JPH0648214B2 - Method for measuring furnace wall temperature in coking furnace carbonization chamber - Google Patents
Method for measuring furnace wall temperature in coking furnace carbonization chamberInfo
- Publication number
- JPH0648214B2 JPH0648214B2 JP56200930A JP20093081A JPH0648214B2 JP H0648214 B2 JPH0648214 B2 JP H0648214B2 JP 56200930 A JP56200930 A JP 56200930A JP 20093081 A JP20093081 A JP 20093081A JP H0648214 B2 JPH0648214 B2 JP H0648214B2
- Authority
- JP
- Japan
- Prior art keywords
- furnace wall
- carbonization chamber
- temperature
- furnace
- wall temperature
- 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 - Lifetime
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
- G01J5/05—Means for preventing contamination of the components of the optical system; Means for preventing obstruction of the radiation path
-
- 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
- G01J5/04—Casings
- G01J5/041—Mountings in enclosures or in a particular environment
-
- 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
- G01J5/04—Casings
- G01J5/047—Mobile mounting; Scanning arrangements
-
- 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
- G01J5/04—Casings
- G01J5/048—Protective parts
-
- 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
- G01J5/06—Arrangements for eliminating effects of disturbing radiation; Arrangements for compensating changes in sensitivity
- G01J5/061—Arrangements for eliminating effects of disturbing radiation; Arrangements for compensating changes in sensitivity by controlling the temperature of the apparatus or parts thereof, e.g. using cooling means or thermostats
-
- 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
- G01J5/08—Optical arrangements
- G01J5/0818—Waveguides
-
- 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
- G01J5/08—Optical arrangements
- G01J5/0879—Optical elements not provided otherwise, e.g. optical manifolds, holograms, cubic beamsplitters, non-dispersive prisms or particular coatings
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】 この発明は、多数の炭化室を有するコークス炉の炉壁温
度の測定方法に関するものである。The present invention relates to a method for measuring a furnace wall temperature of a coke oven having a large number of carbonization chambers.
一般に、コークス炉はそれぞれ独立した炭化室と燃焼室
が交互に配設された炉団によつて形成されている。Generally, the coke oven is formed by a furnace group in which independent carbonization chambers and combustion chambers are alternately arranged.
一方、炭化室内に石炭が装入されてから焼成されるまで
の乾留時間は、例えば装入炭の水分や粒度などの外的条
件によつても影響されるが、大部分は燃焼室の温度によ
つて決定される。そのため、燃焼室の温度測定はコーク
ス製造条件の管理上重要な要件の一つである。On the other hand, the dry distillation time from the charging of coal into the carbonization chamber to the firing is also affected by external conditions such as the water content and particle size of the charging coal, but for the most part it is mostly the temperature of the combustion chamber. It is decided by. Therefore, measuring the temperature of the combustion chamber is one of the important requirements for controlling the coke production conditions.
燃焼室の温度は炭化室,炉幅の関係から押出機側が低
く、窯出し側へ向けてある温度勾配で増加し窯出し側で
最も高くなつている。この温度勾配は炭化室の押出機側
から窯出し側まで装入された石炭を同一時間にコークス
化するために適切な温度勾配でもつて操業管理している
が、燃焼ガス中に含まれるタール等によりバーナの閉塞
が起り、これによる燃焼ガス量のばらつきおよび炭化室
内での装入炭水分,嵩密度のばらつき等により温度勾配
に乱れを生じ、コークス化時間の変動による操業トラブ
ルの発生に加え、エネルギー面からも加熱ガスを多量に
消費する状態となるので、押出機側から窯出し側にかけ
ての適切な温度勾配と絶対に必要とする温度の確保はコ
ークス管理上重要なものである。The temperature of the combustion chamber is lower on the extruder side due to the carbonization chamber and furnace width, increases with a certain temperature gradient toward the kiln discharge side, and is highest on the kiln discharge side. This temperature gradient is controlled with an appropriate temperature gradient to coke the coal charged from the extruder side of the carbonization chamber to the kiln discharge side at the same time, but tar, etc. contained in the combustion gas As a result, burner blockage occurs, which causes fluctuations in the amount of combustion gas, fluctuations in the amount of charged coal in the carbonization chamber, fluctuations in the bulk density, and other factors that cause temperature gradients to fluctuate. Since a large amount of heating gas is consumed in terms of energy, it is important in coke management to secure an appropriate temperature gradient from the extruder side to the kiln discharge side and a temperature that is absolutely necessary.
従来、燃焼室の温度を測定するには光高温計により人為
的に行われている。この温度測定はできるだけ短時間で
行う必要があるにもかかわらず熟練者でも一個所の測定
にかなりの時間を要し、すべての燃焼室の測定を短時間
に行うことは容易でなく、また、人為的な誤差が大きい
等の欠点があつた。Conventionally, an optical pyrometer is used to measure the temperature of the combustion chamber artificially. Even though this temperature measurement needs to be performed in the shortest possible time, even an expert requires a considerable amount of time to measure one point, and it is not easy to measure all combustion chambers in a short time. There were drawbacks such as large artificial error.
光高温計を使用しない温度測定方法としては、燃焼室上
部空間に熱電対を設置して測定する方法や、燃焼室内の
隣り合つた燃焼室の中間の仕切壁上部あるいはヘアピン
上部の耐火物内部に熱電対を設置して測定する方法等が
ある。しかしながらこれらの測定方法のうち、前者の方
法は、種々複雑な伝熱機構に加え、ドラフトの乱れやガ
ス流速の乱れ等によつて測定値が脈動し、炉温を代表し
た値として把握するには問題がある。また、後者の方法
は、耐火物内部の温度を測定するために測定値が燃焼室
内部の温度変化に対し遅れを生ずる欠点があり、両測定
方法とも燃焼室内部の温度を正確に把握するための測定
方法としては満足できる方法ではなかつた。As a temperature measurement method that does not use an optical pyrometer, a thermocouple is installed in the upper space of the combustion chamber for measurement, or inside the refractory inside the partition wall or hairpin above the adjacent combustion chambers in the combustion chamber. There is a method of installing a thermocouple for measurement. However, of these measurement methods, the former method has various complicated heat transfer mechanisms, and measurement values pulsate due to turbulence in draft and gas velocity Has a problem. In addition, the latter method has a drawback that the measured value lags the temperature change inside the combustion chamber because the temperature inside the refractory is measured, and both measurement methods accurately grasp the temperature inside the combustion chamber. It was not a satisfactory method for measuring.
この発明は、上記の欠点を除去するためになされたもの
である。以下、この発明について説明する。The present invention has been made to eliminate the above drawbacks. The present invention will be described below.
第1図はこの発明の一実施例を示す平面図、第2図は第
1図の側面図である。これらの図において、1は移動可
能に設置された押出機で、焼成されたコークスを押し出
すラムビーム2が取り付けられている。3は炭化室、4
は前記炭化室3の炉壁、5は燃焼室、6はガイド車、7
はフード、8は消火車、9は前記ラムビーム2の先端部
2aに取り付けた石英ガラス等の耐熱性のプリズムで、
炉壁4からの輻射光を受光する受光手段となるものであ
る。10は前記プリズム9からの輻射光を受光して炉壁
4の温度に対応する電気信号として取り出すための温度
計で、ラムビーム2の後端部2bに設けられる。温度計
10としては単色温度計,2色温度計,放射温度計,赤
外線放射温度計等が用いられる。11は輻射光の通路と
なるダクト、12は前記プリズム9の受光面9aを清浄
にするためのエアパージ用パイプである。FIG. 1 is a plan view showing an embodiment of the present invention, and FIG. 2 is a side view of FIG. In these drawings, reference numeral 1 denotes an movably installed extruder, to which a ram beam 2 for extruding the baked coke is attached. 3 is a carbonization chamber, 4
Is a furnace wall of the carbonization chamber 3, 5 is a combustion chamber, 6 is a guide wheel, 7
Is a hood, 8 is a fire engine, 9 is a heat-resistant prism such as quartz glass attached to the tip 2a of the ram beam 2,
It serves as a light receiving means for receiving the radiant light from the furnace wall 4. A thermometer 10 is provided at the rear end 2b of the ram beam 2 for receiving the radiant light from the prism 9 and extracting it as an electric signal corresponding to the temperature of the furnace wall 4. As the thermometer 10, a monochromatic thermometer, a two-color thermometer, a radiation thermometer, an infrared radiation thermometer, or the like is used. Reference numeral 11 is a duct that serves as a passage for radiated light, and 12 is an air purging pipe for cleaning the light receiving surface 9a of the prism 9.
次に、動作について説明する。Next, the operation will be described.
測定すべき炭化室3の位置に押出機1を停止させ、ラム
ビーム2を炭化室3内に挿入して焼成したコークスを押
し出しながら測定する。そして炉壁4から放散された輻
射光はプリズム9の受光面9aで受光され、反射面9b
で直角方向に反射し、ダクト11内を直進して温度計1
0に受光されることにより温度測定を行う。このように
して、ラムビーム2を順次移動させながら測定すべき次
の炭化室3内の炉壁4の温度を測定する。また、プリズ
ム9の受光面9aに炭化室3内の塵埃が付着するのを防
ぐためエアパージ用パイプ12からエアを噴出して清掃
し清浄な面を保つようにする。The extruder 1 is stopped at the position of the carbonization chamber 3 to be measured, the ram beam 2 is inserted into the carbonization chamber 3, and the calcined coke is pushed out for measurement. The radiant light radiated from the furnace wall 4 is received by the light receiving surface 9a of the prism 9 and is reflected by the reflecting surface 9b.
At a right angle, and go straight through the duct 11 to reach the thermometer 1
When the light is received at 0, the temperature is measured. In this way, the temperature of the furnace wall 4 in the next carbonization chamber 3 to be measured is measured while sequentially moving the ram beam 2. Further, in order to prevent dust in the carbonization chamber 3 from adhering to the light receiving surface 9a of the prism 9, air is jetted from the air purging pipe 12 to clean and maintain a clean surface.
なお、測定中の炭化室3内の塵埃、煙等の外乱の影響が
少ない場合、または2色温度計のように外乱に強い温度
計の場合はダクト11は必ずしも必要としない。It should be noted that the duct 11 is not always necessary when the influence of disturbance such as dust and smoke in the carbonization chamber 3 during measurement is small, or when the thermometer is strong against disturbance such as a two-color thermometer.
なお、プリズム9からの反射光は光フアイバ(図示せ
ず)を用いて温度計10へ導入することができる。光フ
アイバとしては素線1本の光フアイバ,フアイバロツト
および多数の光フアイバを束ねたバンドルフアイバ,イ
メージガイド等周知のものが用いられる。光フアイバを
用いる場合は、プリズム9の後面9cに光フアイバの一
方の端面を当接し、他方の端面を温度計10の受光面と
当接させるが、光フアイバの各端面とプリズム9及び温
度計10との間にそれぞれレンズを設けておくのが望ま
しい。これらの当接部は、外乱を避けるため両者をセラ
ミツクス系等の高温用接着剤で接着し、遮光材で覆つて
おくのが望ましい。耐熱性の低い光フアイバを用いる場
合は、光フアイバを保護管で覆い、この保護管と光フア
イバとの間隙に冷却用気体を導入する方法、あるいは光
フアイバを二重管で覆い、この二重管内に冷却用の気体
または液体を導入する方法で実施される。The reflected light from the prism 9 can be introduced into the thermometer 10 using an optical fiber (not shown). As the optical fiber, a well-known optical fiber such as an optical fiber having a single wire, a fiber rot, a bundle fiber in which a large number of optical fibers are bundled, an image guide, and the like are used. When an optical fiber is used, one end surface of the optical fiber is brought into contact with the rear surface 9c of the prism 9 and the other end surface is brought into contact with the light-receiving surface of the thermometer 10. However, each end surface of the optical fiber, the prism 9 and the thermometer. It is desirable to provide a lens between each of them. In order to avoid disturbance, it is desirable that these abutting portions are adhered to each other with a high temperature adhesive such as ceramics and covered with a light shielding material. When using an optical fiber with low heat resistance, cover the optical fiber with a protective tube and introduce a cooling gas into the gap between the protective tube and the optical fiber, or cover the optical fiber with a double tube and use this double tube. It is carried out by a method of introducing a cooling gas or liquid into the tube.
以上説明したようにこの発明は、押出機により炭化室内
に挿入されるラムビームの先端部にプリズムを設けて炉
壁からの輻射光を受光したのち、このプリズムにより反
射させ、次いで、前記プリズムからの反射光を前記ラム
ビームの後端部に設けた温度計で受光して炉壁面の温度
を直接測定できるようにしたことにより、炭化室内の正
確な温度を迅速に、かつ人為的な誤差を伴なわずに測定
できるので、炉壁面の温度分布をきわめて短時間に知る
ことができ、炉温管理の自動制御が可能になる。さら
に、炉温の均一化による作業能率の向上、熱量源単位の
低減および炉体の寿命延長等の効果もあり、コークス製
造条件の管理上きわめて有用である利点がある。As described above, the present invention provides a prism at the tip of a ram beam to be inserted into a carbonization chamber by an extruder, receives radiant light from a furnace wall, reflects the light from the furnace, and then reflects it from the prism. Since the temperature of the furnace wall surface can be directly measured by receiving the reflected light with the thermometer installed at the rear end of the ram beam, the accurate temperature inside the carbonization chamber can be measured quickly and with no error. Since it can be measured without measuring, the temperature distribution on the furnace wall surface can be known in an extremely short time, and the furnace temperature management can be automatically controlled. Further, there are effects such as improvement of work efficiency by homogenizing the furnace temperature, reduction of unit of heat source and extension of life of the furnace body, and there is an advantage that it is extremely useful for management of coke manufacturing conditions.
第1図はこの発明の一実施例を示す平面図、第2図は第
1図の側面図である。 図中、1は押出機、2はラムビーム、3は炭化室、4は
炉壁、5は燃焼室、6はガイド車、7はフード、8は消
火車、9はプリズム、10は温度計、11はダクト、1
2はエアパージ用パイプである。FIG. 1 is a plan view showing an embodiment of the present invention, and FIG. 2 is a side view of FIG. In the figure, 1 is an extruder, 2 is a ram beam, 3 is a carbonization chamber, 4 is a furnace wall, 5 is a combustion chamber, 6 is a guide wheel, 7 is a hood, 8 is a fire engine, 9 is a prism, 10 is a thermometer, 11 is a duct, 1
Reference numeral 2 is an air purging pipe.
Claims (1)
け、複数の炭化室内のコークスを順次前記ラムビームに
より押し出すようにしたコークス炉において、前記ラム
ビームの前部に設けたプリズムによつて前記炭化室の炉
壁からの輻射光を前記ラムビームの長手方向に反射し、
この反射された輻射光を前記ラムビームの後部に設けた
温度計で受光し炉壁温度を検出することを特徴とするコ
ーク炉炭化室の炉壁温度の測定方法。1. A coke oven in which an extruder equipped with a ram beam is movably provided so that cokes in a plurality of carbonization chambers are sequentially extruded by the ram beam, and the carbonization is performed by a prism provided in front of the ram beam. Radiant light from the furnace wall of the chamber is reflected in the longitudinal direction of the ram beam,
A method for measuring a furnace wall temperature in a coke oven carbonization chamber, characterized in that the reflected radiant light is received by a thermometer provided at the rear portion of the ram beam to detect the furnace wall temperature.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56200930A JPH0648214B2 (en) | 1981-12-15 | 1981-12-15 | Method for measuring furnace wall temperature in coking furnace carbonization chamber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56200930A JPH0648214B2 (en) | 1981-12-15 | 1981-12-15 | Method for measuring furnace wall temperature in coking furnace carbonization chamber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58102116A JPS58102116A (en) | 1983-06-17 |
| JPH0648214B2 true JPH0648214B2 (en) | 1994-06-22 |
Family
ID=16432643
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56200930A Expired - Lifetime JPH0648214B2 (en) | 1981-12-15 | 1981-12-15 | Method for measuring furnace wall temperature in coking furnace carbonization chamber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0648214B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2011515671A (en) * | 2008-03-20 | 2011-05-19 | シーメンス アクチエンゲゼルシヤフト | Optical measuring device and turbine |
-
1981
- 1981-12-15 JP JP56200930A patent/JPH0648214B2/en not_active Expired - Lifetime
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2011515671A (en) * | 2008-03-20 | 2011-05-19 | シーメンス アクチエンゲゼルシヤフト | Optical measuring device and turbine |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58102116A (en) | 1983-06-17 |
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