JPH0569454B2 - - Google Patents
Info
- Publication number
- JPH0569454B2 JPH0569454B2 JP63189919A JP18991988A JPH0569454B2 JP H0569454 B2 JPH0569454 B2 JP H0569454B2 JP 63189919 A JP63189919 A JP 63189919A JP 18991988 A JP18991988 A JP 18991988A JP H0569454 B2 JPH0569454 B2 JP H0569454B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- molten steel
- molten metal
- hollow tube
- tip
- 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
Landscapes
- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、溶融金属、たとえばタンデイツシユ
内の溶鋼の連続測温方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method for continuous temperature measurement of molten metal, such as molten steel in a tundish.
連続鋳造設備のタンデイツシユ内における溶鋼
温度は、鋳造中、種々の外乱により変動する。一
般に取鍋より一定量の溶鋼をタンデイツシユへ注
入し、タンデイツシユより数基のモールドへと分
配注入され、急冷凝固が完了する連続鋳造プロセ
スにおいて、タンデイツシユは中間プラントに位
置する。そもそもタンデイツシユの主な役割は、
溶鋼の一時的な保持としての役割、介在物を
浮上分離させる役割、複数モールドへの分配の
役割を受けもつ。いずれにおいても温度条件が支
配的なプロセスであり、効率的な操業を確保する
ためには、もとよりタンデイツシユ内溶鋼温度を
把握することが重要である。タンデイツシユ内の
溶鋼温度は鋳造初期に炉壁レンガまたは溶鋼表面
からの抜熱が大きく、さらに連続プロセスの中間
に位置するゆえ、取鍋からの注入溶鋼量とモール
ドへの吐出溶鋼量のアンバランスにより、溶鋼容
量変動が激しく、温度変動が大きくなる。また、
鋳造末期へと、加熱、冷却等の手を加えない場
合、徐々に温度降下するが、使用タンデイツシユ
の鋳造回数や、鋳造前の予熱バラツキにより、そ
の温度下降速度が異なる。タンデイツシユ内溶鋼
温度が低下すると、介在物浮上効果が減少すると
ともに、鋳造ノズル詰りが発生するため、タンデ
イツシユ内溶鋼温度を正確に把握することはきわ
めて重要である。
The temperature of molten steel in the tundish of continuous casting equipment fluctuates due to various disturbances during casting. Generally, in a continuous casting process, a certain amount of molten steel is injected from a ladle into a tundish, and distributed from the tundish into several molds to complete rapid solidification, and the tundish is located in an intermediate plant. In the first place, the main role of tandaitsuyu is to
It plays the role of temporarily holding molten steel, floating and separating inclusions, and distributing it to multiple molds. In either case, temperature conditions are the dominant process, and in order to ensure efficient operation, it is important to understand the molten steel temperature in the tundish. The temperature of the molten steel in the tandate is affected by the large amount of heat removed from the furnace wall bricks or the surface of the molten steel in the early stages of casting, and since it is located in the middle of a continuous process, there is an imbalance between the amount of molten steel injected from the ladle and the amount of molten steel discharged into the mold. , the molten steel capacity fluctuates sharply, and the temperature fluctuates widely. Also,
Towards the end of casting, if no heating, cooling, or other steps are taken, the temperature will gradually drop, but the rate of temperature drop will vary depending on the number of castings of the tundish used and variations in preheating before casting. When the temperature of molten steel in the tundish decreases, the effect of floating inclusions decreases and clogging of the casting nozzle occurs, so it is extremely important to accurately grasp the molten steel temperature in the tundish.
以上のような問題を解決するために最近では、
特開昭61−249655号公報に開示されているタンデ
イツシユ内溶鋼加熱装置の採用が試みられてい
る。これは、溶鋼温度を測定した結果を誘導加熱
装置の電力制御部へフイードバツクし、鋳造初期
から末期の間、温度低下を補償するというもので
ある。 In order to solve the above problems, recently,
Attempts have been made to employ a device for heating molten steel in a tundish, which is disclosed in Japanese Unexamined Patent Publication No. 61-249655. This system feeds back the results of measuring the molten steel temperature to the power control section of the induction heating device to compensate for the temperature drop from the initial stage to the final stage of casting.
ところで、この種の溶鋼温度測定方法として現
在最も広く使用されているのは、消耗型浸漬熱電
対を使用するものである。しかし、これは、不連
続な測温であるため、約3分間隔以下のピツチで
は計測不可能となり、その結果、鋳造初期にみら
れる数十秒周期で約±10℃変動する溶鋼温度の制
御には到底使用できない。また、消耗型浸漬熱電
対のランニングコストに鑑みればその都度の測温
は到底実現不可能である。そこで、ランニングコ
スト低減を考慮した方法として、市販品として、
溶融金属に対し耐熱性の高い保護管(ジルコニア
系セラミツクスやアルミナカーボン質等)の内側
に、白金−白金ロジウム熱電対を挿入したプロー
ブがある。しかし、これは熱電対のコストが若干
高く、かつ約10時間程の寿命は確保されていると
いえども、熱電対は、保護管自身より発生する
COガスにより、浸炭等の影響を受け、経時再現
性が劣化し、最悪断線する事態を招くことがある
などの問題が残されている。 By the way, the currently most widely used method for measuring the temperature of molten steel of this type uses a consumable immersion thermocouple. However, since this is a discontinuous temperature measurement, it is impossible to measure the temperature at intervals of about 3 minutes or less, and as a result, it is difficult to control the temperature of molten steel, which fluctuates by about ±10 degrees Celsius every few tens of seconds, as seen in the early stages of casting. It cannot be used at all. Furthermore, in view of the running costs of consumable immersion thermocouples, it is completely impossible to measure temperature each time. Therefore, as a method to reduce running costs, as a commercially available product,
There is a probe in which a platinum-platinum rhodium thermocouple is inserted inside a protective tube (made of zirconia ceramics, alumina carbon, etc.) that is highly heat resistant to molten metal. However, this is due to the slightly higher cost of the thermocouple, and although the lifespan of about 10 hours is ensured, the thermocouple generates heat from the protective tube itself.
Problems remain, including carburization and other effects caused by CO gas, which deteriorates reproducibility over time and, in the worst case, can lead to wire breakage.
こうした測温現状下にあつて、最も要望視され
ているものは、光学式測温方法である。この例と
しては、特開昭56−60323号、同60−105929号各
公報記載の技術を挙げることができ、耐熱性の導
伝管を溶鋼内に挿入し、不活性ガスを供給するこ
とにより、導伝管先端部が開孔されているゆえ、
溶鋼面が露出し、その表面から得られる放射エネ
ルギーを放射温度計によりサンプリングし、温度
検出する方法である。この方法であれば、保護管
の形状がシンプルかつ必要最小限の損耗ダメージ
しかうけない。さらに、センサ自身のランニング
コストが測温センサ中、最も有利なものであるた
め、今後、光学式測温方法が鉄鋼業界では主流に
なると考えられる。 Under the current state of temperature measurement, the most desired method is an optical temperature measurement method. Examples of this include the techniques described in Japanese Patent Application Laid-open Nos. 56-60323 and 60-105929, in which a heat-resistant conduction pipe is inserted into molten steel and an inert gas is supplied. , since the tip of the conduit is perforated,
In this method, the molten steel surface is exposed and the radiant energy obtained from the surface is sampled using a radiation thermometer to detect the temperature. With this method, the protection tube has a simple shape and suffers only minimal wear and tear damage. Furthermore, since the running cost of the sensor itself is the most advantageous among temperature measurement sensors, it is thought that optical temperature measurement methods will become mainstream in the steel industry in the future.
しかし、周知の通り、不活性ガスを吹き込む
と、導伝管の開孔に臨む溶鋼表面は急冷される。
実際、溶鋼表面にArガスを吹き付けた場合、約
7℃〜10℃の温度低下が発生するとの知見も報告
されている。この場合、不活性ガスの流量調整如
何では、真値とのベースダウンの補正は困難と想
定される。 However, as is well known, when an inert gas is blown into the molten steel, the surface of the molten steel facing the opening of the conduction pipe is rapidly cooled.
In fact, it has been reported that when Ar gas is sprayed onto the surface of molten steel, the temperature decreases by approximately 7°C to 10°C. In this case, it is assumed that it is difficult to correct the base down from the true value depending on how the flow rate of the inert gas is adjusted.
タンデイツシユでの溶鋼温度の最適管理には、
溶鋼凝固温度との差がきわめて少ないことが要求
されており、これは前工程の温度ベースを低下さ
せることによる省エネルギー効果のためである。
過去には、前記温度差(ΔTという)が、ΔT=
30〜40℃であつたが、最近はΔT=10〜20℃を目
標に操業改善およびプラント改善が実施されてい
る。したがつて前記ΔTの目標を達成でき、かつ
低ランニングコストであり、消耗型浸漬熱電対の
現状再現性(σ=2℃)に対して遜色なく再現性
がσ=5℃以下の連続的光学式測温方法の開発が
要請されている。 For optimal control of molten steel temperature in tandem production,
It is required that the difference from the solidification temperature of molten steel be extremely small, and this is to save energy by lowering the temperature base of the previous process.
In the past, the temperature difference (referred to as ΔT) was ΔT=
The temperature was 30-40°C, but recently, operational improvements and plant improvements have been carried out with the goal of achieving ΔT = 10-20°C. Therefore, it is possible to achieve the above-mentioned ΔT target, has low running costs, and is comparable to the current reproducibility of consumable immersion thermocouples (σ = 2°C), and is a continuous optical system with a reproducibility of σ = 5°C or less. There is a need to develop a method for temperature measurement.
そこで、本発明の主たる目的は、ランニングコ
ストが低く、しかも測温に際して精度の高い連続
測温が可能な測温方法と装置を提供することにあ
る。 SUMMARY OF THE INVENTION Accordingly, the main object of the present invention is to provide a temperature measurement method and apparatus that have low running costs and are capable of continuous temperature measurement with high accuracy.
上記課題を解決するための本発明法は、先端が
開放された浸漬中空管の基部側にその先端を睨み
その先端の放射エネルギーに基いて測温する光学
式測温計を設け、前記中空管を溶融金属内に浸漬
するとともに、前記中空管内に所定流量で不活性
ガスを吹込み開放先端から吐出させ溶融金属中に
バブリングさせながら、溶融金属からの放射エネ
ルギーを光学式測温計で検出し、溶融金属との界
面の波動周期内における前記放射エネルギーの最
大値の平均値を溶融金属の測温値とすることを特
徴とするものである。
The method of the present invention for solving the above problems is to provide an optical thermometer on the base side of a submerged hollow tube with an open tip and measure the temperature based on the radiant energy of the tip. While the hollow tube is immersed in the molten metal, an inert gas is blown into the hollow tube at a predetermined flow rate and discharged from the open tip to bubble into the molten metal, while measuring the radiant energy from the molten metal using an optical thermometer. The method is characterized in that the average value of the maximum value of the radiant energy within the wave period of the interface with the molten metal is taken as the measured temperature value of the molten metal.
本発明では、消耗型浸漬熱電対とは異なり、連
続的に測温するものであるから、溶融金属の経時
的温度変化を把えることができ、これに基いて溶
融金属の温度制御する際における有効な手段とな
る。
Unlike a consumable immersion thermocouple, the present invention measures temperature continuously, so it is possible to grasp the temperature change of the molten metal over time, and based on this, when controlling the temperature of the molten metal. It is an effective method.
また、本発明では、先端開放の中空管に不活性
ガスを所定流量で吹込み、先端から吐出させ溶融
金属にバブリングする。このバブリングを行うの
は、バブリングによる溶融金属の攪拌を行わない
と、溶融金属の静圧つり合い表面が常に不活性ガ
スにさらされるため表面温度が低下し、真の溶鋼
温度を検出することができなくなるためである。 Further, in the present invention, an inert gas is blown into a hollow tube with an open tip at a predetermined flow rate, and is discharged from the tip to bubble into the molten metal. This bubbling is performed because if the molten metal is not stirred by bubbling, the static pressure balancing surface of the molten metal will be constantly exposed to inert gas, which will lower the surface temperature and make it impossible to detect the true molten steel temperature. This is because it disappears.
この意味でバブリングを行うことが有効である
が、その反面、バブリングに伴つて静圧のつり合
い溶融金属表面が定期的に凹凸波動を示し、凹時
と凸時における溶融金属表面からの放射エネルギ
ーのベクトルが放射温度計に対して平行に入射さ
れなくなり、その結果、見掛け上の放射率が経時
的に変動するため、温度測定誤差を生じる。 In this sense, bubbling is effective, but on the other hand, as a result of bubbling, the molten metal surface periodically exhibits uneven waves due to static pressure balance, and the radiant energy from the molten metal surface during concavity and convexity increases. The vector is no longer incident parallel to the radiation thermometer, resulting in temperature measurement errors because the apparent emissivity varies over time.
そこで、本発明に従つて、溶融金属表面の波動
周期以下のサンプリング周期をもつて温度検出
し、放射エネルギーの最大値を平均化し、これに
基いて温度値とすると、溶融金属の擬似平滑面の
温度と常に相異ない精度の高い測温ができる。 Therefore, according to the present invention, the temperature is detected with a sampling period equal to or less than the wave period of the molten metal surface, the maximum value of the radiant energy is averaged, and the temperature value is determined based on this. Highly accurate temperature measurement that is always consistent with temperature.
さらに、消耗型浸漬熱電対による1回限りのも
のとは異なり、連続かつ繰り返し使用が可能であ
るからランニングコストが著しく低減する。 Furthermore, unlike the one-time use of consumable immersion thermocouples, it can be used continuously and repeatedly, significantly reducing running costs.
以下本発明をさらに詳説する。 The present invention will be explained in more detail below.
第1図は第1の実施態様を示したもので、たと
えばタンデイツシユ内の溶鋼Mの温度を測定する
ために、その蓋の測温孔にマンホール蓋1が設け
られ、これに次述する測温装置が固定されてい
る。 FIG. 1 shows a first embodiment. For example, in order to measure the temperature of molten steel M in a tundish, a manhole cover 1 is provided in the temperature measurement hole of the lid, and the temperature measurement method described below is installed on the manhole cover 1. The device is fixed.
すなわち、マンホール蓋1には、フランジ付の
筒状支持金物2がボルト固定され、そのフランジ
にガス吹込ユニツト3、エアAiによる空冷ジヤ
ケツト4および保護キヤツプ5が順に固定されて
いる。空冷ジヤケツト4内には放射温度計6が設
けられ、その信号は導路7およびAD変換器8を
介して演算器10に取り込まれ、そこで後述の演
算処理に従う温度結果は温度表示器11に表示さ
れるようになつている。また、放射温度計6の前
面にはシーリングウインド16が配されている。 That is, a flanged cylindrical support metal fitting 2 is bolted to the manhole cover 1, and a gas blowing unit 3, an air cooling jacket 4 using air Ai, and a protective cap 5 are fixed in this order to the flange. A radiation thermometer 6 is provided in the air-cooled jacket 4, and its signal is taken into the arithmetic unit 10 via a conduit 7 and an AD converter 8, where the temperature result according to the arithmetic processing described later is displayed on a temperature display 11. It is becoming more and more common. Further, a ceiling window 16 is arranged in front of the radiation thermometer 6.
他方、支持金物2には、浸漬中空管9が配さ
れ、この中空管9は2重合わせ構造になつてお
り、その外側に耐スラグ用保護管9A1、耐熱性
保護管9A2および耐熱性先端保護管9Bを有し、
内側にステンレス等の保護管骨材9C付の溶鋼保
護管9Dを有し、これらの管9A〜9Dは、たと
えばAl2O3−Cの材質とされ、金属製ソケツト1
1を介して支持金物2にAl2O3等からなるセラミ
ツクボルト12により取付けられている。 On the other hand, an immersion hollow tube 9 is disposed on the support hardware 2, and this hollow tube 9 has a double layered structure, with a slag-resistant protection tube 9A 1 , a heat-resistant protection tube 9A 2 , and It has a heat-resistant tip protection tube 9B,
It has a molten steel protection tube 9D with a protection tube aggregate 9C made of stainless steel or the like inside, and these tubes 9A to 9D are made of, for example, Al 2 O 3 -C, and have a metal socket 1.
1 to the supporting hardware 2 with ceramic bolts 12 made of Al 2 O 3 or the like.
また、前記ガス吹込ユニツト3には、Ar等の
不活性ガスを吹き込む導管13が設けられ、その
途中に定圧弁14および流量調整弁15が配され
ている。導管13の先端は、中空管9内に連通し
ている。 Further, the gas blowing unit 3 is provided with a conduit 13 through which an inert gas such as Ar is blown, and a constant pressure valve 14 and a flow rate regulating valve 15 are disposed in the middle of the conduit 13. The tip of the conduit 13 communicates with the inside of the hollow tube 9.
かかる装置においては、中空管9の先端部を溶
鋼M中に一部浸漬した後、アルゴンガス(Arガ
ス)を一定圧力および一定流量で中空管9内に送
給し、その先端からバブリングさせる。泡を符号
Bで示す。この状態で、放射温度計6により溶鋼
Mを睨み、そこからの放射エネルギーをサンプリ
ングし、温度信号として取り出す。 In such a device, after the tip of the hollow tube 9 is partially immersed in the molten steel M, argon gas (Ar gas) is fed into the hollow tube 9 at a constant pressure and a constant flow rate, and bubbling occurs from the tip. let Bubbles are designated by the symbol B. In this state, the radiation thermometer 6 looks at the molten steel M, samples the radiant energy therefrom, and takes it out as a temperature signal.
この場合、バブリングに伴つて、第5図に示す
ように、溶鋼の静圧つり合い表面が凹凸波動を繰
り返す。本発明では、この波動周期以下の短いサ
ンプリング周期をもつて放射エネルギー変化を把
え、その最大値のみを抽出し、これを平均化処理
して、溶融金属の測温値とする。 In this case, as a result of bubbling, the static pressure balancing surface of the molten steel repeats uneven waves as shown in FIG. In the present invention, changes in radiant energy are grasped using a short sampling period equal to or less than this wave period, only the maximum value thereof is extracted, and this is averaged to be used as a temperature measurement value of the molten metal.
ところで、中空管9の材質としては、上記の例
のほか、Mo−ZrO2系のものなどをも使用できる
が、耐溶損性および耐ヒートシヨツク性の点で、
Al2O3−C系のものが最適である。しかるに、
この系では、溶鋼の熱によつて、主にCOガスを
発生する。このCOガスは、放射温度計に採用さ
れる波長帯域(500nm〜1500nm)においてその
波長を吸収する作用がある。そこで、これによる
精度低下を防止するために、そのCOガスを導管
13を介してのArガス吹出しによつてパージす
るようにと、COガスの影響を排除できる効果も
ある。 By the way, as the material for the hollow tube 9, in addition to the above-mentioned examples, Mo-ZrO 2 based materials can also be used, but in terms of erosion resistance and heat shock resistance, Al 2 O 3 -C based materials are preferred. is the best. However,
In this system, CO gas is mainly generated by the heat of molten steel. This CO gas has the effect of absorbing wavelengths in the wavelength band (500 nm to 1500 nm) used in radiation thermometers. Therefore, in order to prevent the accuracy from decreasing due to this, the CO gas is purged by blowing out Ar gas through the conduit 13, which has the effect of eliminating the influence of the CO gas.
ところで、光学式測温計としては、単色温度
計、多波長温度計等を用いることができる。さら
に、光フアイバーを用いて放射エネルギーのサン
プリングを行うこともできる。 By the way, as the optical thermometer, a monochromatic thermometer, a multi-wavelength thermometer, etc. can be used. Additionally, fiber optics can also be used to sample the radiant energy.
中空管の溶鋼M中への浸漬深さLは、その外径
をDとしたとき、L≧2Dが好ましい。より好ま
しくは、2D≦L≦3Dである。 The immersion depth L of the hollow tube into the molten steel M is preferably L≧2D, where D is the outer diameter of the hollow tube. More preferably, 2D≦L≦3D.
他方、上記の中空管は、ある時間使用したなら
ば、損耗があるので交換される。中空管がAl2O3
−C系のセラミツクであるときは、交換コスト的
に十分見合うけれども、Mo−ZrO2系の場合には
コスト高を招く。しかし、このコストの点を無視
すれば、Mo−ZrO2系のものを用いることができ
る。 On the other hand, the hollow tubes described above wear out and are replaced after a certain period of use. The hollow tube is Al 2 O 3
-C type ceramics are well worth the replacement cost, but Mo--ZrO 2 type ceramics result in higher costs. However, if this cost is ignored, a Mo-ZrO 2 based material can be used.
なお、本発明は、タンデイツシユ内のほか、高
炉樋、トーピード、取鍋、転炉、注銑鍋やモール
ド内等においても適用できる。 The present invention can be applied not only inside a tundish but also inside a blast furnace gutter, torpedo, ladle, converter, iron pouring ladle, mold, etc.
次に実施例を示す。 Next, examples will be shown.
第1図の測温装置により、タンデイツシユ内の
溶鋼の測温を1カ月にわたつて行つた。中空管は
Al2O3−C系のセラミツクとした。 The temperature of the molten steel in the tundish was measured over a period of one month using the temperature measuring device shown in FIG. hollow tube is
It was made of Al 2 O 3 -C ceramic.
測定条件は次の通りである。 The measurement conditions are as follows.
外側管9の浸漬長さLを500mm
〃 外径を60mmφ
〃 内径を20mmφ
アルゴンガス圧力:3Kg/cm2
〃 流量:3Kg/Hr
溶鋼温度:1510〜1570℃
この場合の溶鋼波動周期は0.3〜0.5secであつ
た。アルゴンガス吹込流量との関係を第4図に示
した。そこでサンプリング周期は、10ms以下で
設定した。これによるとA/D変換後のデータは
生データを十分再現できるレベルであつた。この
ときの関係を第5図に示す。第5図に示す様に、
バブリングによる溶鋼波動による温度変動が完全
に再現されていることが判る。 The immersion length L of the outer tube 9 is 500 mm. The outer diameter is 60 mm. The inner diameter is 20 mm. Argon gas pressure: 3 Kg/cm 2 Flow rate: 3 Kg/Hr. Molten steel temperature: 1510 to 1570°C. In this case, the molten steel wave period is 0.3 to 0.5. It was hot in sec. The relationship with the argon gas blowing flow rate is shown in Figure 4. Therefore, the sampling period was set to 10ms or less. According to this, the data after A/D conversion was at a level that could sufficiently reproduce the raw data. The relationship at this time is shown in FIG. As shown in Figure 5,
It can be seen that the temperature fluctuations caused by the molten steel waves caused by bubbling are perfectly reproduced.
その結果、測温装置の測定精度は、Δ=4℃を
みた。そして、測定精度がσ=2℃と高い消耗型
浸漬熱電対との対比を試みたところ、第2図のよ
うに、高い相関をみた。 As a result, the measurement accuracy of the temperature measuring device was found to be Δ=4°C. When we attempted to compare the results with a consumable immersion thermocouple, which has a high measurement accuracy of σ = 2°C, we found a high correlation as shown in Figure 2.
また、中空管の材質をMo−ZrO2系に代えて、
連結鋳造時における連続測温を試みたところ、第
3図のように、今まで把え難かつた鋳込初期およ
び末期の急激な温度変動をも把握できた。しか
も、寿命は約30時間と長時間であることも判つ
た。 In addition, the material of the hollow tube was changed to Mo-ZrO 2 system,
When we attempted continuous temperature measurement during continuous casting, we were able to detect rapid temperature fluctuations at the beginning and end of casting, which had been difficult to detect until now, as shown in Figure 3. Moreover, it was found that the lifespan was long, about 30 hours.
以上の通り、本発明によれば、測定精度として
実用的に十分に高いものとなり、ランニングコス
トの低減を図りつつ連続測温が可能となる。
As described above, according to the present invention, the measurement accuracy is sufficiently high for practical use, and continuous temperature measurement is possible while reducing running costs.
第1図は測温装置例の縦断面図、第2図は本発
明の測温値と浸漬熱電対による測定温度との対比
を示すグラフ、第3図は鋳込初期と末期の連続測
温結果を示すグラフ、第4図はAr流量と溶鋼波
動周期の関係図、第5図は溶鋼波動周期と溶鋼真
温度の関係図である。
6……放射温度計、9……中空管、10……演
算器、13……不活性吹込導管。
Fig. 1 is a longitudinal cross-sectional view of an example of a temperature measuring device, Fig. 2 is a graph showing a comparison between the temperature measurement value of the present invention and the temperature measured by an immersion thermocouple, and Fig. 3 is a continuous temperature measurement at the beginning and end of casting. Graphs showing the results, FIG. 4 is a relationship diagram between Ar flow rate and molten steel wave period, and FIG. 5 is a relationship diagram between molten steel wave period and molten steel true temperature. 6... Radiation thermometer, 9... Hollow tube, 10... Arithmetic unit, 13... Inert blowing conduit.
Claims (1)
の先端を睨みその先端の放射エネルギーに基づい
て測温する光学式測温計を設け、前記中空管を溶
融金属内に浸漬するとともに、前記中空管内に所
定流量で不活性ガスを吹込み開放先端から吐出さ
せ溶融金属中にバブリングさせながら、溶融金属
からの放射エネルギーを光学式測温計で検出し、
溶融金属との界面の波動周期内における前記放射
エネルギーの最大値の平均値を溶融金属の測温値
とすることを特徴とする溶融金属の連続測温方
法。1. An optical temperature meter is provided on the base side of the immersed hollow tube with the tip open, and the temperature is measured based on the radiant energy of the tip, and the hollow tube is immersed in the molten metal. , detecting the radiant energy from the molten metal with an optical thermometer while blowing an inert gas into the hollow tube at a predetermined flow rate and discharging it from the open tip to bubble into the molten metal;
1. A method for continuous temperature measurement of molten metal, characterized in that the average value of the maximum values of the radiant energy within the wave period of the interface with the molten metal is taken as the temperature measurement value of the molten metal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63189919A JPH0238932A (en) | 1988-07-29 | 1988-07-29 | Continuous temperature measuring method for molten metal |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63189919A JPH0238932A (en) | 1988-07-29 | 1988-07-29 | Continuous temperature measuring method for molten metal |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0238932A JPH0238932A (en) | 1990-02-08 |
| JPH0569454B2 true JPH0569454B2 (en) | 1993-10-01 |
Family
ID=16249407
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63189919A Granted JPH0238932A (en) | 1988-07-29 | 1988-07-29 | Continuous temperature measuring method for molten metal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0238932A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5180228A (en) * | 1989-09-18 | 1993-01-19 | Asahi Glass Company Ltd. | Radiation thermometer for molten iron and method for measuring the temperature of molten iron |
| AU2015205700B2 (en) * | 2014-01-08 | 2017-07-06 | Vesuvius Group, Sa | Optical pyrometer |
| CN109211412A (en) * | 2017-06-30 | 2019-01-15 | 沈阳泰合蔚蓝科技股份有限公司 | Temperature measuring device and temperature measuring method for measuring temperature of molten metal |
| EP3640614A4 (en) | 2017-06-30 | 2021-03-31 | Shenyang Taco Blue-tech Co., Ltd. | Temperature measurement device and temperature measurement method for measuring temperature of molten metal |
-
1988
- 1988-07-29 JP JP63189919A patent/JPH0238932A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0238932A (en) | 1990-02-08 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| KR0134654B1 (en) | Apparatus and method for measuring a temperature using optical fiber | |
| US7690841B2 (en) | Device for continuous temperature measurement of molten steel in the tundish using optical fiber and infra-red pyrometer | |
| EP0805964B1 (en) | A sampling device for thermal analysis | |
| US6176295B1 (en) | Plate mold for producing steel billets | |
| US6471397B2 (en) | Casting using pyrometer apparatus and method | |
| JPH01267426A (en) | Temperature measuring device for molten metal | |
| JPH0394129A (en) | Apparatus for continuously measuring temperature of molten metal | |
| JPH0569454B2 (en) | ||
| US5981917A (en) | Ladle preheat indication system | |
| CN1936524A (en) | Pouring-basket plug-rod with continuous temperature measuring function | |
| WO2008043152A1 (en) | Casting steel strip | |
| JP3351120B2 (en) | Measuring method of hot metal temperature at taphole with optical fiber thermometer | |
| JPH0259629A (en) | Continuous temperature measuring instrument for molten metal | |
| JPS6191529A (en) | Temperature measuring apparatus for molten metal | |
| JPS6030565A (en) | Method for stabilizing surface shape of ingot with heated casting mold type continuous casting method | |
| JPH07190749A (en) | Residual thickness detecting structure of refractory for gas blowing-in | |
| JP3214234B2 (en) | Temperature measuring device for high temperature liquid using optical fiber | |
| KR920000415A (en) | Production process of directional solidified casting | |
| JPH0815040A (en) | Optical fiber temperature measuring device for high temperature liquids | |
| SU1320010A1 (en) | Method and apparatus for automatic control of operation of mould of continuous casting machine | |
| JPS6117919A (en) | Temperature measuring instrument of molten metal | |
| JPS60105929A (en) | Method for measuring temperature of molten metal | |
| JP2822875B2 (en) | Molten metal temperature measuring device | |
| JPH0557426A (en) | Ladle for casting | |
| JP3116728B2 (en) | High temperature liquid temperature measuring device using optical fiber |