JPH0473092B2 - - Google Patents
Info
- Publication number
- JPH0473092B2 JPH0473092B2 JP58034363A JP3436383A JPH0473092B2 JP H0473092 B2 JPH0473092 B2 JP H0473092B2 JP 58034363 A JP58034363 A JP 58034363A JP 3436383 A JP3436383 A JP 3436383A JP H0473092 B2 JPH0473092 B2 JP H0473092B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- steel pipe
- furnace
- radiation thermometer
- temperature measurement
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/02—Constructional details
- G01J5/07—Arrangements for adjusting the solid angle of collected radiation, e.g. adjusting or orienting field of view, tracking position or encoding angular position
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/0044—Furnaces, ovens, kilns
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/02—Constructional details
- G01J5/0275—Control or determination of height or distance or angle information for sensors or receivers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/48—Thermography; Techniques using wholly visual means
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】
本発明は、炉内にある管状物体の温度測定方法
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring the temperature of a tubular object in a furnace.
加熱炉または熱処理炉などの炉内にある管状物
体たとえば鋼管の温度を非接触で測定するのに放
射温度計が用いられるが、この放射温度計を用い
る従来の測定方法は第1図に示す如く、炉2内の
鋼管1の内外表面を炉壁に設けた透過窓3を通し
て放射温度計4で覗き、該放射温度計4の視野に
入る鋼管の表面からの放射エネルギーを検出する
というものである。該放射温度計4には測定位置
を変えることのできる走査型のものが使用されて
いる。一方、炉2内を管軸方向と直角方向に搬送
される鋼管1は該鋼管1の長さによつて、炉内搬
送が問題なく行われるようにするため、炉幅方向
の適正な位置に載置されるように炉内に装入され
る。すなわち、該鋼管1の端部と炉側壁内面との
距離は鋼管1の長さによつて変わるので、該鋼管
上の測温点(図中5で示す)の位置(管端からの
距離)が鋼管の長さによつて変わることになる。
また、該鋼管1の外径または内径が変わると内表
面と外表面の測定境界点(図中7で示す)が変わ
つてくる。従つて、このような測温方法では測定
温度と測定位置との対応がとれず、また鋼管の内
表面と外表面の測定区分もできないという問題を
有している。 A radiation thermometer is used to non-contactly measure the temperature of a tubular object, such as a steel pipe, inside a heating furnace or heat treatment furnace.The conventional measurement method using this radiation thermometer is as shown in Figure 1. A radiation thermometer 4 looks through the inner and outer surfaces of the steel pipe 1 in the furnace 2 through a transmission window 3 provided on the furnace wall, and detects the radiant energy from the surface of the steel pipe that falls within the field of view of the radiation thermometer 4. . The radiation thermometer 4 is of a scanning type whose measurement position can be changed. On the other hand, the steel pipe 1 that is transported inside the furnace 2 in a direction perpendicular to the tube axis direction is placed at an appropriate position in the furnace width direction depending on the length of the steel pipe 1 so that the steel pipe 1 can be transported within the furnace without any problems. It is loaded into the furnace so that it is placed on the ground. That is, since the distance between the end of the steel pipe 1 and the inner surface of the furnace side wall varies depending on the length of the steel pipe 1, the position (distance from the pipe end) of the temperature measurement point (indicated by 5 in the figure) on the steel pipe will vary depending on the length of the steel pipe.
Further, when the outer diameter or inner diameter of the steel pipe 1 changes, the measurement boundary point (indicated by 7 in the figure) between the inner surface and the outer surface changes. Therefore, such a temperature measuring method has the problem that the measured temperature cannot correspond to the measured position, and it is also impossible to distinguish between the inner surface and the outer surface of the steel pipe.
鋼の焼入れ、焼戻しなどの熱処理においては、
熱処理過程の被処理材の温度履歴ならびに均熱温
度が機械的強度などの品質に大きく影響すること
は周知のことであり、鋼管の熱処理においても鋼
管の長さ方向および内外表面ともに所要温度範囲
内に加熱均熱、すなわち均一熱処理を行つてバラ
ツキの少ない均一な品質を得ることが重量であ
る。しかし、前述の従来の測温方法によつては、
管軸方向の位置に対応した温度分布および内外表
面温度差が把握できないため、加熱均熱時間のコ
ントロール、鋼管の長さ方向の温度分布コントロ
ールなどの均一熱処理のための必要操作が迅速か
つ的確にできなかつた。 In heat treatment such as hardening and tempering of steel,
It is well known that the temperature history of the material to be treated and the soaking temperature during the heat treatment process greatly affect quality such as mechanical strength, and during heat treatment of steel pipes, both the longitudinal direction and the inner and outer surfaces of the steel pipe are kept within the required temperature range. It is important to carry out heating and soaking, that is, uniform heat treatment, to obtain uniform quality with little variation. However, with the conventional temperature measurement method mentioned above,
Since the temperature distribution corresponding to the position in the tube axis direction and the temperature difference between the inner and outer surfaces cannot be determined, the necessary operations for uniform heat treatment such as controlling the heating soaking time and controlling the temperature distribution in the length direction of the steel tube can be performed quickly and accurately. I couldn't do it.
本発明は、かかる問題点を解決するための測温
方法を提供するものであり、その要旨は、炉壁に
設けた窓を通して、炉内の管状物体の一端側の内
表面または内外表面を覗く位置に設置した放射温
度計により、前記管状物体の一端側の温度を走査
測定し、該測定時の管状物体の寸法と放射温度計
の設置条件を表わす値とを用いて算出される管状
物体上の測温位置と放射温度計の走査角度との対
応関係にもとづいて測温位置に対応した測温情報
を得ることを特徴とする管状物体の温度測定方法
である。 The present invention provides a temperature measurement method to solve such problems, and its gist is to look through a window provided in the furnace wall into the inner surface or inner and outer surfaces of one end side of a tubular object in the furnace. The temperature on one end of the tubular object is scanned and measured by a radiation thermometer installed at a position on the tubular object, and the temperature is calculated using the dimensions of the tubular object at the time of the measurement and a value representing the installation conditions of the radiation thermometer. This method of measuring the temperature of a tubular object is characterized in that temperature measurement information corresponding to the temperature measurement position is obtained based on the correspondence between the temperature measurement position and the scanning angle of the radiation thermometer.
以下本発明を図示の実施例にもとづき詳しく説
明する。 The present invention will be explained in detail below based on the illustrated embodiments.
第2図aは本発明の実施例における装置構成を
示す図、図において4は放射温度計で、計測視野
角度範囲θを走査して、該角度θに対応する炉2
内の鋼管1内外表面の範囲の温度測定が可能であ
る。11は放射温度計4の検出信号から温度信号
に変換する温度測定信号回路、12は放射温度計
4内の走査回路からの信号にもとづき放射温度計
4の時時刻刻の走査角度±θa(図示のαなる角度
に相当する走査角度を零とする)を求める走査角
度信号回路である。13は設定器で、炉2内の鋼
管1の測温側の端部6と炉側壁内面との距離L1
(鋼管1の長さによつて決まる)、鋼管1の外径D
および肉厚tも設定入力するものである。 FIG. 2a is a diagram showing the configuration of an apparatus in an embodiment of the present invention. In the figure, 4 is a radiation thermometer that scans the measurement field of view angle range θ, and measures the furnace 2 corresponding to the angle θ.
It is possible to measure the temperature of the inner and outer surfaces of the steel pipe 1 inside. 11 is a temperature measurement signal circuit that converts the detection signal of the radiation thermometer 4 into a temperature signal, and 12 is a temperature measurement signal circuit that converts the detection signal of the radiation thermometer 4 into a temperature signal. This is a scanning angle signal circuit that calculates the scanning angle corresponding to the angle α of . Reference numeral 13 denotes a setting device that determines the distance L 1 between the temperature measuring side end 6 of the steel pipe 1 in the furnace 2 and the inner surface of the furnace side wall.
(Determined by the length of steel pipe 1), outer diameter D of steel pipe 1
and the wall thickness t are also input.
また、14も設定器であり、放射温度計4の設
置条件であるH(鋼管1に対する相対高さ)、L2
(炉側壁内面からの水平距離)、α(基準傾角)お
よびL0max(放射温度計4の設置条件から制約さ
れる鋼管外表面測温可能な距離)を設定入力する
ものである。 In addition, 14 is a setting device, which is the installation condition of the radiation thermometer 4, H (relative height to the steel pipe 1), L 2
(horizontal distance from the inner surface of the furnace side wall), α (reference inclination angle), and L 0 max (distance at which the temperature can be measured on the outer surface of the steel pipe, which is restricted by the installation conditions of the radiation thermometer 4) are input.
15は演算回路であり、前記設定器13および
14からの設定値L1,D,H,L2,α,L0max
を用いて、第2図bに示す鋼管1の内表面測温の
ための走査角度範囲(±θi)と外表面測温のため
の走査角度範囲(+θ0)とを基準傾角αを基準に
して下式
(−θi)=tan-1{(H−t)/(L1+L2)}−α
……(1)
(+θi)=α−tan-1{(H−D+t)/(L1+L2)}
……(2)
(+θ0)=(α−θi)−tan-1{(H−D)/(L0max
+L1+L2)} ……(3)
によつて算出し、走査角度信号回路12からの角
度信号(±θa)が前記角度範囲(±θi)または
(+θ0)の範囲であるとき対応した判別信号を出
力する内外面測温判別回路である。 15 is an arithmetic circuit, and the set values L 1 , D, H, L 2 , α, L 0 max from the setting devices 13 and 14 are
Using the scanning angle range (±θi) for temperature measurement on the inner surface of the steel pipe 1 and the scanning angle range (+θ 0 ) for temperature measurement on the outer surface of the steel pipe 1 shown in FIG. The following formula (-θi) = tan -1 {(H-t)/(L 1 +L 2 )}-α
...(1) (+θi) = α−tan -1 {(H−D+t)/(L 1 +L 2 )}
……(2) (+θ 0 )=(α−θi)−tan −1 {(H−D)/(L 0 max
+L 1 +L 2 )} ...(3), and when the angle signal (±θa) from the scanning angle signal circuit 12 is within the angle range (±θi) or (+θ 0 ), the corresponding This is an internal/external temperature determination circuit that outputs a determination signal.
16は温度測定信号回路11からの温度信号
を、内外面測温判別回路15からの内表面測温ま
たは外表面測温の判別信号にもとづいて、内表面
温度信号と外表面温度信号とに区分する温度信号
区分回路である。また、17も演算回路であり、
鋼管1の内表面上および外表面上の各測定位置を
鋼管端部6または7からの距離として表わした場
合の該測温位置(第2図c中のLiおよびL0)に
対応する内表面走査角度範囲(θic)および外表面
走査角度(θpc)は演算回路15と同じ計算によ
り求められるもので、(θic)=(−θi)+(+θi)
およ
び(θpc)=(+θp)の関係があり、基準傾角度αを
零基準しているため、放射温度計の走査角度(+
θa)との対応を容易に採れるものである。 16 divides the temperature signal from the temperature measurement signal circuit 11 into an inner surface temperature signal and an outer surface temperature signal based on the discrimination signal of inner surface temperature measurement or outer surface temperature measurement from the inner and outer surface temperature measurement discrimination circuit 15. This is a temperature signal division circuit. In addition, 17 is also an arithmetic circuit,
The inner surface corresponding to the temperature measurement position (Li and L 0 in Fig. 2 c) when each measurement position on the inner surface and outer surface of the steel pipe 1 is expressed as a distance from the steel pipe end 6 or 7. The scanning angle range (θ ic ) and the outer surface scanning angle (θ pc ) are obtained by the same calculation as in the arithmetic circuit 15, and are (θ ic )=(−θ i )+(+θ i ).
and (θ pc ) = (+θ p ), and since the reference inclination angle α is set to zero, the scanning angle of the radiation thermometer (+
θ a ) can be easily matched.
図c中の基準傾角度αを基準にした内表面走査
角度−θicおよび+θicならびに外表面走査角度θpc
と内表面測温位置Liおよび外表面測温位置L0との
対応関係は、
走査角度−θicが(−θi)の範囲内においては(4)
式、
Li=f(−θic,L1,α,L2,H,D,t)
……(4)
走査角度+θicが(+θi)の範囲内においては(5)
式、
Li=f(±θic,L1,α,L2,H,D,t)
……(5)
走査角度θpcが(+θp)の範囲内においては(6)
式、
Lp=f(θpc,
(+θi),L1,α,L2,H,D,t) ……(6)
の関連式から求められる。(+θi),(−θi)および
(+θp)は演算回路15で算出された値を利用し
ている。式(4)、(5)、(6)中の−θic、+θic,θpcは
放射
温度計の走査角度(±θa)に前述の通り容易に置
き換えられ、走査角度(±θa)と測温位置(Liお
よびLp)との関係線図データをもつている。走査
角度信号回路12からの角度(±θa)を測温位置
信号に変換する測温位置信号回路である。 Inner surface scanning angles −θ ic and +θ ic and outer surface scanning angle θ pc based on reference inclination angle α in Figure c.
The correspondence relationship between the inner surface temperature measurement position L i and the outer surface temperature measurement position L 0 is (4) when the scanning angle −θ ic is within the range of (−θ i ).
Formula, L i = f (-θ ic , L 1 , α, L 2 , H, D, t)
...(4) When the scanning angle +θ ic is within the range of (+θ i ), (5)
Formula, L i = f (±θ ic , L 1 , α, L 2 , H, D, t)
...(5) When the scanning angle θ pc is within the range of (+θ p ), (6)
It is obtained from the related expression L p = f (θ pc , (+θ i ), L 1 , α, L 2 , H, D, t) (6). The values calculated by the arithmetic circuit 15 are used for (+θ i ), (−θ i ), and (+θ p ). −θ ic , +θ ic , θ pc in equations (4), (5), and (6) can be easily replaced with the scanning angle (±θ a ) of the radiation thermometer as described above, and the scanning angle (±θ a ) and temperature measurement positions (L i and L p ). This is a temperature measurement position signal circuit that converts the angle (±θ a ) from the scanning angle signal circuit 12 into a temperature measurement position signal.
18は温度測定信号回路11からの温度信号
を、測温位置信号回路17からの出力にもとづい
て、測温位置と測温値を対応づけて出力する温度
パターン測定回路である。さらに、19は温度信
号区分回路16からの内表面温度、外表面温度に
もとづいて、それぞれの最大値、平均値、最小値
を求め内表面と外表面の温度差の最大値、最小値
ならびに平均温度差を出力する温度差演算回路で
ある。 Reference numeral 18 denotes a temperature pattern measuring circuit that outputs a temperature signal from the temperature measuring signal circuit 11 based on the output from the temperature measuring position signal circuit 17 in association with a temperature measuring position and a measured temperature value. Furthermore, 19 calculates the maximum value, average value, and minimum value of each of the inner surface temperature and outer surface temperature from the temperature signal classification circuit 16, and calculates the maximum value, minimum value, and average value of the temperature difference between the inner surface and the outer surface. This is a temperature difference calculation circuit that outputs a temperature difference.
上記の構成により、炉2内への鋼管1の装入位
置が鋼管の長さによつて変つても、鋼管1の内表
面および外表面の各測温位置に対応した測温値が
検出でき、内外面の温度差や温度分布なども算出
することができる。こうして算出した温度情報に
もとづき、炉の操業条件を適確にコントロールす
ることができる。 With the above configuration, even if the charging position of the steel pipe 1 into the furnace 2 changes depending on the length of the steel pipe, temperature values corresponding to each temperature measurement position on the inner and outer surfaces of the steel pipe 1 can be detected. It is also possible to calculate the temperature difference and temperature distribution between the inner and outer surfaces. Based on the temperature information calculated in this way, the operating conditions of the furnace can be accurately controlled.
なお、上記実施例における放射温度計4は走査
機能を内蔵した型式のものであるが、温度計全体
の角度を調整する型式の放射温度計であつてもよ
いことはもちろんであり、また設定器13,14
から入力するL1,Dおよびtは他のプロセスコ
ンピユーターあるいはビジネスコンピユーターか
ら自動入力することもできる。 Although the radiation thermometer 4 in the above embodiment is of a type with a built-in scanning function, it is of course possible to use a type of radiation thermometer that adjusts the angle of the entire thermometer. 13,14
L 1 , D and t inputted from can also be automatically inputted from another process computer or business computer.
第1図は従来の測温方法を説明する図、第2図
は本発明の実施例における装置構成を示す図であ
る。
1:鋼管、2:炉、3:透過窓、4:放射温度
計、11:温度測定信号回路、12:走査角度信
号回路、13:設定器、14:設定器、15:内
外面測温判別回路、16:温度信号区分回路、1
7:測温位置信号回路、18:温度パターン測定
回路、19:温度差演算回路。
FIG. 1 is a diagram illustrating a conventional temperature measuring method, and FIG. 2 is a diagram illustrating an apparatus configuration in an embodiment of the present invention. 1: Steel pipe, 2: Furnace, 3: Transmission window, 4: Radiation thermometer, 11: Temperature measurement signal circuit, 12: Scanning angle signal circuit, 13: Setting device, 14: Setting device, 15: Inside and outside temperature measurement discrimination Circuit, 16: Temperature signal division circuit, 1
7: Temperature measurement position signal circuit, 18: Temperature pattern measurement circuit, 19: Temperature difference calculation circuit.
Claims (1)
一端側の内表面または内外表面を覗く位置に設置
した放射温度計により、前記管状物体の一端側の
温度を走査測定し、該測定時の管状物体の寸法と
放射温度計の設置条件を表わす値とを用いて算出
される管状物体上の測温位置と放射温度計の走査
角度との対応関係にもとづいて測温位置に対応し
た測温情報を得ることを特徴とする管状物体の温
度測定方法。1 Scanning and measuring the temperature at one end of the tubular object in the furnace using a radiation thermometer installed at a position that looks into the inner surface or inner and outer surfaces of one end of the tubular object in the furnace through a window provided in the furnace wall; The temperature measurement corresponding to the temperature measurement position is calculated based on the correspondence between the temperature measurement position on the tubular object and the scanning angle of the radiation thermometer, which is calculated using the dimensions of the tubular object and the value representing the installation conditions of the radiation thermometer. A method for measuring the temperature of a tubular object, characterized by obtaining temperature information.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58034363A JPS59160724A (en) | 1983-03-04 | 1983-03-04 | Method for measuring temperature of tubular object |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58034363A JPS59160724A (en) | 1983-03-04 | 1983-03-04 | Method for measuring temperature of tubular object |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59160724A JPS59160724A (en) | 1984-09-11 |
| JPH0473092B2 true JPH0473092B2 (en) | 1992-11-19 |
Family
ID=12412077
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58034363A Granted JPS59160724A (en) | 1983-03-04 | 1983-03-04 | Method for measuring temperature of tubular object |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59160724A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6680303B2 (en) * | 2017-02-24 | 2020-04-15 | Jfeスチール株式会社 | Apparent emissivity calculation method, temperature measurement method, pipe material manufacturing method, and temperature measurement device |
| JP6787419B2 (en) * | 2018-02-14 | 2020-11-18 | Jfeスチール株式会社 | Temperature measurement system, temperature measurement method and manufacturing method of pipe material |
-
1983
- 1983-03-04 JP JP58034363A patent/JPS59160724A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59160724A (en) | 1984-09-11 |
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