JPH02228529A - Reference temperature source apparatus - Google Patents

Reference temperature source apparatus

Info

Publication number
JPH02228529A
JPH02228529A JP1050370A JP5037089A JPH02228529A JP H02228529 A JPH02228529 A JP H02228529A JP 1050370 A JP1050370 A JP 1050370A JP 5037089 A JP5037089 A JP 5037089A JP H02228529 A JPH02228529 A JP H02228529A
Authority
JP
Japan
Prior art keywords
black body
temperature
temperature difference
reference temperature
black
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP1050370A
Other languages
Japanese (ja)
Inventor
Masaru Kurokawa
黒川 賢
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Avio Infrared Technologies Co Ltd
Original Assignee
NEC Avio Infrared Technologies Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Avio Infrared Technologies Co Ltd filed Critical NEC Avio Infrared Technologies Co Ltd
Priority to JP1050370A priority Critical patent/JPH02228529A/en
Publication of JPH02228529A publication Critical patent/JPH02228529A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To enable accurate measurement with one black body by developing a specified temperature difference between one end and the other end of a metal body while a plurality of black body sections are formed therebetween. CONSTITUTION:When one end 21a of a metal body 21 is cooled with an electronic cooling element 23 while the other end 21b thereof is heated with a heater 24, a temperature difference is developed between one end 21a and the other end 21b thereof, which in turn generates a temperature gradient between one end 21a and the other end 21b thereof 21. Hence, a radiation energy level varies among black body sections 22 to make them as a reference temperature source with a temperature difference. Moreover, the black body sections can produce any fine temperature difference as desired by varying a position where they are set and a shape or the like of the metal body 21. Thus, a photographing is performed directly with a thermography device using the black body section 22 as reference temperature source thereby enabling direct evaluation with only one black body.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、放射温度計の校正やサーモグラフィ装置の校
正及び精度測定の際に使用して好適な基準温度源装置に
関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a reference temperature source device suitable for use in calibrating radiation thermometers, calibrating thermography devices, and measuring accuracy.

〔発明の概要〕[Summary of the invention]

本発明は、放射温度計の校正やサーモグラフィ装置の精
度測定の際に使用して好適な基準温度源装置に関し、金
属体の一端と他端とが所定の温度差となる様にすると共
に、この金属体の一端と他端との間に複数個の黒体部を
形成したことにより、サーモグラフィ装置の校正及び精
度測定をより正確に行えるようにしたものである。
The present invention relates to a reference temperature source device suitable for use in calibrating a radiation thermometer or measuring the accuracy of a thermography device. By forming a plurality of black body parts between one end and the other end of the metal body, it is possible to more accurately calibrate and measure the accuracy of the thermography apparatus.

〔従来の技術〕[Conventional technology]

従来、被測定物の表面から放射される赤外線エネルギー
を検出して温度を測定する放射温度計においては、メー
カーでの出荷時等に基準温度源としての黒体を用いて校
正を行っている。この黒体は第6図に示す如く、黒体炉
(1)と温度制御部(2)とから構成されており、黒体
炉(1)の発熱体には2本の白金抵抗線(JISo、5
級) (3)、(4)が埋め込まれており、一方の白金
抵抗線(3)は温度制御用に、他方の白金抵抗線(4)
は温度検出用に夫々用いられる。
Conventionally, radiation thermometers that measure temperature by detecting infrared energy emitted from the surface of a measured object are calibrated using a blackbody as a reference temperature source at the time of shipment from the manufacturer. As shown in Figure 6, this blackbody is composed of a blackbody furnace (1) and a temperature control section (2), and the heating element of the blackbody furnace (1) has two platinum resistance wires (JIS , 5
(3) and (4) are embedded, one platinum resistance wire (3) is for temperature control and the other platinum resistance wire (4) is embedded.
are used for temperature detection.

温度制御用の白金抵抗線(3)は、ブリッジの一辺を形
成し、他の辺の抵抗値を変化させ、目標温度を設定する
。このブリッジ回路(5)の不平衡電圧を増幅回路(6
)で増幅した後、同期検波回路(7)で同期検波し、こ
の同期検波信号で位相制御回路(8)を動作させて黒体
炉(1)内のヒータ(9)に流れる電流を増減させて目
標温度に安定させるようにする。
A platinum resistance wire (3) for temperature control forms one side of the bridge, changes the resistance value of the other side, and sets the target temperature. The unbalanced voltage of this bridge circuit (5) is converted into an amplifier circuit (6).
), the signal is synchronously detected by the synchronous detection circuit (7), and this synchronous detection signal operates the phase control circuit (8) to increase or decrease the current flowing to the heater (9) in the blackbody furnace (1). temperature to stabilize it at the target temperature.

また、温度検出用の白金抵抗体の抵抗値と同じになるよ
うに可変抵抗器(10)のダイヤルをセットし、比較器
(11)の出力が零になれば、指示メータ(12)が零
を示すように調整されており、この可変抵抗器(10)
のダイヤルの読みから黒体の温度を正確に知ることがで
きる。
Also, set the dial of the variable resistor (10) so that the resistance value is the same as the platinum resistor for temperature detection, and when the output of the comparator (11) becomes zero, the indicator meter (12) will read zero. This variable resistor (10) is adjusted to show
The temperature of the black body can be determined accurately by reading the dial.

黒体の温度が決まれば、この黒体から放出される赤外線
エネルギーの値も決まり、この黒体に対して放射温度計
を向ければ、この黒体を基準温度源として放射温度計の
校正を行うことができる。
Once the temperature of the black body is determined, the value of infrared energy emitted from this black body is also determined, and by pointing the radiation thermometer at this black body, the radiation thermometer is calibrated using this black body as a reference temperature source. be able to.

ところで、放射温度計が被測定物の温度測定に使われる
のに対して、原理的には同じだが、被測定物の温度分布
を放射温度計で測定し、温度に対応したカラー又はモノ
クロの画像として表示するサーモグラフィ装置がある。
By the way, while a radiation thermometer is used to measure the temperature of a measured object, the principle is the same, but a radiation thermometer measures the temperature distribution of the measured object and produces a color or monochrome image corresponding to the temperature. There is a thermography device that displays as

そしてこのサーモグラフィ装置においてはその精度(感
度の良さ)を示す目安として最小検知温度差(Nois
e EquivalentTemperature D
ifference : N E T D )がある。
In this thermography device, the minimum detectable temperature difference (Nois) is used as a measure of its accuracy (sensitivity).
e Equivalent Temperature D
difference: NETD).

即ち、サーモグラフィ装置では温度分布測定が目的であ
るから、どれだけの温度差までがどの程度識別できるか
が重要で、NETDは放射温度計の温度信号中に含まれ
る雑音電圧を等価的に温度差に換算した数値で示し、こ
のNETDが小さいほど、温度分布測定に関する感度の
良さを表わす。
In other words, since the purpose of a thermography device is to measure temperature distribution, it is important to be able to distinguish between temperature differences and to what extent. NETD can equivalently convert the noise voltage contained in the temperature signal of a radiation thermometer into a temperature difference. The smaller the NETD, the better the sensitivity regarding temperature distribution measurement.

このNETDの測定方法例としては、温度の異る二つの
黒体からなる標準炉(標準炉A、標準炉B)を撮像装置
(15)により撮像しく第7図参照)、そのときの信号
波形(第8図参照)をブラウン管オシロスコープ(16
)により観測し、次式(1)によってNETDを算出す
る。なお、医用赤外線撮像装置の場合は標準炉Aの温度
TAは30士ビC9標準炉Bの温度T、は35±1 ’
Cとする。
As an example of how to measure NETD, a standard furnace (standard furnace A, standard furnace B) consisting of two black bodies with different temperatures is imaged using an imaging device (15) (see Figure 7), and the signal waveform at that time is (See Figure 8) with a cathode ray tube oscilloscope (16
), and NETD is calculated using the following equation (1). In addition, in the case of a medical infrared imaging device, the temperature TA of standard furnace A is 30 cm, and the temperature T of standard furnace B is 35 ± 1'.
Let it be C.

ここに、NETD:最小検知温度差(°C)T p、、
 T m :標準炉A、標準炉Bの温度(°C)S;標
準炉A、標準炉Bの信号の 電圧差(V) N1.:雑音電圧のP−P値(V) [発明が解決しようとする課題] しかしながら、従来のNETDの測定方法においては、
2個の黒体を使用しているため大型化するとかコスト高
になるという不都合が有り、また、黒体において温度検
出用の白金抵抗線をその確度が0.15級のものを採用
したとしても、そのバラツキにより0.1°C等の微小
温度差の黒体を2個実現させることは困難で、そのため
前述した如き方法で間接評価している。
Here, NETD: Minimum detectable temperature difference (°C) T p,,
T m : Temperature of standard furnace A and standard furnace B (°C) S; Voltage difference between signals of standard furnace A and standard furnace B (V) N1. : P-P value (V) of noise voltage [Problem to be solved by the invention] However, in the conventional NETD measurement method,
Since two black bodies are used, there are disadvantages such as increase in size and cost.Also, even if a platinum resistance wire for temperature detection is used for the black bodies, the accuracy of which is 0.15 class. However, due to the variation, it is difficult to realize two black bodies with a minute temperature difference such as 0.1° C. Therefore, indirect evaluation is performed using the method described above.

本発明は斯かる点に鑑み、1個の黒体で正確な精度測定
が行える基準温度源装置を提案することを目的とする。
In view of the above, an object of the present invention is to propose a reference temperature source device that can perform accurate precision measurements using a single black body.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の基準温度源装置は、例えば第1図に示す如く、
金属体(21)の一端(21a)と他端(21b)とが
所定の温度差となるようにすると共に、この金属体(2
1)の一端(21a)と他端(21b)との間に複数個
の黒体部(22)を形成するようにしたものである。
The reference temperature source device of the present invention is, for example, as shown in FIG.
The metal body (21) is made to have a predetermined temperature difference between one end (21a) and the other end (21b), and
1) A plurality of blackbody portions (22) are formed between one end (21a) and the other end (21b).

〔作用] 斯かる本発明によれば、金属体(21)の一端(21a
)と他端(21b)との間においては所定の温度勾配が
生じ、この金属体(21)の一端(21a)と他端(2
1b)との間の適宜箇所に形成された複数の黒体部(2
2)は互いに所定の微小温度差を持った基準温度源とな
り、この微小温度差の基準温度源を直接撮像すれば、ど
の程度の温度差まで識別できるか直接評価でき、サーモ
グラフィ装置の校正及び精度測定を1個の黒体で正確に
1行うことができる。
[Function] According to the present invention, one end (21a) of the metal body (21)
) and the other end (21b), a predetermined temperature gradient occurs between the one end (21a) and the other end (21b) of this metal body (21).
A plurality of black body parts (2) formed at appropriate locations between
2) serves as a reference temperature source with a predetermined minute temperature difference from each other, and by directly imaging the reference temperature source with a minute temperature difference, it is possible to directly evaluate how much temperature difference can be discriminated, which improves the calibration and accuracy of thermography equipment. Accurately one measurement can be performed with one blackbody.

〔実施例〕〔Example〕

以下、本発明基準温度源装置の一実施例を第1図乃至第
4図を参照して説明する。
Hereinafter, one embodiment of the reference temperature source device of the present invention will be described with reference to FIGS. 1 to 4.

第1図乃至第4図において従来と同一構成要素には同一
符号を付し、その詳細説明は省略する。
In FIGS. 1 to 4, the same components as those of the conventional system are given the same reference numerals, and detailed explanation thereof will be omitted.

(21)は金属体としての金属六角柱で、例えば銅。(21) is a metal hexagonal prism as a metal body, for example copper.

黄銅等から成り、その一端(21a)と他端(21b)
とが所定の温度差となる様に、一端(21a)側には冷
却手段としての電子冷却素子(23)が設けられ、他端
(21b)側には加熱手段としてのニクロム線等のヒー
タ(24)が設けられている。そして、金属六角柱(2
1)の一端(21a)と他端(21b)との間には適宜
間隔を置いて複数個の黒体部(22)が設けられている
Made of brass etc., one end (21a) and the other end (21b)
An electronic cooling element (23) as a cooling means is provided on one end (21a) side, and a heater (such as a nichrome wire) as a heating means is provided on the other end (21b) side so that a predetermined temperature difference between 24) is provided. Then, a metal hexagonal column (2
1) A plurality of black body portions (22) are provided at appropriate intervals between one end (21a) and the other end (21b).

この黒体部(22)は放射率の高い塗料を塗布すること
によって形成されているが、穴を設けて実効放射率を上
げることにより形成してもよい。なお、(25)は一端
(21a)側の測温抵抗体、(26)は他端(21b)
側の測温抵抗体を夫々示している。
Although this black body portion (22) is formed by applying a paint with high emissivity, it may also be formed by providing holes to increase the effective emissivity. In addition, (25) is the resistance temperature detector on one end (21a) side, and (26) is the other end (21b).
The temperature measuring resistors on the sides are shown respectively.

このような基準温度源装置としての黒体においては、金
属六角柱(21)の一端(21a)を電子冷却素子(2
3)で冷却し、他端(21b)をヒータ(24)で加熱
すれば、一端(21a)と他端(21b)との間に温度
差が生じ、金属六角柱(21)の一端(21a)と他端
(21b)との間で温度勾配が生じる。従って各黒体部
(22)における放射エネルギー量は第4図に示すよう
に異なることとなり、各黒体部(22)は温度差を持っ
た基準温度源となる。しかも、この黒体部(22)を設
ける位置や、金属六角柱(21)の形状等を変えること
により、各黒体部(22)は任意の微小温度差とすると
ができる。
In such a black body as a reference temperature source device, one end (21a) of the metal hexagonal column (21) is connected to the electronic cooling element (2).
3) and then heat the other end (21b) with the heater (24), a temperature difference will be created between one end (21a) and the other end (21b), and one end (21a) of the metal hexagonal column (21) will be cooled. ) and the other end (21b). Therefore, the amount of radiant energy in each black body part (22) differs as shown in FIG. 4, and each black body part (22) serves as a reference temperature source with a temperature difference. Moreover, by changing the position of the black body part (22), the shape of the metal hexagonal column (21), etc., each black body part (22) can have an arbitrary minute temperature difference.

従って、このような微小温度差の黒体部(22)を基準
温度源としてサーモグラフィ装置により直接撮像すれば
、どの程度の温度差まで識別できるか一台の黒体で直接
評価でき、サーモグラフィ装置の精度測定を小型化され
た装置で極めて容易且つ正確に行うことができる。また
、このような黒体を放射温度計の基準温度源に用いれば
、従来の一点測定に対して複数点測定が容易に行えるこ
ととなり、放射温度計の校正もより正確に行うことがで
きる。
Therefore, if the black body part (22) with such minute temperature difference is directly imaged with a thermography device as a reference temperature source, it is possible to directly evaluate how much temperature difference can be discriminated with a single black body, and the temperature difference of the thermography device can be directly evaluated. Accuracy measurement can be performed extremely easily and accurately using a miniaturized device. Further, if such a black body is used as a reference temperature source of a radiation thermometer, multiple point measurements can be easily performed instead of the conventional single point measurement, and the radiation thermometer can be calibrated more accurately.

第5図は本発明の他の実施例を示しているが、上述の実
施例との相違する点を述べれば、冷却手段として電子冷
却素子等の高価なものを用いず、ファン(図示せず)等
を用いて一端を放熱手段(28)により周囲温度程度に
保つようにしたものである。
FIG. 5 shows another embodiment of the present invention, and the difference from the above embodiment is that an expensive cooling device such as an electronic cooling element is not used, and a fan (not shown) is used as the cooling means. ), etc., and one end is kept at around ambient temperature by means of heat dissipation means (28).

このようにした黒体においても上述の実施例と同等の効
果を奏する。
A blackbody constructed in this manner also provides the same effects as those of the above-mentioned embodiments.

なお、上述の実施例においては金属体として金属六角柱
のものを述べたが、金属板でもよい。
In the above embodiment, a metal hexagonal column was used as the metal body, but a metal plate may also be used.

また、本発明は上述実施例に限定されるものではなく、
本発明の要旨を逸脱しない範囲で種々の構成がとりうろ
ことは勿論である。
Furthermore, the present invention is not limited to the above-mentioned embodiments,
Of course, various configurations are possible without departing from the gist of the present invention.

夕である。It is evening.

〔発明の効果] 以上述べた如く、本発明によれば、サーモグラフィ装置
の精度測定を一台の黒体で極めて正確に行うことができ
る利益がある。
[Effects of the Invention] As described above, according to the present invention, there is an advantage that accuracy measurement of a thermography apparatus can be performed extremely accurately using a single black body.

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

第1図は本発明基準温度源装置の一実施例の要部を示す
斜視図、第2図は第1図の一側(低温側)の構成図、第
3図は第1図の他側(高温側)の構成図、第4図は放射
エネルギー量と各黒体部位置との関係を示す線図、第5
図は本発明の他の実施例を示す全体構成図、第6図は従
来の黒体の全体構成図、第7図は従来のサーモグラフィ
装置の精度測定の概略構成図、第8図は第7図の装置に
よって得られた信号を示す線図である。
Fig. 1 is a perspective view showing the main parts of an embodiment of the reference temperature source device of the present invention, Fig. 2 is a configuration diagram of one side (low temperature side) of Fig. 1, and Fig. 3 is the other side of Fig. 1. (high temperature side); Figure 4 is a diagram showing the relationship between the amount of radiant energy and the position of each black body;
Figure 6 is an overall configuration diagram showing another embodiment of the present invention, Figure 6 is an overall configuration diagram of a conventional black body, Figure 7 is a schematic configuration diagram of accuracy measurement of a conventional thermography device, and Figure 8 is a diagram showing the overall configuration of a conventional black body. FIG. 2 is a diagram showing the signals obtained by the illustrated device;

Claims (1)

【特許請求の範囲】[Claims] 金属体の一端と他端とが所定の温度差となる様にすると
共に、上記金属体の一端と他端との間に複数個の黒体部
を形成したことを特徴とする基準温度源装置。
A reference temperature source device characterized in that a predetermined temperature difference exists between one end and the other end of the metal body, and a plurality of black body portions are formed between the one end and the other end of the metal body. .
JP1050370A 1989-03-02 1989-03-02 Reference temperature source apparatus Pending JPH02228529A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1050370A JPH02228529A (en) 1989-03-02 1989-03-02 Reference temperature source apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1050370A JPH02228529A (en) 1989-03-02 1989-03-02 Reference temperature source apparatus

Publications (1)

Publication Number Publication Date
JPH02228529A true JPH02228529A (en) 1990-09-11

Family

ID=12857005

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1050370A Pending JPH02228529A (en) 1989-03-02 1989-03-02 Reference temperature source apparatus

Country Status (1)

Country Link
JP (1) JPH02228529A (en)

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