the temperature is derived based on the energy intensity in the measurement field of view. Therefore, by using the two-color radiation thermometer having the above-mentioned characteristics, it is possible to measure It is possible to more accurately measure the temperature of the measuring object while suppressing the temperature measurement error.

<About the findings obtained by the present inventors>
Next, after briefly explaining the principle of the two-color radiation thermometer, the knowledge obtained by the present inventors will be described in detail with reference to FIGS. 3 to 17. 3 to 17 are explanatory diagrams for explaining the findings obtained by the present inventors.

[Principle of two-color radiation thermometer]
The two-color radiation thermometer uses the ratio of the spectral radiances L(λ ₁ , T) and L(λ ₂ , T) of two wavelengths λ ₁ , λ ₂ to specify the temperature T of the measurement target. It is a measuring device. The two spectral radiances observed using the above equation (3) are represented by the following equations (4) and (5).

Here, assuming that the spectral emissivities are equal to each other at _two wavelengths λ ₁ and λ ₂ (ε(λ ₁ )=ε(λ ₂ )=ε), the above formula (4) is divided by the formula (5). The dichroic ratio R, which is defined as a ratio, is expressed by the following equation (6).

Here, in the above formula (6), R _λ and Λ are as in the following formulas (6a) and (6b).

The above equation (6) shows that the dichroic ratio R is a function of the temperature T.
Now, it is considered to measure the temperature of a certain measurement object using a two-color thermometer. At this time, when setting the _two wavelengths λ ₁ and λ ₂ used for temperature measurement, two wavelengths close to each other (for example, wavelengths 1200 nm and 1250 nm) are selected, and two wavelengths separated to some extent (for example, 1200 nm, Attention will be paid to how the dichroic ratio R changes when (1300 nm) is selected. The state of such a change can be obtained by substituting the two types of wavelengths λ ₁ and λ ₂ into the equations (6) to 6(b).

The state of the obtained changes is shown in FIG. In FIG. 3, the horizontal axis represents the temperature T [° C.], and the vertical axis represents the dichroic ratio R calculated based on the equation (6).
As is clear from FIG. 3, the dichroic ratio R monotonically increases with the temperature T. Further, it can be seen that the closer the two selected wavelengths are to each other, the more gentle the change of the dichroic ratio R is. The gentle change in the dichroic ratio R (in other words, the temperature gradient of the dichroic ratio) means that the change amount of the dichroic ratio R is small even if the temperature T changes greatly. ing. In other words, when the two selected wavelengths are close to each other, even if the temperature changes, the change amount of the dichroic ratio is small, so that the temperature measurement sensitivity decreases.

From such a fact, when the temperature is measured using the two-color thermometer, it is preferable that the temperature corresponding to the difference between the two wavelengths to be selected is equal to or higher than the temperature resolution of the two-color thermometer. It can be seen that it is more preferable that the desired temperature range has a significant slope in the correspondence relationship between the dichroic ratio R and the temperature as shown in FIG. The wavelength difference corresponding to such temperature resolution varies depending on the dichroic thermometer used, but for example, the absolute value |λ ₁ −λ ₂ | of the difference between the two selected wavelengths is 100 nm or more. It is preferable.

[About the findings obtained by the present inventors]
The principle of the two-color thermometer focused on in the embodiment of the present invention has been briefly described above.
Now, in the above formula (3), the spectral radiance L in the monochromatic thermometer (measurement wavelength λ=1.55 μm) and the two-color thermometer (measurement wavelengths λ ₁ =0.90 μm, λ ₂ =1.55 μm) The temperature of the corner portion of the red hot steel plate was calculated and estimated. At this time, the temperature of the object to be measured was set to 800° C., and the lower limit temperature of the thermometer (determined by the minimum radiance at which the light detection amount operates correctly) was set to 600° C. Further, the separation distance between the thermometer and the measurement object was 3000 mm, the measurement visual field was a circular spot with a diameter of 36 mm, and the ratio of the measurement area other than the measurement object was derived as the attenuation rate.

First, FIG. 4 shows the derived relationship between the two-color ratio (λ ₁ /λ ₂ ) and the temperature in the two-color radiation thermometer. Further, using the results shown in FIG. 4, it will be considered to measure the temperature of the corner portion of the red hot steel material in each of the monochromatic thermometer and the bicolor thermometer. When the corner portion comes into the measurement field of view of the thermometer, the field of view is lost. As a result, the radiated light observed is attenuated even at the same temperature, and the temperature measurement result is as shown in FIG. 5A. That is, when trying to measure the corner portion of the red-hot steel material, when the temperature of the corner portion is 800° C., the attenuation rate is 85% (only 7.5 mm from the end of the steel material to the center portion of the steel material) when the temperature of the corner portion is 800° C. When measuring the range up to the facing position), the temperature is 680°C. This result means that the measurement error is 120° C. when the attenuation rate is 85%. On the other hand, in the two-color thermometer, as shown in FIG. 5A, the temperature measurement result is 800° C., which shows that the correct temperature can be measured. This result shows that even if 85% of the area in the measurement field of view is something other than the object to be measured, it can be accurately measured by detecting the radiance corresponding to 600° C. or higher. ing.

Further, as shown in FIG. 5B, when the same calculation as above is performed with the temperature of the corner portion set to 900° C., the radiance becomes high, so that the attenuation rate is 93% (4. It is understood that the temperature can be accurately measured up to the case where the range up to the position toward the central portion of the steel material is measured by 4 mm).

This result shows that the higher the temperature of the object to be measured, the more accurately the temperature of the corner can be measured using the two-color thermometer. Various photodetectors provided in a radiation thermometer have a minimum value (hereinafter, also simply referred to as "minimum radiant light amount") in the amount of radiant light (luminance) that can be detected. The dichroic thermometer outputs an accurate temperature by detecting the emitted light of the minimum emitted light amount or more by each detector set to two wavelengths, and the detected emitted light amount is less than the minimum emitted light amount. Therefore, a measurement error will occur. The higher the temperature of the object to be measured, the larger the absolute amount of heat radiation, and as a result, it is possible to measure the temperature of the corner portion farther. Further, in the two-color thermometer, if the amount of emitted light detected in the measurement visual field is equal to or more than the minimum amount of emitted light, the temperature of the measuring object can be accurately measured. The above is the first finding obtained by the present inventors.

Next, as illustrated in FIG. 6, a steel plate in a high temperature state (temperature T, emissivity ε) is taken as an example of the measurement object, and water, which is an example of an absorber, is a water film on the steel plate. As a result, further knowledge obtained by the present inventors will be described in detail.

For example, in the continuous casting process and hot rolling process of the steel manufacturing process, the temperature of the red-hot steel material moving on the transfer line is frequently measured. However, the cooling water may remain on the steel material or the evaporated cooling water may be trapped as steam at the place where the slab is pulled out from the continuous casting machine or between the rolling stands in the hot rolling process. Regarding the scattering of light due to steam on the optical path, a two-color thermometer can be applied because thermal radiation shows almost the same attenuation even if the two wavelengths to be observed are not widely separated from each other. On the other hand, when the accumulated water forms a water film on the steel material, the spectral absorptivity of water shows a strong wavelength dependence in the near-infrared region suitable for radiation temperature measurement. Will function as an absorber. As a result, the assumption that attenuation of thermal radiation occurs similarly at the two wavelengths does not hold and the dichroic radiation thermometer cannot be used properly. Water is transparent in the visible light band with a wavelength of about 800 nm or less, but in the short wavelength band such as the visible light band, thermal radiation is not emitted unless the temperature of the measurement target becomes high, so the temperature range of the measurement target is high. Will be limited to.

Further, in the steel manufacturing process as described above, in addition to water, glass, a solution present on the steel plate, fats and resins present on the steel plate, etc., have a uniform spectral absorptance in the near infrared band. Without (that is, showing strong wavelength dependence), it functions as an absorber.

The situation where the absorber exists in the optical path between the measurement object of the radiation thermometer and the radiation thermometer is a situation that can occur not only in the steel manufacturing process as described above but also in various other measurement environments. ..

The present inventors have solved such a problem, and even when detecting thermal radiation light in a state where an absorber is present on the optical path from the measurement object to the radiation thermometer, the temperature of the measurement object As a result of earnestly studying to realize a two-color radiation thermometer capable of accurately measuring the temperature, the following findings can be obtained.

Further, in the steel manufacturing process as described above, water is sprayed on the high-temperature steel material to cool the high-temperature steel material, but the amount of water present on the surface of the steel material is the amount of heat removed from the steel material. It is considered to be an important operating factor that influences. The present inventors can obtain a more accurate temperature of an object to be measured by using the temperature measuring device and the temperature measuring method according to the embodiment of the present invention as described below, and thus the object to be measured can be obtained. It has been conceived that the thickness of water (that is, absorber) existing on the optical path from the object to the radiation thermometer can be calculated more accurately.

Water, which is an example of an absorber, is transparent up to near the long wavelength end of the visible light band (near wavelength 800 nm), but at wavelengths of 800 nm and above belonging to the near infrared band, strong wavelengths such as shown in FIG. It becomes a semi-transparent material having dependence. Further, as is clear from Lambert-Beer's law, the thicker the water film, the more the amount of light in the near-infrared band absorbed by water increases, and thus the spectral transmittance becomes a small value.

In order to avoid the influence of water in the radiation thermometry, a method of measuring the temperature in a wavelength band of 800 nm or less where almost no light absorption of water exists may be considered. Thermometers (single wavelength radiation thermometers)" are commercially available. However, thermal radiation has a characteristic that it rapidly decreases toward the shorter wavelength side, and the temperature of an object to be measured needs to be at least 650° C. or higher in a radiation thermometer with an observation wavelength of 800 nm.

Further, as described above, if steam, which is a scatterer, is present, it is difficult to perform accurate temperature measurement by monochromatic radiation thermometry even if the water is transparent. Here, a specific example in which the measurement becomes inaccurate when a single-wavelength radiation temperature measurement is performed in a wavelength range of 800 nm or more where water absorbs light will be shown. For example, at a wavelength of 1300 nm, the light intensity is attenuated according to the water thickness and the spectral transmittance shown in FIG. 7. The calculation of the effect of such attenuation on the temperature measurement value is as shown in FIG. In FIG. 8, the horizontal axis represents the thickness of the water film [mm], and the vertical axis represents the temperature measurement error [° C.]. As is clear from FIG. 8, even if the thickness of water is only about 2 mm, a temperature measurement error of about 30° C. will occur. Therefore, in an actual measurement environment in which the water thickness is unknown, it becomes extremely difficult to perform accurate temperature measurement when using a monochromatic radiation thermometer.

Subsequently, in the radiation thermometer having an observation wavelength of 800 nm, the reason why the temperature of the object to be measured needs to be at least 650° C. or more is an explanatory diagram showing the relationship between the blackbody radiance and the wavelength and temperature. This will be described with reference to FIG.

In FIG. 9, the horizontal axis represents temperature and the vertical axis represents black body spectral radiance. As shown in FIG. 9, the blackbody spectral radiance increases monotonically with increasing temperature. Here, the detection limit of a sensor used in a general radiation thermometer is thermal radiation with a magnitude of black body spectral radiance of about 1. Therefore, focusing on the curve of the observation wavelength 800 nm in FIG. 9, the intersection of the straight line represented by “black body spectral radiance=1” and the curve of the observation wavelength 800 nm is about 650° C.

As described above, when using a dichroic radiation thermometer, it is preferable to separate the two wavelengths by at least 100 nm or more. Therefore, in order to realize a two-color radiation thermometer in a wavelength band in which water is transparent, it is preferable that the short wavelength side of the observation wavelength is near 800 nm-100 nm=700 nm. In such a case, as shown in FIG. 9, the measurement lower limit temperature of the two-color radiation thermometer becomes about 740° C. Further, as shown in FIG. 9, if the observation wavelength is set to, for example, 1000 nm, temperature measurement from 500° C. is possible, and if the observation wavelength is set to, for example, 1200 nm, the lower limit measurement temperature is expanded to around 400° C. Is possible.

Therefore, from the above knowledge, it is understood that the observation wavelength should be set to the longer wavelength side in order to secure a wide measurement temperature range. However, when a two-color radiation thermometer is constructed by using two kinds of wavelengths having an observation wavelength of 800 nm or more, as is clear from FIG. 7, such a wavelength band has a wavelength dependence in which the spectral absorption rate of water is remarkable. It becomes the band shown. The two types of spectral radiance L observed in such a wavelength band are represented by the following formulas (7) and (8) when the absorption of water as an absorber is taken into consideration.

Here, in the above formulas (7) and (8), τ ₁ is the spectral transmittance of water at the wavelength λ ₁ , and τ ₂ is the spectral transmittance of water at the wavelength λ ₂ . Further, the spectral transmittance τ of water is a function of the spectral absorption coefficient of water, the thickness of water, and the interface reflectance determined from the refractive index of both at the interface between water and air (details will be described below). ..). At this time, if the interface reflection is omitted, the spectral transmittances τ ₁ and τ ₂ of water can be expressed as τ ₁ =exp(−α ₁ ×t) and τ ₂ =exp(−α ₂ ×t), respectively. it can. Here, α ₁ is the spectral absorption coefficient of water at the wavelength λ ₁ , α ₂ is the spectral absorption coefficient of water at the wavelength λ ₂ , and t is the thickness of the water film.

In the above formulas (7) and (8), the two wavelengths λ ₁ and λ ₂ have different attenuation amounts due to absorption due to the wavelength dependence of the spectral absorption coefficient of water as shown in FIG. 7. In that case, in the relational expression between the dichroic ratio and the temperature defined by the equation (6), τ ₁ and τ ₂ which are terms due to water absorption do not cancel out.

For example, in a two-color thermometer focusing on wavelengths of 1000 nm and 1100 nm, the dichroic ratio changes as shown in FIG. 10 between the case where there is no water and the case where thermal radiation is observed through water. It will be. For example, assuming that the true temperature of the measurement object is 700° C., as apparent from FIG. 10, the apparent temperature is about 640° C. when the water film having a thickness of 5 mm is present, and the water film having a thickness of 10 mm is When present, the apparent temperature is about 590°C. In the actual temperature measurement in which the thickness of the water film changes irregularly, the presence of water as the absorber causes a large temperature measurement error.

As a result of further studies based on the above findings, the inventors of the present invention accurately measure the temperature of an object to be measured with a two-color radiation thermometer even when an absorber is present on the optical path. In order to do so, if the terms τ ₁ and τ ₂ which are the terms due to the absorption by the absorber in the above formulas (7) and (8) are canceled out when the dichroic ratio R is calculated, I thought about good things. In order to cancel out the term caused by the absorption by the absorber, it is only necessary to select two observation wavelengths having the same spectral absorptance of the absorber and measure the temperature of the measurement target.

FIG. 11 is a graph showing the wavelength dependence of the spectral absorption coefficient of water, which is an example of an absorber. The horizontal axis of FIG. 11 is the wavelength, and the vertical axis is the spectral absorption coefficient. As a result of examining FIG. 11 based on the above findings, the present inventors have come to the idea that the observation wavelength of the two-color radiation thermometer should be selected based on the technical idea described below.

○About selection method of observation wavelength-Part 1
In order to specify two wavelengths whose spectral absorption coefficients are equal to each other, the spectrum of the spectral absorption coefficient as shown in FIG. 11 is focused on, and a straight line represented by (spectral absorption coefficient=arbitrary constant) (in other words, In the spectrum as shown in FIG. 11, it suffices to pay attention to the number of intersections between the straight line parallel to the horizontal axis) and the curve corresponding to the spectrum of the spectral absorption coefficient. At this time, two wavelengths having spectral absorption coefficients equal to each other may be appropriately selected from a wavelength band in which the number of intersections of the curve and the straight line is 2 or more.

For example, in the case of water shown in FIG. 12A, there are the following two wavelength bands in which the number of intersections is 2 or more.
(1) From the other intersection point (a line represented by a spectral absorption coefficient ≈0.02) of the line in contact with the saddle part of the spectrum in the wavelength range of 1070 to 1080 nm, contact the peak in the wavelength range of 970 to 980 nm. Wavelength band up to the other intersection (a wavelength of about 1130) of a straight line (a line represented by a spectral absorption coefficient ≈0.05): First wavelength selection region (2) A straight line (spectral spectrum) in contact with the saddle part of the spectrum near the wavelength of 1260 nm From the other crossing point of the absorption coefficient ≈0.11) (around the wavelength of 1155 nm) to the other line of the line tangent to the peak near the wavelength of 1190 nm (a straight line indicated by the spectral absorption coefficient ≈0.13) Wavelength band up to intersection (wavelength near 1300 nm): second wavelength selection region

Two wavelengths having the same spectral absorption coefficient may be selected using these two types of wavelength selection regions as a guide. At this time, as described above, it is possible to select two wavelengths having a wavelength difference of, for example, about 100 nm so that the temperature corresponding to the difference between the two wavelengths is equal to or higher than the temperature resolution of the dichroic radiation thermometer. preferable.

Based on the above technical idea, for example, in FIG. 12B, two wavelengths of 1000 nm and 1130 nm can be selected from the first wavelength selection region. Further, for example, in FIG. 12C, two wavelengths of 1190 nm and 1300 nm can be selected from the second wavelength selection band. The combination of the wavelengths is just an example, and the wavelength may be appropriately selected from the two types of wavelength selection regions based on the above technical idea.

Such a dichroic radiation thermometer using a specific spectrum (a specific wavelength in a narrow band in which the wavelength bandwidth is negligible) uses a narrow band optical interference filter, and uses such a narrow band optical interference filter. It can be realized by installing it in a color radiation thermometer. Such a narrow band optical interference filter is available as a commercial product as long as it has a half width of about 10 nm, and it is also possible to manufacture a narrow band optical interference filter by using a known technique. is there. The wavelength selection filter will be described below again.

○About the selection method of observation wavelength-Part 2
In general, a radiation thermometer rarely observes a narrow band spectral radiance that can be regarded as a specific single wavelength as described above. This is because when the observation wavelength band is narrow, the absolute amount of light detected by the radiation thermometer becomes small, the detection sensitivity decreases, and the measurement lower limit temperature increases. When measuring thermal radiation with a finite wavelength bandwidth rather than a narrow band using a general wavelength selection filter, etc., the above two observation wavelengths can be selected as follows. it can.

That is, when the bandwidth of the wavelength to be observed cannot be ignored as in the above case 1, the simple average value of the absorption coefficient of the observation band is not used as the effective spectral absorption coefficient, but the wavelength corresponding to the temperature of the measurement target is used. The spectral absorption coefficient weighted by the spectral radiance having dependence and averaged may be obtained and used for the processing. That is, such a method has a finite bandwidth so that the “apparent spectral absorption coefficients” calculated by weighted averaging the spectral absorption coefficient of the absorber with the spectral radiance of the temperature to be measured are equal to each other. This is a method of selecting a band. Hereinafter, the selection method will be specifically described with reference to FIGS. 13A and 13B.

As a specific example, consider a case where two wavelengths having a bandwidth of 40 nm are selected starting from the first wavelength selection region shown in FIG. 12B.
First, the observation wavelength on the short wavelength side of the first wavelength selection region is fixed to a wavelength of 980 nm to a wavelength of 1020 nm with a bandwidth of 40 nm. Strictly speaking, in the wavelength range of 980 nm to 1020 nm, the effective spectral absorption coefficient α _eff is Planck's black body radiation considering the spectral absorption coefficient α(λ) at the wavelength λ and the wavelength dependence of the spectral radiance. Using the weighting factor w(λ) determined from the equation, the following equation (9) is used.

Here, assuming that the temperature of the measurement target is 900° C., the weighting coefficient w(λ) that normalizes the wavelength dependence of the spectral radiance L is calculated. The obtained weighting factor w(λ) is shown by a chain line in FIG. 13A. In the example shown in FIG. 13A, the average value of the spectral absorption coefficient weighted by the weighting coefficient is 4.2×10 ⁻² [1/mm]. On the other hand, if the spectral absorption coefficients are averaged (simple averaging) with a uniform weight without considering the wavelength dependence of the spectral radiance L, it becomes 4.3×10 ⁻² [1/mm]. became.

Next, for the observation wavelength on the long wavelength side of the first wavelength selection region, the spectral absorption coefficient averaged by weighting the spectral radiance of 900° C. as described above is the weighted spectral absorption coefficient on the short wavelength side. The wavelength band around 1130 nm is selected so as to be 4.2×10 ⁻² [1/mm], which is the same as As a result, as illustrated in FIG. 13B, the wavelengths of 1100 nm to 1140 nm meet such conditions. The simple average spectral absorption coefficient in the wavelength band shown in FIG. 13B was 4.1×10 ⁻² [1/mm].

As described above, the value of the apparent spectral absorption coefficient (effective absorption coefficient) depends on whether or not the wavelength dependence of the spectral radiance L of the measurement target is taken into consideration in the example shown in FIGS. 13A and 13B. It changes by 2×10 ⁻² [1/mm]. On the contrary, if the simple average of the spectral absorption coefficients of the observation band is used when estimating the apparent spectral absorption coefficient, the effective spectral absorption coefficient is 0. A mismatch of about 2×10 ⁻² [1/mm] will occur.

In the above description, the weighting coefficient based on the spectral radiance is calculated assuming that the measurement target is 900° C. However, as shown in FIG. 14, for example, the spectral radiance changes significantly when the temperature range is about 200° C. There is no. Therefore, if the approximate temperature of the measurement target can be predicted based on past operation data and the like, it becomes possible to give a weighting coefficient based on the spectral radiance.

Here, regarding the influence of the difference of the effective absorption coefficient of 0.2×10 ⁻² [1/mm] on the accuracy of the two-color radiation thermometer between the case where the spectral absorption coefficient is corrected by the weighting coefficient and the case where it is not executed. consider. For example, in a situation in which thermal radiation is measured through a water film having a thickness of 10 mm, the spectral absorption coefficients of water at two wavelengths are equal to each other, 4.2×10 ⁻² [1/mm], and the spectrum on the short wavelength side. The dichroic ratio in each case where the absorption coefficient is 4.3×10 ⁻² [1/mm] and the long-wavelength side spectral absorption coefficient is 4.1×10 ⁻² [1/mm]. R was calculated based on the above formula (6). The obtained results are shown in FIG. According to the results shown in FIG. 15, the dichroic ratio in the above two cases had a difference corresponding to a temperature difference of about 20° C. Therefore, when the observation wavelength has a range (when the observation wavelength is formed from a finite band), the spectral absorption coefficients of the absorbers averaged using weighting based on the spectral characteristics of the thermal radiation are accurate to each other. It is desirable to select two wavelength bands so that

As described above, according to the second observation wavelength selection method, when the radiation temperature measurement is performed using the observation wavelength having a finite bandwidth, the two-color radiation thermometer has the same light amount attenuation between the wavelengths. The spectral absorption coefficient is corrected so that it occurs. Since the measurement error can be further reduced by correcting the spectral absorption coefficient, even when the narrow band observation wavelength is selected based on the first observation wavelength selection method, It is more preferable to perform the correction processing of the spectral absorption coefficient described in the second observation wavelength selection method. At this time, as described above, it is preferable to determine the effective value α _eff of the spectral absorption coefficient in consideration of the wavelength dependence of the spectral radiance.

When estimating the effective absorption coefficient in the observation wavelength band, in addition to the spectral characteristics of the thermal radiation to be measured, the spectral transmission characteristics of the wavelength selection filter and the spectral sensitivity characteristics of the photodetector built into the radiation thermometer. The weighted average of the spectral data relating to the spectral absorption coefficient may be used as the weight. In this case, the term relating to the spectral transmission characteristic of the wavelength selection filter and the term relating to the spectral sensitivity characteristic of the photodetector incorporated in the radiation thermometer increase in the numerator part of the relational expression shown in the equation (9). It will be. By further weighting and averaging the spectral absorption coefficients by further utilizing the spectral transmission characteristics and spectral sensitivity characteristics, it becomes possible to perform a correction in a form that is closer to the actual one in consideration of the distribution of the spectral absorption coefficients, thus improving accuracy. It will be possible.

Further, in the second selection method of the observation wavelengths, the case where the bandwidths of the two observation wavelengths are the same as each other has been described, but the bandwidths of the two observation wavelengths may be different. For example, in the near infrared band, the spectral radiance increases as the wavelength becomes longer, so the observation band width on the long wavelength side may be made narrower than that on the short wavelength side.

Next, with reference to FIG. 16 and FIG. 17, the inventors have come up with the findings regarding the method of measuring the thickness of the water film located above the surface of the measurement target together with the temperature of the measurement target. explain.

If the situation shown in FIG. 6 is considered more strictly as a situation in which cooling water is flowing on the upper surface of a red-hot steel material as an example of the measurement object, such a situation is modeled as shown in FIG. can do.

If the temperature of the red-hot steel material is high, the water located on the upper surface of the steel material is in a film boiling state, and a water vapor layer as shown in FIG. 16 is formed between the steel material surface and the water film. The water film floats from the surface of the steel material. At this time, the radiation thermometer is supposed to look at the steel material to be measured from diagonally above the steel material in the vertical direction as shown in FIG. Inside the water film, light emitted from the steel material is absorbed according to the thickness t of the water film, and the radiance is attenuated. More specifically, when the angle formed by the optical axis of the radiation thermometer and the surface normal direction of the object to be measured is θ ₀ , inside the water film, the relation expressed by Snell's law (n _The light emitted from the steel material travels at an angle θ ₁ that satisfies _a ·sin θ ₀ =n _w ·sin θ ₁ ). Therefore, the radiance of the light emitted from the steel material is attenuated according to the optical path length (t/cos θ ₁ ). Further, interface reflections of reflectance ρ ₁ and ρ ₂ occur at the interface between the water film and the water vapor layer and at the interface between the water film and the atmosphere layer, respectively. Radiation light resulting from such absorption by the water film and interface reflection at the water film interface is measured by a radiation thermometer. Here, the water vapor as a gas has completely different optical characteristics from the liquid water, and the water vapor is almost transparent in the wavelength band of 940 nm to 1650 nm. That is, it can be considered that there is no absorption of radiated light in the water vapor layer shown in FIG.

The effective spectral transmittance τ ₁ in the above formula (7) is given by the following formula (10) by the interface reflection loss at the interface of the water film and the spectral absorption coefficient α _{1 at} the wavelength λ ₁ inside the water film. expressed.

Further, since the reflectances ρ ₁ and ρ _{2 at} the water film interface are ρ ₁ =ρ ₂ from the relationship of the refractive index in each layer as described above, the value of the reflectance is changed again to ρ=ρ ₁ =ρ _Set to ₂ . It is necessary to consider the reflectance ρ separately for the reflectance ρ _p of the _p- polarized component and the reflectance ρ _s of the s-polarized component, except for θ=0°. Therefore, the above equation (10) is transformed into the following equation (11). Here, in the following formula (11), the reflectances ρ _p and ρ _s are expressed as the following formulas (12) and (13) at the water film/atmosphere interface, for example.

Here, n _v is the refractive index of water vapor (n _v =1.00), n _w is the refractive index of water (n _w =1.33), and n _a is the refractive index of the atmosphere ( n _a =1.00). In the present technique, the spectral absorption coefficient alpha ₁ at the wavelength lambda _1, the spectral absorption coefficient alpha ₂ at the wavelength lambda _2, but the wavelength lambda ₁ to be equal to each _other, lambda ₂ is selected, The reflectance [rho _p , Ρ _s are constants determined only by the refractive index of each layer and the refraction angle, as in the above formulas (12) and (13). Therefore, even if the formula (8) is used instead of the formula (7), the value of the transmittance τ ₂ becomes equal to the value of the transmittance τ ₁ .

When the temperature T of the steel material to be measured is obtained based on the dichroic ratio shown in the equation (6), the transmittance τ _{1 at the} wavelength λ ₁ is obtained by transforming the equation (4) into the following equation. It is calculated as in (14). Here, in the following formula (14), the numerator is the radiance value observed by the radiothermometer, and the denominator corresponds to the radiance value radiated from the black body at the temperature T. Further, in the following formula (14), the spectral emissivity ε(λ ₁ ) of the steel material is a stable value of about 0.8 in the wavelength band of λ ₁ =1.1 μm to 1.3 μm.

Next, by substituting the above equation (10) into the above equation (7) and solving for the thickness t of the water film, the following equation (15) can be obtained.

Here, in the above formula (15), as the spectral absorption coefficient α ₁ of water, a value obtained in an experiment conducted in advance may be used. For example, when the combination of the wavelengths λ ₁ and λ ₂ is (1100 nm, 1130 nm), 0.0428 mm ⁻¹ may be used as the spectral absorption coefficient α ₁ of water. When the combination of wavelengths λ ₁ and λ ₂ is (1190 nm, 1300 nm), 0.129 mm ⁻¹ may be used as the spectral absorption coefficient α ₁ of water.

Therefore, when the temperature T of the steel material to be measured is obtained, the transmittance τ ₁ is calculated based on the above equation (14), and the obtained transmittance τ ₁ and the radiance obtained by the radiation thermometer are calculated. By using the measured value of, the refractive index of each medium as shown in FIG. 16, the spectral absorption coefficient α of water as described above, and the installation angle θ of the radiation thermometer, ), the thickness t of the water film can be calculated.

Here, regarding the above formula (15), how the thickness t of the water film changes with the decrease of the spectral transmittance τ is described for each of the angles θ ₀ =0°, 30°, and 45°. The calculated results are shown in FIG. 17 below. In the above formula (15), as the spectral absorption coefficient α ₁ of water, α ₁ =0.129 mm ⁻¹ which is the value at the wavelength λ ₁ =1.19 μm is used, and the refractive index is shown in FIG. Values were used. As is clear from FIG. 17, when the spectral transmittance τ decreases, the thickness of the water film increases. Further, according to the installation angle theta ₀ of the radiation thermometer, the optical path length of the water film of the emitted light is changed, also the relationship between the spectral transmittance and the water film thickness shown in FIG. 17, the installation angle theta ₀ It has changed slightly depending on.

As described above, even in the situation where the film boiling water covers the surface of the hot steel material which is glowing red, it is possible to obtain an accurate radiation temperature measurement method using the two-color radiation thermometer as shown in the above findings. If the temperature T can be obtained, the thickness of the water film can be accurately calculated. The above is the second finding obtained by the present inventors.

As a result of further studies based on such findings, the inventors of the present invention have come up with a more preferable temperature measuring device, which will be described below, that carries out the radiation temperature measurement processing based on the second knowledge. In the more preferable temperature measuring device described below, even if the spectral absorption coefficient of the absorber is measured in a band having wavelength dependence in order to lower the lower limit temperature of measurement, a two-color radiation thermometer is used. The radiation thermometry used makes it possible to accurately measure the temperature of the measuring object. Further, since the temperature of the measurement object is obtained more accurately, the thickness of the absorber such as the water film covering the surface of the measurement object can be calculated more accurately.

(Embodiment)
<About the structure of the temperature measuring device>
Next, with reference to FIGS. 18A and 18B, the overall configuration of the temperature measuring device 10, which is an example of a two-color radiation thermometer used in the temperature measuring method according to the embodiment of the present invention, will be described in detail. 18A and 18B are explanatory diagrams showing an example of the overall configuration of the temperature measuring device 10 according to the present embodiment.

The temperature measuring device 10 according to the present embodiment is a device that detects thermal radiation light in the near-infrared band emitted by the measurement object and measures the temperature of the measurement object based on the detection result of the radiance of the thermal radiation light. is there. Further, in a more preferable temperature measuring device 10, the thermal radiation light in the near-infrared band emitted by the measurement object is present in at least a part of the optical path, the absorber having wavelength dependence of the spectral absorption coefficient in the near-infrared band. It is a device for detecting the temperature of the measurement object based on the detection result of the radiance of the thermal radiation light while detecting the temperature of the measurement object. Here, as the absorber having wavelength dependence of the spectral absorption coefficient in the near infrared band, for example, at least one of water, oil and fat, solution, glass and resin can be mentioned.

Further, in the present embodiment, as the near-infrared band, the band of 800 nm to 1600 nm is focused, and particularly preferably, the band of 940 nm to 1350 nm is focused. The reason why the lower limit of the particularly preferable wavelength band is set to 940 nm is that water becomes a semitransparent material having a strong wavelength dependence in the wavelength range of 800 nm or more (particularly 940 nm or more) belonging to the near infrared band as shown in FIG. is there. The reason why the upper limit of the particularly preferable wavelength band is 1350 nm is that water becomes opaque at a water film thickness of 10 mm or more at 1350 nm or more as shown in FIG.

Such a temperature measuring device 10 mainly includes, for example, as shown in FIG. 18A, a measuring unit 101, a calculation processing unit 103, and a storage unit 105.

The measurement unit 101 measures the magnitude of the emitted thermal radiation (observation light) with respect to the measurement object that emits the thermal radiation that belongs to the near infrared band, such as a steel plate in a high temperature state. Further, in the particularly preferable temperature measuring device 10, the measuring unit 101 measures the heat radiation light of the measurement object at each of two types of wavelengths at which the spectral absorption coefficients of the absorber are the same, and these two types of wavelengths are measured. The measurement data showing the detection result of the radiance of the thermal radiation light in is generated.

These measuring units 101 correspond to, for example, an optical system including various lenses/lens groups in a two-color radiation thermometer, sensors such as photodetectors, and the like. A more detailed configuration of the measurement unit 101 will be described below again. Further, the two kinds of wavelengths measured by the measuring unit 101 of the particularly preferable temperature measuring device 10 are preset in accordance with the two kinds of “observation wavelength selection methods” as described above.

When the measurement unit 101 measures the size of the thermal radiation of the measurement object and generates the measurement data indicating the detection result of the radiance of the thermal radiation, the generated measurement data is sent to the arithmetic processing unit 103 described later. Output.

The arithmetic processing unit 103 is realized by a CPU (Central Processing Unit), a ROM (Read Only Memory), a RAM (Random Access Memory), a communication device, and the like. The arithmetic processing unit 103 controls the measurement process performed by the measuring unit 101 in a centralized manner. The arithmetic processing unit 103 also performs arithmetic processing for calculating the temperature of the measurement target based on the measurement data measured by the measuring unit 101. More specifically, the arithmetic processing unit 103 calculates the spectral radiance and the temperature derived from the measurement data corresponding to the two types of wavelengths generated by the measuring unit 101 and the Planck's black body radiation equation as described above. The temperature of the measuring object is calculated based on the relational expression between and. The information on the temperature of the measurement object calculated by the arithmetic processing unit 103 is output as an image via a display screen or the like, as a printed matter via a printer or the like, or as data itself.

The detailed configuration of the arithmetic processing unit 103 will be described in detail below.

The storage unit 105 is realized by, for example, a RAM, a storage device, or the like included in the temperature measuring device 10 according to this embodiment. The storage unit 105 stores various information such as the spectral absorption coefficient of the absorber of interest, the spectral radiance of the measurement target obtained by analyzing past operation data, and the weighting coefficient used to correct the spectral absorption coefficient. The parameters and data of are stored. In addition to these data, various parameters that need to be stored in the storage unit 105 when the temperature measuring device 10 according to the present embodiment performs some processing, the progress of processing, or the like, or Various databases and programs are recorded as appropriate. In the storage unit 105, the measurement unit 101, the arithmetic processing unit 103, and the like can freely perform data read/write processing.

The measurement unit 101, the arithmetic processing unit 103, and the storage unit 105 may be realized inside one measurement device as one function of a two-color radiation thermometer, as schematically shown in FIG. 18A. Further, the measurement unit 101, the arithmetic processing unit 103, and the storage unit 105 may be distributed and installed in a plurality of devices as illustrated in FIG. 18B, for example. In the example shown in FIG. 18B, the functions of the measurement unit 101 and the storage unit 105 are realized inside the measurement unit that functions as, for example, a two-color radiation thermometer, and calculations such as a personal computer, various servers, and various process computers are performed. The case where the functions of the arithmetic processing unit 103 and the storage unit 105 are realized in the processing device is illustrated. Note that in FIG. 18B, the storage unit 105 is realized as the storage units 105a and 105b in each of the measurement unit and the arithmetic processing device, but the storage unit 105 may be realized only inside the measurement unit, It may be realized only inside the arithmetic processing unit.

<About the configuration of the measurement unit 101>
Subsequently, a configuration example of the measurement unit 101 according to the present embodiment will be described in detail with reference to FIGS. 19 to 21. FIG. 19 is an explanatory diagram schematically showing an example of the configuration of the measuring unit included in the temperature measuring device according to the present embodiment. 20 to 21 are explanatory views schematically showing an example of the configuration of the position control mechanism in the measuring unit according to the present embodiment.

The measuring unit 101 according to the present embodiment corresponds to an optical system in a two-color radiation thermometer, operates under the control of the arithmetic processing unit 103, and heats the near-infrared band emitted by the measurement target. Measure the emitted light. As schematically shown in FIG. 19, the measuring unit 101 includes a light receiving unit 111 that receives the heat radiation light from the measurement object, and a detection unit 113 that detects the heat radiation light received by the light receiving unit 111. A position control mechanism 115 that changes the relative positional relationship between the measurement target and the light receiving unit 111 and causes the light receiving unit 111 to measure the distribution of thermal radiation light in the width direction of the measurement target.

In the measurement unit 101 according to this embodiment, the light receiving unit 111 and the detection unit 113 as described above may be optically connected by various known light transmission mechanisms. As such a light transmission mechanism, for example, various known optical fibers OF can be cited. By connecting the light receiving unit 111 and the detection unit 113 by an optical transmission mechanism such as an optical fiber OF, the light receiving unit 111 can be arranged separately from the detection unit 113, and according to the present embodiment. The convenience when using the temperature measuring device is further improved.

As shown in FIG. 19, the light receiving unit 111 connects the light receiving lens 121 that receives the heat radiation light from the measurement object and the heat radiation light from the measurement object that has passed through the light receiving lens 121 to the optical fiber OF. Connection coupler 123 for The light receiving lens 121 and the connection coupler 123 function as a light guiding optical system that guides the heat radiation light to the detection unit 113.

Here, the specific configuration of the light receiving unit 111 according to the present embodiment is not particularly limited. For example, in FIG. 19, one biconvex lens is illustrated as the light receiving lens 121, but the light receiving lens 121 may be a lens group including a plurality of optical elements. The lens used for the light receiving lens 121 is not particularly limited, and a known optical element such as a spherical lens or an aspherical lens can be appropriately used. The connecting coupler 123 and the optical fiber OF are not particularly limited, and various known connecting couplers and optical fibers can be used.

The heat radiation light from the measurement object is converted into a substantially parallel light flux by the light receiving lens 121 of the light receiving unit 111, and reaches the connection coupler 123. The connection coupler 123 connects the heat radiation light guided from the light receiving lens 121 to one end of the optical fiber OF. The heat radiation light from the measurement object, which is received by the light receiving unit 111 and then transmitted by the optical fiber OF, is guided to the detection unit 113.

As illustrated in FIG. 20, the detection unit 113 includes a connection coupler 151 optically connected to the optical fiber OF, a beam splitter 153, optical filters 155a and 155b, condenser lenses 157a and 157b, and a sensor. 159a and 159b.

The heat radiation light from the measurement object that has passed through the connection coupler 151 is guided to a beam splitter 153 which is an example of a branch optical element. The luminous flux of the heat radiation light that has reached the beam splitter 153 is split into two optical paths by the beam splitter 153.

As shown in FIG. 20, an optical filter 155a, which is an example of a first optical filter, is provided on one optical path after branching, and a second optical filter 155a is provided on the other optical path after branching. An optical filter 155b, which is an example of the above, is provided.

The optical filters 155a and 155b are filters that function as wavelength selection filters, select the wavelength of the heat radiation light, and transmit the heat radiation light having a specific wavelength to the sensors 159a and 159b in the subsequent stage. As the optical filters 155a and 155b, known ones can be used as long as they can transmit light of two preset wavelengths (observation wavelengths). Further, as described in the knowledge regarding the “selection method of observation wavelength”, the optical filters 155a and 155b may be narrow band wavelength selection filters, or may be a general band (a finite bandwidth (Having) wavelength selection filter.

The thermal radiation light having one of the two observation wavelengths that has passed through the optical filter 155a is condensed by the condenser lens 157a onto the sensor 159a which is an example of the first detection element. Further, the thermal radiation light having the other wavelength of the two observation wavelengths that has passed through the optical filter 155b is condensed by the condenser lens 157b onto the sensor 159b which is an example of the second detection element.

The sensors 159a and 159b detect the spectral radiance of the thermal radiation light from the measurement object guided by the condenser lenses 157a and 157b, respectively, and generate the data of the obtained luminance signal. After that, each of the sensors 159a and 159b outputs the obtained luminance signal to the arithmetic processing unit 103. The brightness signal corresponds to the measurement data indicating the detection result of the radiance of the thermal radiation light.

Here, the sensors 159a and 159b are not particularly limited, and known ones can be used as long as they are suitable for the above-mentioned two kinds of wavelengths for detecting the heat radiation light. Examples of such a sensor (photodetector) include a detection element using Si and a detection element using InGaAs.

Note that, in FIG. 20, the condenser lenses 157a and 157b are schematically illustrated by using one biconvex lens, but the condenser lenses 157a and 157b are a lens group including a plurality of lenses. May be. The lenses used for the condenser lenses 157a and 157b are not particularly limited, and known optical elements such as spherical lenses and aspherical lenses can be appropriately used.

Here, in the more preferable temperature measuring device 10 in the present embodiment, as one of the combinations of the two observation wavelengths (that is, the transmission wavelengths of the optical filters 155a and 155b), for example, the second wavelength selection shown in FIG. 12A is selected. It is assumed that 1190 nm is selected from the region. In this case, the other wavelength is selected from around 1300 nm. Here, as is clear from FIG. 12A, in this wavelength band, the spectral absorption coefficient of water increases as the wavelength becomes longer.

The spectral absorption coefficient at a wavelength selected from around 1300 nm is required to match the spectral absorption coefficient at a wavelength of 1190 nm. If they do not match, the principle described above does not hold, and a temperature measurement error occurs as the degree of matching decreases.

In the following, in the more preferable temperature measuring device 10, the manner in which a temperature measurement error occurs is confirmed by the following test.
That is, five kinds of wavelength selection filters having a half-value width of the transmission band of about 10 nm and a center wavelength of the transmission band of 1300.0 nm, 1301.8 nm, 1303.2 nm, 1304.2 nm, 1304.7 are prepared. Then, on the measurement object in the state of 900° C., the difference between the temperature indication values in the case where the water as the absorber is present and the case where the water is not present is investigated. The obtained results are shown in FIG.

As is clear from FIG. 21, it is understood that the temperature measurement value does not change regardless of the presence or absence of water in the case of the wavelength selection filter having the center wavelength of 1303.2 nm. This is because the spectral absorption coefficient of water (spectral transmittance when radiated light passes through water) exactly matches at the wavelength of 1190 nm and the wavelength of 1303.2 nm. That is, by selecting such a central wavelength, the temperature can be measured without being affected by water.

On the other hand, when the center wavelength of the transmission band of the wavelength selection filter deviates from 1303.2 nm by 1 nm to the long wavelength side, due to the mismatch of the spectral transmittance of water, the temperature of about 10°C is measured when the water film thickness is 2.5 mm. It is understood that an error occurs and a temperature measurement error of about 20° C. occurs when the water film has a thickness of 5 mm. As is clear from these results, the transmission wavelength band (center wavelength) of the wavelength selection filters used as the optical filters 155a and 155b should be selected according to the expected thickness of the water film, the accuracy required for the temperature measurement error, and the like. Is preferred. For example, if a water film having a maximum thickness of about 5 mm is expected, the transmission wavelength of the wavelength selection filter is preferably selected with an accuracy of about ±0.5 nm. Further, if it is desired to keep the temperature measurement error within the range of ±10° C., the width of the transmission wavelength band of the wavelength selection filter is preferably set to about 1.0 nm.

Returning to FIG. 19 again, the position control mechanism 115 according to the present embodiment will be described.
As described above, the position control mechanism 115 according to the present embodiment changes the relative positional relationship between the measurement target and the light receiving unit 111 to receive the distribution of thermal radiation light in the width direction of the measurement target. This is a mechanism for measuring by the unit 111. As a result, with the temperature measuring device 10 according to the present embodiment, it is possible to measure the temperature distribution in the width direction including the corner portion of the measurement object of interest.

Further, regarding the sensors 159a and 159b used for measurement, when the minimum emitted light amount which is the minimum emitted light amount required for temperature calculation in the measurement visual field is specified in advance, the position control mechanism 115 causes the sensor 159a, For 159b, it is preferable to change the relative positional relationship between the measurement object and the light receiving unit 111 until the amount of emitted light detected in the measurement visual field becomes less than the minimum amount of emitted light. As a result, in the temperature measuring device 10 according to the present embodiment, it becomes possible to more accurately measure the temperature distribution in the width direction including the corner portion of the measurement object of interest.

Hereinafter, the position control mechanism 115 according to the present embodiment will be described more specifically with reference to FIGS. 22A to 23.

The position control mechanism 115 according to the present embodiment may be a drive mechanism that moves the light receiving unit 111 along the width direction of the measurement target, as schematically shown in FIG. 22A, for example. In FIG. 22A, the direction perpendicular to the paper surface is the longitudinal direction of the measurement target, the surface normal direction of the measurement target is the thickness direction of the measurement target, and for both the longitudinal direction and the thickness direction. The direction orthogonal to each other is the width direction of the measurement target. At this time, the drive mechanism that functions as the position control mechanism 115 moves the light receiving unit 111 along the width direction of the measurement target object, so that the relative positional relationship between the light reception unit 111 and the measurement target object. Changes, it becomes possible to measure the temperature distribution in the width direction for the measurement object of interest.

Such a drive mechanism is not particularly limited, and various known drive mechanisms such as actuators can be appropriately used.

Further, the position control mechanism 115 according to the present embodiment may be an angle control mechanism that changes the angle formed by the surface normal direction of the measurement target and the optical axis of the light receiving unit 111. For example, in FIG. 22B, the direction perpendicular to the paper surface is the longitudinal direction of the measurement target, the surface normal direction of the measurement target is the thickness direction of the measurement target, and in both the longitudinal direction and the thickness direction. It is assumed that the direction orthogonal to the direction is the width direction of the measurement object. At this time, a rotation axis is provided in a direction parallel to the longitudinal direction, and the light receiving unit 111 rotates about the rotation axis within a range of −φ° to +φ°, whereby the light receiving unit 111 and the measurement target object. The relative positional relationship between and changes, and it becomes possible to measure the temperature distribution in the width direction of the measurement object of interest.

Here, the rotation angle φ corresponds to the angle formed by the optical axis of the light receiving unit 111 and the surface normal direction of the measurement target. Further, the size of the rotation angle φ is not particularly limited, and is appropriately set according to the width of the measurement target and the installation height of the light receiving unit 111 (height from the surface of the measurement target). do it. However, when the size |φ| of the rotation angle φ exceeds 45°, the energy of the thermal radiation light received by the light receiving unit 111 may be too small, and therefore the size |φ| , 0° or more and 45° or less. The rotation angle φ corresponds to the angle θ ₀ in the model shown in FIG.

As the angle adjusting mechanism shown in FIG. 22B, for example, various known swinging mechanisms using an actuator or the like may be applied, or an image pickup lens having a tilt mechanism, or an image pickup having a tilt mechanism and a shift mechanism. Various imaging lenses such as lenses may be used.

Further, as an angle control mechanism for changing the angle formed by the surface normal direction of the measuring object and the optical axis of the light receiving unit 111, for example, a mechanism using a rotating mirror as shown in FIG. 23 is used. It is also possible. In FIG. 23, the direction perpendicular to the paper surface is the width direction of the measurement target, the surface normal direction of the measurement target is the thickness direction of the measurement target, and for both the longitudinal direction and the thickness direction. The direction orthogonal to each other is the longitudinal direction of the measurement object. In the example shown in FIG. 23, between the light guide optical system (that is, the light receiving mirror 121 and the connection coupler 123) in the light receiving unit 111 and the measurement target, the direction oblique to the surface normal direction of the measurement target is oblique. Is provided with a mirror M, and the surface normal direction of the object to be measured and the optical axis connecting the light receiving lens 121 and the connection coupler 123 are set to be orthogonal to each other.

At this time, the mirror M is rotated by a predetermined angle with the optical axis connecting the light receiving lens 121 and the connection coupler 123 (in other words, the longitudinal direction of the measurement target) as a rotation axis, whereby the surface normal direction of the measurement target is measured. It is possible to change the angle formed by the optical axis of the light receiving unit 111. As a result, the relative positional relationship between the light receiving unit 111 and the measurement target changes, and the temperature distribution in the width direction can be measured for the measurement target of interest.

Also in the example shown in FIG. 23, the size of the rotation angle of the mirror M about the rotation axis is not particularly limited, and the width of the measurement target and the installation height of the light receiving unit 111 (measurement target). The height from the surface) may be set appropriately. However, if the size of the rotation angle exceeds 45°, the energy of the heat radiation light received by the light receiving unit 111 may be too small. Therefore, the size of the rotation angle is 0° or more and 45° or less. Preferably.

The angle adjusting mechanism as shown in FIG. 23 can be realized by using a known drive mechanism such as an actuator and various known mirrors.

Further, in the measuring unit 101 according to the present embodiment, the position control mechanism 115 is a combination of the drive mechanism shown in FIG. 22A and the angle adjustment mechanism shown in FIG. 22B or 23. May be.

Here, the moving speed in the width direction of the drive mechanism as shown in FIG. 22A and the rotation speed of the angle adjusting mechanism as shown in FIGS. 22B and 23 are not particularly limited. However, in the case where the measurement object is, for example, moving on a conveyance line, the movement speed is adjusted so as to be synchronized with the movement timing of the measurement object in consideration of the conveyance speed of the measurement object. The rotation speed is preferably determined, and the detection rates (measurement cycles) of the sensors 159a and 159b in the detection unit 113 are also preferably synchronized with the conveyance speed of the measurement target.

The configuration example of the measuring unit 101 according to the present embodiment has been briefly described above with reference to FIGS. 19 to 23.

<Regarding Configuration Example of Arithmetic Processing Unit 103>
Next, a configuration example of the arithmetic processing unit 103 according to the present embodiment will be described with reference to FIGS. 24 and 25. FIG. 24 is a block diagram showing a configuration example of the arithmetic processing unit 103 according to the present embodiment, and FIG. 25 shows a configuration example of the arithmetic processing unit 103 in a more preferable temperature measuring device 10 according to the present embodiment. FIG.

As illustrated in FIG. 24, the arithmetic processing unit 103 according to the present embodiment includes a measurement control unit 171, a data acquisition unit 173, a temperature calculation unit 175, a result output unit 177, and a display control unit 179. Prepare mainly.

The measurement control unit 171 is realized by, for example, a CPU, a ROM, a RAM, an input device, an output device, a communication device, and the like. The measurement control unit 171 is a processing unit that integrally controls the functions of the temperature measuring device 10 according to the present embodiment. Further, the measurement control unit 171 controls the operation of the measurement unit 101 so as to measure the heat radiation light from the measurement object at the two types of wavelengths as described above. Furthermore, the measurement control unit 171 outputs various set values such as the measurement conditions of the thermal radiation light including the arrangement conditions of the device to the temperature calculation unit 175 and the thickness calculation unit 177 as necessary. Is also possible.

The data acquisition unit 173 is realized by, for example, a CPU, a ROM, a RAM, a communication device, and the like. The data acquisition unit 173 acquires the brightness signals at the two types of wavelengths generated by the measurement unit 101, and outputs the brightness signals to the temperature calculation unit 175 described later. Further, the data acquisition unit 173 may associate the acquired brightness signals at the two types of wavelengths with time information regarding the date and time when the brightness signals were acquired, and store the history information in the storage unit 105.

The temperature calculation unit 175 is realized by, for example, a CPU, ROM, RAM and the like. The temperature calculation unit 175 utilizes the luminance signals at the two types of wavelengths output from the data acquisition unit 173, and divides one luminance signal by the other luminance signal to obtain a dichroic ratio (in other words, the spectral radiance Ratio). Further, the temperature calculation unit 175 calculates the temperature of the measurement target by using the calculated dichroic ratio and the relational expression between the dichroic ratio and the temperature.

Note that when the temperature calculation unit 175 calculates the dichroic ratio R, which luminance signal of the two types of wavelengths λ ₁ and λ ₂ is used as the denominator and which luminance signal is used as the numerator for calculation is particularly important. The present invention is not limited to this, and it suffices that the reference luminance signal is not changed during the arithmetic processing.

The temperature calculation unit 175 outputs the information regarding the temperature T of the measurement target calculated as described above to the result output unit 177 described later.

The result output unit 177 is realized by, for example, a CPU, a ROM, a RAM, an output device, a communication device, and the like. The result output unit 177 outputs the information about the temperature T of the measurement object output from the temperature calculation unit 175 to the user of the temperature measurement device 10. Specifically, the result output unit 177 associates the data corresponding to the temperature measurement result with the time data regarding the date and time when the data was generated, and outputs the data to various servers or control devices or outputs from a printer or the like. The device is used to output as a paper medium. Further, the result output unit 177 may output the data corresponding to the determination result to various information processing devices such as a computer provided outside or to various recording media.

In addition, when the result output unit 177 outputs data corresponding to the temperature measurement result to an output device such as a display provided in the temperature measuring device 10 or a display included in various externally provided devices, The determination result is output in cooperation with the display control unit 179 described later.

The display control unit 179 is realized by, for example, a CPU, ROM, RAM, output device, communication device, and the like. The display control unit 179 performs display control when displaying data corresponding to the temperature measurement result and the thickness calculation result on various display devices such as a display. As a result, the user of the temperature measuring device 10 can grasp the measurement result regarding the temperature of the measurement object and the calculation result regarding the thickness of the absorber on the spot.

Further, as shown in FIG. 25, the more preferable arithmetic processing unit 103 of the temperature measuring apparatus 10 in the present embodiment is a measurement control unit 171, a data acquisition unit 173, a display control unit 179, and a temperature calculation unit 181. A thickness calculation unit 183 and a result output unit 185 are mainly provided.

Here, the more preferable measurement control unit 171, data acquisition unit 173, and display control unit 179 in the temperature measuring device 10 have the same configuration as the arithmetic processing unit 103 shown in FIG. The detailed description is omitted below.

The temperature calculation unit 181 is realized by, for example, a CPU, ROM, RAM and the like. The temperature calculation unit 181 uses the luminance signals at the two types of wavelengths output from the data acquisition unit 173 to divide one luminance signal by the other luminance signal to obtain a dichroic ratio (in other words, the spectral radiance Ratio). Further, the temperature calculation unit 181 calculates the temperature of the measurement object by using the calculated dichroic ratio and the relational expression between the dichroic ratio and the temperature.

As is clear from the above equation (6), the dichroic ratio R can be calculated by dividing one of the luminance signals at the two wavelengths by the other luminance signal. On the other hand, in the more preferable temperature measuring device 10 in the present embodiment, since the absorption of the thermal radiation light by the absorber is taken into consideration as shown in the above formulas (7) and (8), the dichroic ratio R Is expressed by the following expression (16) when the expression is derived in the same manner as the expression (6) using the above expressions (7) and (8).

As is clear from the findings described above, the measurement unit 101 according to the present embodiment measures the spectral radiance at the wavelengths at which the absorbers have the same spectral absorption coefficient. Therefore, the terms relating to absorption by the absorber shown in the first term of the median side of the equation (16) cancel each other out in the numerator and denominator, and the value becomes 1. Therefore, R _λ and Λ on the right side of the equation (16) are the same as the equations (6a) and (6b).

Here, R _λ and Λ shown in the equations (6a) and (6b) are constants determined by the measurement conditions that can be acquired from the measurement unit 101. Therefore, the temperature calculation unit 181 can calculate the temperature T of the measurement target using the calculated dichroic ratio R and the relational expression (leftmost side=rightmost side) in the above equation (16). It will be possible.

Note that when the temperature calculation unit 181 calculates the dichroic ratio R, which luminance signal of the two types of wavelengths λ ₁ and λ ₂ is used as the denominator and which luminance signal is used as the numerator for calculation is particularly important. The present invention is not limited to this, and it suffices that the reference luminance signal is not changed during the arithmetic processing.

Further, the temperature calculation unit 181 may directly calculate the temperature by using the above equations (7) and (8) without using the dichroic ratio R represented by the above equation (16). That is, if the emissivity ε at two types of wavelengths λ ₁ and λ ₂ is known, the unknowns in the above formulas (7) and (8) are the temperature T and the thickness t of the water film. Therefore, the temperature calculation unit 175 can calculate the temperature T by simultaneously solving the above equations (7) and (8) to obtain the solution of the simultaneous equations. Further, even if the emissivity ε at the two kinds of wavelengths λ ₁ and λ ₂ is unknown, if the emissivity ε at the wavelength λ ₁ and the emissivity ε at the wavelength λ ₂ are equal to each other, similarly, It is possible to directly calculate the temperature T by using the simultaneous equations (7) and (8). Here, the solution method of the simultaneous equations is not particularly limited, and for example, when it can be solved analytically, it may be solved analytically, may be solved by numerical calculation, or may be solved as an optimum value problem. May be.

The temperature calculation unit 181 outputs the information regarding the temperature T of the measurement object calculated as described above to the thickness calculation unit 183 and the result output unit 185 described later.

The thickness calculator 183 is realized by, for example, a CPU, a ROM, a RAM, and the like. The thickness calculator 183 calculates the black body radiance at any of the two wavelengths calculated from the obtained temperature of the measurement object, the radiance of the measured thermal radiation, and the two wavelengths of the absorber. At the measuring object side of the absorber, the reflectance of the thermal radiation at the interface of the absorber on the side of the measuring object, the reflectance of the thermal radiation at the interface of the absorber on the side of measuring unit 101, and Using the setting conditions and, the thickness of the absorber is further calculated.

More specifically, the thickness calculator 183 measures the measured values of the luminance signal (spectral radiance) at the two types of wavelengths output from the data acquirer 173 and the temperature T of the measurement target calculated by the temperature calculator 181. Is used to calculate the transmittance τ based on the above equation (14). The thickness calculator 183 also obtains the transmittance τ, the reflectances ρ _p and ρ _s of the heat radiation light in the absorber, the spectral absorption coefficient α of the absorber, and the installation of the light receiver 111 in the measurement unit 101. The thickness t of the absorber is calculated based on the above equation (15) using the condition (specifically, the angle θ formed by the surface normal direction of the measurement target and the optical axis of the light receiving unit 111). To do.

The thickness calculation unit 183 outputs the information regarding the thickness t of the absorber calculated as described above to the result output unit 185 described later.

The result output unit 185 is realized by, for example, a CPU, a ROM, a RAM, an output device, a communication device, and the like. The result output unit 185 outputs the information about the temperature T of the measurement object output from the temperature calculation unit 181 and the information about the thickness t of the absorber output from the thickness calculation unit 183 to the user of the temperature measurement device 10. .. Specifically, the result output unit 185 outputs the data corresponding to the temperature measurement result and the thickness calculation result to various servers and control devices in association with the time data regarding the date and time when the data was generated. , Output as a paper medium using an output device such as a printer. Further, the result output unit 185 may output the data corresponding to the determination result to various information processing devices such as a computer provided outside, or may output the data to various recording media.

Further, the result output unit 185 outputs data corresponding to the temperature measurement result and the thickness calculation result to an output device such as a display provided in the temperature measuring device 10 or a display included in various externally provided devices. When outputting, the determination result is output in cooperation with the display control unit 179.

Heretofore, an example of the function of the arithmetic processing unit 103 according to the present embodiment has been shown. Each component described above may be configured by using a general-purpose member or circuit, or may be configured by hardware specialized for the function of each component. Further, the CPU or the like may perform all the functions of each component. Therefore, the configuration to be used can be appropriately changed according to the technical level at the time of implementing the present embodiment.

Note that it is possible to create a computer program for realizing each function of the arithmetic processing unit according to the present embodiment as described above, and install the computer program in a personal computer or the like. It is also possible to provide a computer-readable recording medium in which such a computer program is stored. The recording medium is, for example, a magnetic disk, an optical disk, a magneto-optical disk, a flash memory, or the like. Further, the above computer program may be distributed, for example, via a network without using a recording medium.

The configuration of the temperature measuring device 10 according to the present embodiment has been described above in detail with reference to FIGS. 18A to 25.

Depending on the size of the measurement target of interest in the width direction, there is a possibility that the temperature measurement cannot be performed for the entire width direction of the measurement target by using only one temperature measuring device 10. In that case, by installing a plurality of temperature measuring devices 10 according to the present embodiment along the width direction of the measurement object, it is possible to perform temperature measurement over the entire width direction of the measurement object. Becomes

<About hardware configuration>
Next, the hardware configuration of the temperature measuring device 10 according to the embodiment of the present invention will be described in detail with reference to FIG. FIG. 26 is a block diagram for explaining the hardware configuration of the temperature measuring device 10 according to the embodiment of the present invention.

The temperature measuring device 10 mainly includes a CPU 901, a ROM 903, and a RAM 905. The temperature measuring device 10 further includes a host bus 907, a bridge 909, an external bus 911, an interface 913, a measuring unit 101, an input device 915, an output device 917, a storage device 919, a drive 921, a connection port 923, and a communication device 925. Equipped with.

The CPU 901 functions as a central processing unit and a control unit, and according to various programs recorded in the ROM 903, the RAM 905, the storage device 919, or the removable recording medium 927, the whole operation of the temperature measuring device 10 or a part thereof is performed. Control. The ROM 903 stores programs used by the CPU 901, calculation parameters, and the like. The RAM 905 temporarily stores a program used by the CPU 901, parameters that change appropriately during execution of the program, and the like. These are connected to each other by a host bus 907 composed of an internal bus such as a CPU bus.

The host bus 907 is connected to an external bus 911 such as a PCI (Peripheral Component Interconnect/Interface) bus via a bridge 909.

As described above, the measuring unit 101 detects the thermal radiation light from the measurement target and measures the magnitude of the spectral radiance.

The input device 915 is an operation unit operated by a user, such as a mouse, a keyboard, a touch panel, a button, a switch, and a lever. Further, the input device 915 may be, for example, a remote control means (so-called remote control) using infrared rays or other radio waves, or an external connection device such as a mobile phone or a PDA corresponding to the operation of the temperature measuring device 10. It may be 929. Further, the input device 915 is composed of, for example, an input control circuit that generates an input signal based on the information input by the user using the above-described operation unit and outputs the input signal to the CPU 901. By operating the input device 915, the user of the temperature measuring device 10 can input various data to the temperature measuring device 10 and instruct a processing operation.

The output device 917 is configured by a device capable of visually or audibly notifying the user of the acquired information. Such devices include CRT display devices, liquid crystal display devices, plasma display devices, EL display devices and display devices such as lamps, audio output devices such as speakers and headphones, printer devices, mobile phones, and facsimiles. The output device 917 outputs results obtained by various processes performed by the temperature measuring device 10, for example. Specifically, the display device displays the results obtained by the various processes performed by the temperature measuring device 10 as text or images. On the other hand, the audio output device converts an audio signal composed of reproduced audio data and acoustic data into an analog signal and outputs the analog signal.

The storage device 919 is a device for storing data configured as an example of a storage unit of the temperature measuring device 10. The storage device 919 includes, for example, a magnetic storage device such as an HDD (Hard Disk Drive), a semiconductor storage device, an optical storage device, or a magneto-optical storage device. The storage device 919 stores programs executed by the CPU 901, various data, various data acquired from the outside, and the like.

The drive 921 is a reader/writer for a recording medium, and is built in or externally attached to the temperature measuring device 10. The drive 921 reads the information recorded on the removable recording medium 927 such as a mounted magnetic disk, optical disk, magneto-optical disk, or semiconductor memory, and outputs it to the RAM 905. The drive 921 can also write a record on a removable recording medium 927 such as a mounted magnetic disk, optical disk, magneto-optical disk, or semiconductor memory. The removable recording medium 927 is, for example, a DVD medium, an HD-DVD medium, a Blu-ray (registered trademark) medium, or the like. The removable recording medium 927 may be a compact flash (registered trademark) (CompactFlash: CF), a flash memory, an SD memory card (Secure Digital memory card), or the like. The removable recording medium 927 may be, for example, an IC card (Integrated Circuit card) equipped with a non-contact type IC chip, an electronic device, or the like.

The connection port 923 is a port for directly connecting the device to the temperature measuring device 10. Examples of the connection port 923 include a USB (Universal Serial Bus) port, an IEEE 1394 port, and a SCSI (Small Computer System Interface) port. Another example of the connection port 923 is an RS-232C port, an optical audio terminal, an HDMI (High-Definition Multimedia Interface) port, or the like. By connecting the external connection device 929 to the connection port 923, the temperature measuring device 10 acquires various data directly from the external connection device 929 or provides various data to the external connection device 929.

The communication device 925 is, for example, a communication interface including a communication device or the like for connecting to the communication network 931. The communication device 925 is, for example, a wired or wireless LAN (Local Area Network), Bluetooth (registered trademark), or a communication card for WUSB (Wireless USB). Further, the communication device 925 may be a router for optical communication, a router for ADSL (Asymmetrical Digital Subscriber Line), a modem for various kinds of communication, or the like. The communication device 925 can send and receive signals and the like to and from the Internet and other communication devices, for example, according to a predetermined protocol such as TCP/IP. The communication network 931 connected to the communication device 925 is configured by a network connected by wire or wirelessly, and may be, for example, the Internet, a home LAN, infrared communication, radio wave communication, satellite communication, or the like. ..

The example of the hardware configuration capable of realizing the function of the temperature measuring device 10 according to the embodiment of the present invention has been described above. Each component described above may be configured by using a general-purpose member, or may be configured by hardware specialized for the function of each component. Therefore, it is possible to appropriately change the hardware configuration to be used according to the technical level at the time of implementing the present embodiment.

(About temperature measurement method)
Next, the temperature measuring method according to the present embodiment will be described with reference to FIGS. 27 to 31. 27 to 31 are explanatory diagrams for explaining the temperature measuring method according to the present embodiment.

The temperature measuring method according to the present embodiment, as mentioned earlier, detects the thermal radiation light in the near-infrared band emitted by the measurement object, and the measurement object based on the detection result of the radiance of the thermal radiation light. It is a method of measuring the temperature of an object. More specifically, in the temperature measuring method according to the present embodiment, the light receiving unit that receives the heat radiation light of the measurement target, the detection unit that detects the heat radiation light received by the light receiving unit, the measurement target and the light receiving unit. By using a two-color radiation thermometer having a position control mechanism that changes the relative positional relationship with the position control mechanism that measures the distribution of thermal radiation light in the width direction of the measurement target by the light receiving unit. The heat radiation light is detected, and the temperature distribution along the width direction of the measurement object is measured. By using a two-color radiation thermometer, it is possible to suppress the occurrence of temperature errors due to the lack of the field of view of the radiation thermometer, even at the corners of the measurement object, and suppress temperature measurement errors at the edge of the object. However, the temperature of the measuring object can be measured more accurately.

Further, by using the more preferable temperature measuring device 10 in the present embodiment, even if an absorber such as water exists between the measurement object and the light receiving unit 111, the temperature of the measurement object Can be measured more accurately.

In the temperature measuring method according to the present embodiment, as schematically shown in FIG. 27, the position control mechanism 115 is used to change the relative positional relationship between the light receiving unit 111 and the measurement object. The temperature distribution of the measurement object in the width direction can be measured. At this time, in order to measure the temperature of the corner portion of the object to be measured more accurately by the temperature measuring device 10, the position control mechanism 115 has the position control mechanism 115 in the measurement visual field of the two-color radiation thermometer as illustrated in FIG. , The minimum radiant light amount which is the minimum radiant light amount required for temperature calculation is specified in advance, and the measured object is present until the actually detected radiant light amount is less than the minimum radiant light amount, It is preferable to change the relative positional relationship with the light receiving unit 111. In other words, the position control mechanism 115, as shown in the lower left diagram of FIG. 27, controls the light receiving unit 111 so that the amount of emitted light from the region occupied by the measurement target in the measurement field of view becomes equal to or greater than the minimum amount of emitted light. It is preferable to control the position. This makes it possible to measure the temperature of the measurement object more accurately.

Further, the position where something other than the measurement object exists within the range of the measurement visual field in the temperature measuring device 10 is regarded as the start position of the corner portion in the width direction of the measurement object, and the width direction of the measurement object is determined. It is possible to make up to the end of the corner of the measurement object. Further, a position where there is no object other than the measurement target in the measurement visual field can be regarded as a region other than the corner portion in the width direction of the measurement target.

In the two-color radiation thermometer (temperature measuring device 10) as described above, the radiance of the thermal radiation light at each of the two types of wavelengths of interest is set so as to be output independently of each other, and then the measurement is performed. It is also possible to perform the following control while scanning the temperature distribution in the width direction of the object.

For example, as shown schematically in FIG. 28, when an object other than the measurement object is located within the range of the radiance measurement field of view of the two-color radiation thermometer, the temperature measurement device 10 pays attention. Using the radiance of thermal radiation at each of the two wavelengths (in other words, in the two-color mode that functions as a two-color radiation thermometer), the temperature of the measurement target is measured, and within the range of the measurement visual field. When the object to be measured occupies, the temperature measuring device 10 uses the radiance of the thermal radiation light of one of the two types of wavelengths of interest (in other words, functions as a monochromatic radiation thermometer). The temperature of the measuring object may be measured. As a result, in the corners where temperature measurement errors tend to occur, the temperature is measured in the two-color mode, which allows more accurate temperature measurement, while the temperature measurement errors are relatively suppressed. In regions other than the above, temperature measurement can be performed in the monochromatic mode with a relatively small calculation load.

Further, the same control as that shown in FIG. 28 is focused on the angle formed by the optical axis of the light receiving unit 111 and the surface normal direction of the measurement target in the angle control mechanism as shown in FIG. 22B or 23. However, it is also possible to carry out. Here, as shown in the schematic diagram shown in FIG. 29, the distance from the temperature measuring device 10 to the measurement target (more specifically, the distance from the light receiving unit 111 to the measurement target. Is set to H [mm], the width of the measurement target is set to W [mm], and the size of the measurement diameter of the temperature measuring device 10 is set to D _L [mm]. As schematically shown in FIG. 29, the magnitude |φ| of the angle φ when the end of the measurement diameter coincides with the position of the corner of the object to be measured is the geometrical |φ| From this relationship, |φ|=|tan ^-1 [{(W/2)-( _DL /2)}/H]| can be expressed. From this, when the temperature measuring device 10 scans the temperature distribution in the width direction of the measurement target, the angle φ formed by the surface normal direction of the measurement target and the optical axis of the light receiving unit 111 is |φ|=|tan ^-1 [{(W/2)-(D _L /2)}/H]| When the value represented by | is exceeded, inside the measurement diameter, Because of the existence of objects, the temperature measuring device 10 functions in the dichroic mode, and measures the temperature of the object to be measured using the radiance of the thermal radiation light at each of the two types of wavelengths of interest. To do. On the other hand, the size of the angle φ formed by the surface normal direction of the measurement target and the optical axis of the light receiving unit 111 is |φ|=|tan ⁻¹ [{(W/2)−(D _L /2)). }/H]|, the temperature measuring device 10 functions in the single-color mode, and there is no object other than the measurement object inside the measurement diameter. The temperature of the measurement object may be measured using the radiance of the thermal radiation light of either one of the two types of wavelengths.

When performing the switching control between the two-color mode and the single-color mode as described above, the wavelength of the thermal radiance used in the single-color mode is preferably a wavelength that is less likely to be affected by the absorber such as water. ..

The temperature of the measuring object measured according to the method described above is a temperature calculated based on the information obtained from all the measurement visual fields. However, when outputting the obtained temperature, it is important to associate at which position in the width direction of the measurement target the temperature is measured. Therefore, in the temperature measuring method according to the present embodiment, when outputting the temperature of the measurement object, the center of gravity position of the region occupied by the measurement object in the measurement visual field of the temperature measurement device 10 is specified, and the obtained measurement result Is preferably output in association with the specified center-of-gravity position. By outputting the temperature measurement result in association with the position of the center of gravity of the region occupied by the measurement object in the measurement field of view, it is possible to more accurately grasp the temperature distribution along the width direction of the measurement object. Become.

As shown schematically in FIG. 30A, when all of the measurement field of view of the temperature measuring device 10 is occupied by the measurement object, the position of the center of gravity of the region occupied by the measurement object in the measurement field of view is: It is equal to the center position of the measurement visual field.

On the other hand, as schematically shown in FIG. 30B, when a region other than the measurement object occupies the measurement visual field of the temperature measuring device 10, the center of gravity of the region occupied by the measurement object in the measurement visual field is generated. The position is different from the center position of the measurement visual field. Therefore, the temperature calculation unit 181 in the arithmetic processing unit 103 of the temperature measurement device 10 according to the present embodiment calculates the barycentric position of the region occupied by the measurement object in the measurement visual field as follows, and the obtained measurement result Is preferably associated with.

Now, let us consider a case where there is an area occupied by the measuring object (the circular arc portion shown in FIG. 31) as schematically shown in FIG. At this time, as shown in FIG. 31, the half angle of the circular arc is θ, the radius of the measurement visual field is r, the chord length is H, and half the chord length is h. In this case, the area S ₁ of the measurement visual field and the area S ₂ of the circular arc are expressed by the equations (21) and (22), respectively. Further, the following equations (23) and (24) are established from the geometrical relationship shown in FIG.

Further, the parameter x in FIG. 31 can be calculated from the geometrical relationship as “edge position of measurement object−(center position of measurement visual field O−radius r of measurement visual field)”. In addition, a relational expression representing the relationship between the attenuation rate represented by “Equation (22)/Equation (21)” and the parameter x is specified in advance to correspond to the actually measured attenuation rate of the radiance. You may specify the value of the parameter x to perform.

If the value of the parameter x at the time of actual measurement can be specified as described above, the center-of-gravity position X _G of interest can be calculated from the following equation (25).

The temperature measuring method according to the present embodiment has been described above with reference to FIGS. 27 to 31.

In the temperature measuring method according to the present embodiment, a plurality of temperature measuring devices 10 are installed in the vicinity of the corners of the object to be measured, and then the temperature measurement result obtained from each temperature measuring device 10 is determined to determine the corners. May be evaluated.

Further, as the temperature measuring device 10, it is also possible to use a thermoviewer or the like that can measure thermal radiation light at a specific wavelength.

A temperature measuring device 10 (wavelength λ ₁ =1.2 μm, λ ₂ =1.3 μm, detector: InGaAs detector) according to the present invention is prepared, and a general monochromatic thermometer (wavelength λ=0.8 μm, Si Using a detector) and the temperature measuring device 10, a red hot steel material having a width of 2200 mm and heated to 900° C. or higher was used as a measurement target, and the temperature near the end portion thereof was measured. The distance between each thermometer and the object to be measured is 1174 mm in the case of a monochromatic thermometer and 2000 mm in the case of the temperature measuring device 10 so that the size of both measurement diameters is 49 mm. did.

As shown schematically in FIG. 30, the displacement amount=0 when the end of the measurement field of view of each thermometer was in contact with the corner, and each thermometer was displaced in the direction shown in FIG. .. By displacing each of the thermometers in this way, a visual field loss occurs.

The obtained results are shown in FIG.
As is clear from FIG. 33, in the case of using the monochromatic thermometer, when the displacement amount exceeds 0 and the visual field loss occurs, the temperature immediately decreases, whereas the temperature measuring device according to the present invention. In No. 10, it can be confirmed that the temperature can be accurately measured in the period from the occurrence of the visual field loss to the displacement of 29 mm.

Further, a temperature measuring device 10 (wavelength λ ₁ =1.2 μm, λ ₂ =1.3 μm, detector: InGaAs detector) according to the present invention is prepared, and a general monochromatic thermometer (wavelength λ=1.0 μm) is prepared. , InGaAs detector) and the temperature measuring device 10 were used to measure the temperature of the slab during casting by a continuous casting machine. The obtained results are shown in FIG. 34. In FIG. 34, the obtained measurement result is associated with the position of the center of gravity of the measurement visual field and output.

As is clear from FIG. 34, it is understood that the monochromatic thermometer and the temperature measuring device 10 output almost the same temperature up to the outermost edge portion (a position near 750 mm in FIG. 34) of the slab having a width of 1500 mm. ..

On the other hand, focusing on the outermost edge portion, a general single-color thermometer shows a high temperature of 650 to 700° C. even after passing the outermost edge portion, while the temperature measuring device 10 of the present invention displays the outermost edge portion. When it passes, the lower limit temperature is indicated. From these results, it was confirmed that the temperature of the object to be measured could be accurately measured by the temperature measuring method using the temperature measuring device 10 according to the present invention.

The preferred embodiments of the present invention have been described in detail above with reference to the accompanying drawings, but the present invention is not limited to these examples. It is obvious that a person having ordinary knowledge in the technical field to which the present invention pertains can come up with various changes or modifications within the scope of the technical idea described in the claims. Of course, it is understood that these also belong to the technical scope of the present invention.

10 temperature measuring device 101 measuring unit 103 arithmetic processing unit 105 storage unit 111 light receiving unit 113 detecting unit 121 light receiving lens 123, 151 connection coupler 153 beam splitters 155a, 155b optical filter 157a, 157b condensing lens 159a, 159b sensor 171 measurement control unit 173 Data acquisition unit 175,181 Temperature calculation unit 183 Thickness calculation unit 177,185 Result output unit 179 Display control unit

Claims (15)

Detecting the near infrared band thermal radiation emitted by the measurement object, a temperature measuring method for measuring the temperature of the measurement object based on the detection result of the radiance of the thermal radiation light,
A light receiving unit that receives the thermal radiation light of the measurement object, a detection unit that detects the thermal radiation light received by the light receiving unit, and a relative positional relationship between the measurement object and the light receiving unit is changed. By using a two-color radiation thermometer having a position control mechanism for measuring the distribution of the thermal radiation light in the width direction of the measurement object by the light receiving unit, the thermal radiation light of the measurement object is used. A temperature measuring method of detecting and measuring a temperature distribution along the width direction of the measurement target including the vicinity of the end of the measurement target. The two-color radiation thermometer, the minimum radiant light amount which is the minimum radiant light amount required for temperature calculation in the measurement visual field of the two-color radiation thermometer is specified in advance,
The position control mechanism changes the relative positional relationship between the measurement target and the light receiving unit until the amount of emitted light detected in the measurement field of view of the two-color radiation thermometer becomes less than the minimum amount of emitted light. The temperature measuring method according to claim 1. The temperature measuring method according to claim 1, wherein the position control mechanism is an angle control mechanism that changes an angle formed by a surface normal direction of the measurement target and an optical axis of the light receiving unit. The angle control mechanism, between the measurement object and the light guide optical system that guides the thermal radiation light to the detection unit, a mirror provided obliquely to the surface normal direction, The angle formed between the surface normal direction and the optical axis of the light receiving section is changed by rotating the measurement object by a predetermined angle with the longitudinal direction as a rotation axis. Temperature measurement method. The temperature control method according to claim 1, wherein the position control mechanism is a drive mechanism that moves the light receiving unit along a width direction of the measurement target. The two-color radiation thermometer is a two-color radiation thermometer capable of independently outputting the radiance of the thermal radiation light at each of two wavelengths of interest.
While scanning the temperature distribution in the width direction of the measurement object,
When an object other than the measurement object is located within the range of the radiance measurement field of view of the two-color radiation thermometer, the two-color radiation thermometer is used for each of the two types of wavelengths of interest. Using the radiance of the thermal radiation, to measure the temperature of the measurement object,
When the measurement object occupies the range of the measurement visual field, the two-color radiation thermometer uses the radiance of the thermal radiation light in one of two wavelengths of interest. The temperature measuring method according to claim 1, wherein the temperature of the measurement target is measured. The distance from the two-color radiation thermometer to the measurement object is H [mm], the size of the measurement diameter of the two-color radiation thermometer is D _L [mm], and the width of the measurement object is W[ mm],
The two-color radiation thermometer is a two-color radiation thermometer capable of independently outputting the radiance of the thermal radiation light at each of two wavelengths of interest, and as the position control mechanism, the measurement is performed. The surface normal direction of the object, and the optical axis of the light-receiving unit, has an angle control mechanism for changing the angle formed,
While scanning the temperature distribution in the width direction of the measurement object,
The magnitude of the angle formed by the surface normal direction of the measurement object and the optical axis of the light receiving section is |φ|=|tan ⁻¹ [{(W/2)−(D _L /2)}/H. ] When the value represented by | is exceeded, the two-color radiation thermometer uses the radiance of the thermal radiation light at each of the two types of wavelengths of interest to determine the temperature of the measurement object. Measure
The magnitude of the angle formed by the surface normal direction of the measurement object and the optical axis of the light receiving section is |φ|=|tan ⁻¹ [{(W/2)−(D _L /2)}/H. ] When the value is less than or equal to the value represented by |, the two-color radiation thermometer uses the radiance of the thermal radiation light of one of the two types of wavelengths of interest to measure the measurement target. The temperature measuring method according to claim 1, wherein the temperature of the object is measured. The two-color radiation thermometer,
Calculate the dichroic ratio by dividing one of the measurement data of the radiance at the two types of wavelengths of interest by the other,
The temperature measurement according to any one of claims 1 to 7, wherein the calculated dichroic ratio is used to calculate the temperature of the measurement object based on a relational expression between the dichroic ratio and temperature. Method. The two-color radiation thermometer,
In a state in which an absorber having a wavelength dependence of a spectral absorption coefficient in the near-infrared band is present in at least a part of an optical path, the thermal radiation of the measurement object is absorbed by the spectral absorption of the absorber. Generating measurement data showing the detection results of the radiance of the thermal radiation light at the two wavelengths having the same coefficient, respectively, and
The temperature of the measurement object is calculated based on the generated measurement data corresponding to the two types of wavelengths and a relational expression between spectral radiance and temperature. The method for measuring temperature according to item 1. The detection unit,
A branching optical element for branching the thermal radiation of the measurement object into two optical paths;
A first detection element that detects the branched thermal radiation light at one of the two types of wavelengths;
A second detection element that detects the branched thermal radiation light at the other wavelength of the two types of wavelengths;
A first optical filter which is provided between the branch optical element and the first detection element, and which transmits the thermal radiation light having one wavelength of the two types of wavelengths;
A second optical filter that is provided between the branch optical element and the second detection element and that transmits the thermal radiation light of the other wavelength of the two types of wavelengths;
The temperature measuring method according to claim 9, further comprising: As the two types of wavelengths, two types of wavelength bands having a predetermined width including wavelengths at which the spectral absorption coefficients of the absorber are the same are selected,
10. The two types of the wavelength bands are selected so that the apparent spectral absorption coefficients calculated by weighted averaging the spectral absorption coefficients of the absorber with the spectral radiance of the temperature to be measured are equal to each other. Alternatively, the method for measuring temperature according to item 10. The two-color radiation thermometer calculates a black body radiance at any of the two types of wavelengths calculated using the temperature of the measurement object, the radiance of the measured thermal radiation, and the absorber. Of the spectral absorption coefficient at the two types of wavelengths, the reflectance of the thermal radiation light at the interface of the absorber on the side of the measurement object, the reflectance of the thermal radiation light at the interface of the absorber, and the detection The temperature measuring method according to any one of claims 9 to 11, wherein the thickness of the absorber is further calculated using the setting conditions in the section. The temperature measuring method according to any one of claims 8 to 12, wherein the absorber is at least one of water, oil and fat, a solution, glass, and a resin. The measurement result of the temperature of the measurement object is output in association with the position of the center of gravity of the region occupied by the measurement object in the measurement visual field of the two-color radiation thermometer. The method for measuring temperature according to item. The temperature measuring method according to claim 1, wherein the near-infrared band is 940 nm to 1350 nm.

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