JPS61126440A - Temperature measuring device - Google Patents

Temperature measuring device

Info

Publication number
JPS61126440A
JPS61126440A JP24740784A JP24740784A JPS61126440A JP S61126440 A JPS61126440 A JP S61126440A JP 24740784 A JP24740784 A JP 24740784A JP 24740784 A JP24740784 A JP 24740784A JP S61126440 A JPS61126440 A JP S61126440A
Authority
JP
Japan
Prior art keywords
temperature
thermocouple
cooling pipe
cooling
radiator
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
JP24740784A
Other languages
Japanese (ja)
Inventor
Akira Yamada
明 山田
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.)
Mitsubishi Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries 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 Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP24740784A priority Critical patent/JPS61126440A/en
Publication of JPS61126440A publication Critical patent/JPS61126440A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01KMEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K13/00Thermometers specially adapted for specific purposes
    • G01K13/02Thermometers specially adapted for specific purposes for measuring temperature of moving fluids or granular materials capable of flow

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Temperature Or Quantity Of Heat (AREA)

Abstract

PURPOSE:To take a measurement securely without any influence of a high- temperature radiator by providing a cooling means which cools a cylinder wherein fluid to be measured flows to specific temperature and calculating a temperature value at which the temperature measured value of the object body coincides with the temperature measured value of the cylinder. CONSTITUTION:The 1st thermocouple 10 are installed at the space part of the cylinder body 14 where gas 12 flows and the 2nd thermocouple 17 are installed nearby a cooling pipe 15 provided on the side wall of the cylinder body 14. Then, when the radiator 13 having the quantity Qr of heat at temperature T1 is present nearby the cylinder body 14, the quantity Qg of cooling heat of a cooling material 16 supplied to the cooling pipe 15 is set to a specific value at which the heat conduction between the 1st thermocouple 10 and cooling pipe 15 is eliminated, and then the temperature T2 of the cooling pipe 15 is made coincident with the temperature measured value Tm of the 1st thermocouple 10. Consequently, the temperature measure value Tm is obtained as the actual temperature Tg of the gas 12 after the influence of the radiator 13 is removed.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、特にガス流体の温度測定を行なう温度測定装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a temperature measuring device, in particular for measuring the temperature of a gaseous fluid.

[従来技術] 従来、ガスの温度を測定するには、例えば第3図に示す
ような熱雷対10を使用した温度測定装置が用いられる
ことが多い。この温度測定装置は、熱雷対10の一端を
一定の温度(冷接点)に保持し、端子間の熱起電力を測
定することにより他端11(熱接点)の温度を求めるよ
うに構成されている。
[Prior Art] Conventionally, in order to measure the temperature of gas, a temperature measuring device using a thermal lightning pair 10 as shown in FIG. 3, for example, is often used. This temperature measuring device is configured to maintain one end of the thermal lightning pair 10 at a constant temperature (cold junction) and determine the temperature of the other end 11 (hot junction) by measuring the thermoelectromotive force between the terminals. ing.

この他端11が第3図に示すようにガス流体12に接近
することにより、他端11の温度Tmとガス流体12の
温度TOとが一致することになる。このため、他f41
1の濃度Tmを求めることにより、被測温流体であるガ
ス流体12の温度Toを求めることが可能となる。
When the other end 11 approaches the gas fluid 12 as shown in FIG. 3, the temperature Tm of the other end 11 and the temperature TO of the gas fluid 12 match. For this reason, other f41
By determining the concentration Tm of 1, it becomes possible to determine the temperature To of the gas fluid 12, which is the fluid to be measured.

[発明が解決しようとする問題点] ところで、熱電対10の近くに高温の輻射体13が存在
すると、輻射体13の熱量Qrが熱電対10に伝えられ
て、ガス流体12の温度測定に悪影響を及ぼすことにな
る。具体的には、熱電対1oの熱量Qcが伝えられるガ
ス流体12の温度Toと熱電対1oの温度Tmとが一致
しなくなるような事態が発生する。例えば、輻射体13
の温度T1がガス流体12の温度TQより大きい場合、
濃度Tgが熱電対10の温度Tmより小さくなる。また
逆に温度T1が温度TOより小さい場合、温度Tgが熱
電対10の温度Tmより大きくなる。
[Problems to be Solved by the Invention] By the way, if a high-temperature radiator 13 exists near the thermocouple 10, the amount of heat Qr of the radiator 13 is transmitted to the thermocouple 10, which adversely affects the temperature measurement of the gas fluid 12. This will affect the Specifically, a situation occurs in which the temperature To of the gas fluid 12 to which the amount of heat Qc of the thermocouple 1o is transferred does not match the temperature Tm of the thermocouple 1o. For example, the radiator 13
If the temperature T1 of is greater than the temperature TQ of the gas fluid 12,
The concentration Tg becomes smaller than the temperature Tm of the thermocouple 10. Conversely, when temperature T1 is smaller than temperature TO, temperature Tg becomes larger than temperature Tm of thermocouple 10.

本発明の目的は、前記のような問題点を解決するための
もので、高温の輻射体が温度測定範囲に接近して存在す
る場合でも、ガス等の流体の温度を確実に測定すること
ができる温度測定装置を提供することにある。
The purpose of the present invention is to solve the above-mentioned problems, and it is possible to reliably measure the temperature of a fluid such as gas even when a high-temperature radiant is present close to the temperature measurement range. The objective is to provide a temperature measuring device that can.

[問題点を解決するための手段及び作用]本発明は、被
測温流体を流過させる筒体を所定の温度で冷却する冷却
手段を設け、被測温流体の温度計測値と筒体の温度計測
値とが一致する温度値を求めるように構成する。
[Means and effects for solving the problems] The present invention provides a cooling means for cooling the cylinder through which the temperature-measuring fluid flows to a predetermined temperature, and the temperature measurement value of the temperature-measuring fluid and the cylinder body are combined. It is configured to find a temperature value that matches the measured temperature value.

このような構成により、筒体に輻射体から熱量が伝えら
れる場合でも、その輻射体の影響を除去でき、確実に被
測温流体の温度を測定することが可能となる。
With such a configuration, even when heat is transmitted from the radiant to the cylinder, the influence of the radiant can be removed, and the temperature of the temperature-measuring fluid can be reliably measured.

[実施例コ 以下図面を参照して本発明の一実施例を説明する。第1
図は一実施例に係わる温度測定装置の構成を示す斜視図
である。第1図において、筒体14は、被測温流体であ
る例えばガス流体12を導入流過させる被測温部である
。この筒体14の空間部には、ガス流体12の温度を計
測するための第1の熱電対10が設置されている。筒体
14の側壁には冷却管15が設置されており、この冷却
管15に所定の温度の冷却材16が供給される。さらに
、筒体14の側壁には冷却管15の温度を計測するため
の第2の熱雷対17が設置されている。
[Embodiment] An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure is a perspective view showing the configuration of a temperature measuring device according to an embodiment. In FIG. 1, the cylindrical body 14 is a temperature-measuring section through which a temperature-measuring fluid, for example, a gas fluid 12, is introduced and flows. A first thermocouple 10 for measuring the temperature of the gas fluid 12 is installed in the space of the cylinder 14 . A cooling pipe 15 is installed on the side wall of the cylinder 14, and a coolant 16 at a predetermined temperature is supplied to the cooling pipe 15. Furthermore, a second thermal lightning pair 17 for measuring the temperature of the cooling pipe 15 is installed on the side wall of the cylindrical body 14 .

このような構成の温度測定装置において、同実施例の作
用効果を第2図を参照して説明する。先ず、ガス流体1
2を筒体14の内部に導入し、同時に冷却管15に所定
の流量と温度の冷却材16を供給する。ここで、第1図
に示すように、筒体14の外部で比較的接近した位置に
、温度T1で熱量Qrの輻射体13が存在すると仮定す
る。このため、輻射体13の熱量が筒体14の側壁に伝
えられて、その側壁の温度が上昇する。
In the temperature measuring device having such a configuration, the effects of this embodiment will be explained with reference to FIG. 2. First, gas fluid 1
2 is introduced into the cylindrical body 14, and at the same time, a coolant 16 at a predetermined flow rate and temperature is supplied to the cooling pipe 15. Here, as shown in FIG. 1, it is assumed that a radiator 13 with a temperature T1 and a heat amount Qr exists at a relatively close position outside the cylindrical body 14. Therefore, the amount of heat from the radiator 13 is transmitted to the side wall of the cylindrical body 14, and the temperature of the side wall increases.

上記のような状態において、冷却管15に供給される冷
却材16の冷却熱量が所定の値QOより小さい場合、第
2図に示すように冷却管15の温度T2(即ち第2の熱
電対17の温度計測値)は輻射体13により温度が高く
なり、第1の熱雷対10の温度計測値Tmより高い。さ
らに、第1の熱雷対10は冷却管15から熱が伝わるた
め、その計測値Tmは実際のガス流体12の温度Toよ
り高くなる。また逆に、冷却材16の冷却熱量が所定値
Qgより大きい場合、冷却管15の温度T2は低温にな
り、第1の熱電対10の温度計測値Tmより低下する。
In the above state, if the amount of cooling heat of the coolant 16 supplied to the cooling pipe 15 is smaller than the predetermined value QO, the temperature T2 of the cooling pipe 15 (that is, the second thermocouple 17 (temperature measurement value Tm) becomes higher due to the radiator 13 and is higher than the temperature measurement value Tm of the first thermal lightning pair 10. Furthermore, since heat is transferred to the first thermal lightning pair 10 from the cooling pipe 15, its measured value Tm becomes higher than the actual temperature To of the gas fluid 12. Conversely, when the cooling heat amount of the coolant 16 is larger than the predetermined value Qg, the temperature T2 of the cooling pipe 15 becomes low and lower than the temperature measurement value Tm of the first thermocouple 10.

このとき、第1の熱電対10から冷却管15へ熱が伝わ
るため、第1の熱電対10の温度計測値Tmは実際のガ
ス流体12の温度TOより低くなる。
At this time, since heat is transferred from the first thermocouple 10 to the cooling pipe 15, the temperature measurement value Tm of the first thermocouple 10 becomes lower than the actual temperature TO of the gas fluid 12.

冷却材16の冷却熱量が所定値QQであると、冷却管1
5の温度T2と第1の熱電対10の温度計測値Tmが第
2図に示すように一致することになる。
When the amount of cooling heat of the coolant 16 is a predetermined value QQ, the cooling pipe 1
The temperature T2 of No. 5 and the temperature measurement value Tm of the first thermocouple 10 match as shown in FIG.

即ち、冷却材16の冷却熱量Qqは輻射体13からの輻
射熱の影響を除去し、第1の熱雷対10と冷却管15間
の伝熱作用を除去できる□設定値である。これにより、
冷却管15の温度T2に一致する温度計測値Tmを、実
際のガス流体12の温度Tgとして求めることができる
That is, the amount of cooling heat Qq of the coolant 16 is a set value that can eliminate the influence of radiant heat from the radiator 13 and the heat transfer between the first thermal lightning pair 10 and the cooling pipe 15. This results in
A temperature measurement value Tm that corresponds to the temperature T2 of the cooling pipe 15 can be determined as the actual temperature Tg of the gas fluid 12.

このようにして、輻射体13が存在する場合、冷却管1
5に供給する冷却材16の冷却熱量(流量と温度により
決定する)を所定の値に調整することにより、冷却管1
5の温度T2と第1の熱雷対10の温度計測値Tmを一
致させることができる。この一致した状態を第1及び第
2の熱電対の各温度計測値から確認することにより、輻
射体13の輻射の影響を除去したガス流体12の実際の
温度Tgを、第1の熱電対10の温度計測値として求め
ることができる。
In this way, if the radiator 13 is present, the cooling pipe 1
By adjusting the amount of cooling heat (determined by the flow rate and temperature) of the coolant 16 supplied to the cooling pipe 1 to a predetermined value,
5 can be made to match the temperature measurement value Tm of the first thermal lightning pair 10. By confirming this coincident state from each temperature measurement value of the first and second thermocouples, the actual temperature Tg of the gas fluid 12 from which the influence of radiation from the radiator 13 has been removed can be determined from the first thermocouple 10. It can be obtained as a temperature measurement value.

尚、前記実施例において、筒体14は直線線上の円筒を
想定したが、これに限ることなく屈曲した円筒または角
筒の筒体でもよい。
In the above embodiments, the cylinder 14 is assumed to be a straight cylinder, but is not limited to this, and may be a bent cylinder or a rectangular cylinder.

[発明の効果] 以上詳述したように本発明によれば、高温の輻射体が温
度測定範囲に接近して存在する場合でも、ガス等の流体
の温度を確実に測定することができる。したがって、本
発明を適用すれば、例えば火炎などの輻射体が存在する
場所において、ガス等の流体の温度を測定する場合に極
めて有効となるものである。
[Effects of the Invention] As described in detail above, according to the present invention, the temperature of a fluid such as gas can be reliably measured even when a high-temperature radiator exists close to the temperature measurement range. Therefore, if the present invention is applied, it will be extremely effective when measuring the temperature of a fluid such as gas in a place where a radiant such as a flame is present.

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

第1図は本発明の一実施例に係わる温度測定装置の構成
を示す斜視図、第2図は同実施例の作用効果を説明する
ための特性図、第3図は従来の温度測定装置の動作を説
明するための図である。 10、17・・・熱電対、13・・・輻射体、14・・
・筒体、15・・・冷却管、16・・・冷却材。 出願人復代理人 弁理士 鈴江武彦 第1図
Fig. 1 is a perspective view showing the configuration of a temperature measuring device according to an embodiment of the present invention, Fig. 2 is a characteristic diagram for explaining the effects of the embodiment, and Fig. 3 is a diagram of a conventional temperature measuring device. FIG. 3 is a diagram for explaining the operation. 10, 17...Thermocouple, 13...Radiator, 14...
- Cylindrical body, 15... Cooling pipe, 16... Coolant. Applicant Sub-Agent Patent Attorney Takehiko Suzue Figure 1

Claims (1)

【特許請求の範囲】[Claims] 被測温流体を導入流過させる筒体と、この筒体を所定の
温度で冷却する冷却手段と、前記筒体内を流過する被測
温流体の温度計測を行なう第1の温度計測手段と、前記
冷却手段により冷却される前記筒体の温度計測を行なう
第2の温度計測手段とを備え、前記第1の温度計測手段
及び第2の温度計測手段の各温度計測値に基づいて前記
被測温流体の温度測定値を求めることを特徴とする温度
測定装置。
A cylindrical body through which a fluid to be measured is introduced and flows; a cooling means for cooling the cylindrical body to a predetermined temperature; and a first temperature measuring means for measuring the temperature of the fluid to be measured passing through the cylindrical body. and a second temperature measuring means for measuring the temperature of the cylindrical body cooled by the cooling means; A temperature measuring device characterized in that it obtains a temperature measurement value of a temperature measuring fluid.
JP24740784A 1984-11-22 1984-11-22 Temperature measuring device Pending JPS61126440A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24740784A JPS61126440A (en) 1984-11-22 1984-11-22 Temperature measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24740784A JPS61126440A (en) 1984-11-22 1984-11-22 Temperature measuring device

Publications (1)

Publication Number Publication Date
JPS61126440A true JPS61126440A (en) 1986-06-13

Family

ID=17162972

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24740784A Pending JPS61126440A (en) 1984-11-22 1984-11-22 Temperature measuring device

Country Status (1)

Country Link
JP (1) JPS61126440A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7543983B2 (en) * 2005-12-30 2009-06-09 Hon Hai Precision Industry Co., Ltd. Device for measuring temperature of heat pipe
CN102305675A (en) * 2011-05-25 2012-01-04 中国华能集团清洁能源技术研究院有限公司 Indirect temperature measuring device in entrained flow gasifying furnace

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7543983B2 (en) * 2005-12-30 2009-06-09 Hon Hai Precision Industry Co., Ltd. Device for measuring temperature of heat pipe
CN102305675A (en) * 2011-05-25 2012-01-04 中国华能集团清洁能源技术研究院有限公司 Indirect temperature measuring device in entrained flow gasifying furnace

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