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JPS5832207B2 - Charge deposition layer thickness detection sonde - Google Patents
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JPS5832207B2 - Charge deposition layer thickness detection sonde - Google Patents

Charge deposition layer thickness detection sonde

Info

Publication number
JPS5832207B2
JPS5832207B2 JP5729276A JP5729276A JPS5832207B2 JP S5832207 B2 JPS5832207 B2 JP S5832207B2 JP 5729276 A JP5729276 A JP 5729276A JP 5729276 A JP5729276 A JP 5729276A JP S5832207 B2 JPS5832207 B2 JP S5832207B2
Authority
JP
Japan
Prior art keywords
furnace
sonde
gas
layer thickness
charge
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
Application number
JP5729276A
Other languages
Japanese (ja)
Other versions
JPS52141257A (en
Inventor
正 磯山
有治 金山
博義 寺田
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.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP5729276A priority Critical patent/JPS5832207B2/en
Publication of JPS52141257A publication Critical patent/JPS52141257A/en
Publication of JPS5832207B2 publication Critical patent/JPS5832207B2/en
Expired legal-status Critical Current

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  • Vertical, Hearth, Or Arc Furnaces (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Blast Furnaces (AREA)

Description

【発明の詳細な説明】 本発明は、高炉、シャフト炉などのように炉頂部よりコ
ークス、焼結鉱、ペレットおよび塊鉱石(以下鉱石類と
称す)を層状に装入している炉で、コークスと鉱石類推
積層の電気抵抗の差を利用することによって、装入物の
堆積層厚を測定する場合の検出ゾンデの構造に関するも
のである。
Detailed Description of the Invention The present invention relates to a furnace in which coke, sintered ore, pellets, and lump ores (hereinafter referred to as ores) are charged in layers from the top of the furnace, such as a blast furnace or shaft furnace. The present invention relates to the structure of a detection sonde for measuring the thickness of a charge deposit by utilizing the difference in electrical resistance between coke and ore-like layers.

高炉およびシャフト炉などの還元溶解炉では、ベル型も
しくは旋回シュート型の炉頂装入装置によって所定量づ
つ非連続で、しかもコークスと鉱石類を交互に装入して
いる。
In reduction melting furnaces such as blast furnaces and shaft furnaces, coke and ores are charged discontinuously and alternately in predetermined amounts using a bell-shaped or rotating chute-type furnace top charging device.

この場合、ベル型装入装置1では、第1図においてムー
バブルアーマ−2の位置により、また旋回シュート型装
入装置では、シュートの傾斜角の違いにより装入物分布
形状が変化する。
In this case, in the bell-shaped charging device 1, the shape of the charge distribution changes depending on the position of the movable armor 2 in FIG. 1, and in the rotating chute-type charging device, depending on the inclination angle of the chute.

このことは同時に、炉径方向における装入物堆積層厚も
大きく変化する。
At the same time, the charge deposition layer thickness in the furnace radial direction also changes significantly.

この結果、炉下部の羽目から送風して生じる炉内ガスの
流れに大きな影響を与える。
As a result, the flow of gas in the furnace caused by air being blown from the slats in the lower part of the furnace is greatly affected.

すなわち、通気抵抗の大きい鉱石層が厚い部分にはガス
流れが少なく反対に薄い部分にはガス流れが多くなる。
In other words, there is less gas flow in areas where the ore layer with high ventilation resistance is thick, and conversely, gas flow is greater in areas where the ore layer is thin.

このガス流れが著しく偏流した場合には、棚吊り、スリ
ップ、さらにはガス吹抜けなどのトラブルを生じ、炉の
正常な操業が維持できなくなる。
If this gas flow is significantly unbalanced, problems such as shelving, slipping, and gas blow-through may occur, making it impossible to maintain normal operation of the furnace.

したがって、安定した操業状態を維持するには、常に望
ましいガス流れ分布となるよう装入物の層厚を調整する
必要がある。
Therefore, in order to maintain stable operating conditions, it is necessary to constantly adjust the layer thickness of the charge to obtain the desired gas flow distribution.

層厚を調整する方法として、ベル型装入装置ではアーマ
−プレート2の位置を変更し、また旋回シュート型装入
装置ではシュートの傾斜角を変える手段があるが、いづ
れにしても適切な層厚調整を行なうためには、堆積層厚
を確実に測定しなければならない。
The layer thickness can be adjusted by changing the position of the armor plate 2 in a bell-type charging device, or by changing the angle of inclination of the chute in a rotating chute-type charging device. In order to adjust the thickness, it is necessary to reliably measure the thickness of the deposited layer.

第1図、第2図a、bに従来の装入物層厚測定方法例お
よび検知ゾンデの構造例を示す。
1 and 2a and 2b show an example of a conventional charge layer thickness measurement method and an example of the structure of a detection sonde.

ここで、第2図aは装入物粒径が30mm以下の比較的
細粒の多い場合に使用され、第2図すは、30mm以上
の粗粒の多い場合によく使用される検知ゾンデの例であ
る。
Here, Fig. 2a shows a detection sonde which is used when the charge particle size is relatively large in size of 30 mm or less, and Fig. 2 shows a detection sonde which is often used in cases where there are many coarse particles with a particle size of 30 mm or more. This is an example.

この方法は、一対の電極間距離40mmでコークス堆積
層の電気抵抗が1〜3g1鉱石類が1000〜1000
0.Qで両者に大きな差異があることを利用したもので
ある。
In this method, when the distance between a pair of electrodes is 40 mm, the electrical resistance of the coke deposited layer is 1 to 3 g, and the ore is 1000 to 1000.
0. This takes advantage of the fact that there is a large difference in Q between the two.

装入物堆積層の電気抵抗測定は、絶縁物質12を挾んで
一対の電極10.11を有するゾンデで行ない、このゾ
ンデ2個7.7′を、高さhだけ異ならせて、炉壁から
炉内へ挿入固定し、該電極に接触する装入物の電気抵抗
値から、コークス層5か、鉱石類層6かを判定して、そ
の装入物層の降下時間tを求め、同時に、コークス、鉱
石類層間の境界面を検知し、この境界面が2個のゾンデ
7.7′の間を降下する時間から、装入物の降下速度■
を求め、このVとゾンデ7又は7′で検知したtとから
装入物層厚を求める方法である。
The electrical resistance measurement of the charge deposited layer is carried out using a sonde having a pair of electrodes 10.11 with the insulating material 12 in between. Determine whether it is a coke layer 5 or an ore layer 6 from the electrical resistance value of the charge that is inserted and fixed into the furnace and comes into contact with the electrode, determine the falling time t of the charge layer, and at the same time, The interface between the coke and ore layers is detected, and from the time it takes for this interface to descend between the two sondes 7.7', the rate of descent of the charge is
This method calculates the charge layer thickness from this V and t detected by the sonde 7 or 7'.

したがって、装入物の電気抵抗をいかに精度よく測定す
るかということが、層厚測定の重要なポイントとなって
いる。
Therefore, how to accurately measure the electrical resistance of the charge is an important point in layer thickness measurement.

なお、第1図において、3は検尺針、4は炉壁を示して
いる。
In addition, in FIG. 1, 3 indicates a measuring needle, and 4 indicates a furnace wall.

しかるに、第2図a、bに示す従来の検知ゾンデによる
測定では、炉内装入物の電気抵抗測定値が、経時的に大
きく変化し、ある期間以上経過するとほとんど抵抗測定
ができなくなる欠点をもっている。
However, the measurement using the conventional detection sonde shown in Figure 2 a and b has the disadvantage that the measured electrical resistance of the contents in the furnace changes greatly over time, and after a certain period of time it becomes almost impossible to measure the resistance. .

この例を第3図a、b、cに示す。すなわち、検知ゾン
デ設置2日後では、コークス層1〜”Qz鉱石類層80
0〜1000.Qを示しているが、20日後では、鉱石
類層が80〜110.Qまで低下し、50日後では、1
0Q前後となり、コークス層か、鉱石類層かの判定がで
きず装入物層厚を求めることが不可能となる。
Examples of this are shown in Figures 3a, b, and c. That is, two days after the installation of the detection sonde, the coke layer 1 to "Qz ore layer 80"
0~1000. However, after 20 days, the ore layer is 80~110. Q and after 50 days, 1
It becomes around 0Q, and it becomes impossible to determine whether it is a coke layer or an ore layer, and it becomes impossible to determine the charge layer thickness.

この原因は、炉内に挿入された検知ゾンデの電極10.
11間の絶縁物質12に、炉内ガスに混じって飛散する
コークス粉や、炉内ガス中に含まれるCOガスが2CO
−+CO2+Cなる反応でCを析出し、このCが付着す
ることによって、絶縁不良を起し、電極10.11間の
電気抵抗がコークスの電気抵抗と同程度まで低下するこ
とによるものである。
This is due to the detection sonde's electrode 10 inserted into the furnace.
The insulating material 12 between 11 and 2CO contains coke powder mixed with the furnace gas and CO gas contained in the furnace gas.
This is because C is precipitated by the reaction -+CO2+C, and this C adheres, causing insulation failure and reducing the electrical resistance between the electrodes 10 and 11 to the same level as the electrical resistance of coke.

本発明は、これらの問題を解決し、長期間にわたって安
定して装入物の電気抵抗を測定できるようにしたもので
ある。
The present invention solves these problems and makes it possible to measure the electrical resistance of a charge stably over a long period of time.

以下第4図a + bおよび第5図に、本発明の層厚検
知ゾンデの構造例を示す。
4a + b and FIG. 5 below show structural examples of the layer thickness sensing sonde of the present invention.

第4図aは、一対の電極io、ii間の絶縁物質12内
に先端部まで通じるガス導入管14を設け、炉内装入物
に面する電極10.11の間に、多数の円形、あるいは
長方形またはスリット型の小穴を明けたドーナツ型円板
状のアダプター15を絶縁物質で製作してこれを嵌合し
、一方、炉外側よりガス導入管14にガス吹込管13を
取付け、外部よりN2、空気などのガスを吹込み、アダ
プター15の小穴よりガスを噴出させる構造とすること
を特徴とする。
In FIG. 4a, a gas introduction pipe 14 is provided in the insulating material 12 between a pair of electrodes io and ii, leading to the tip, and a large number of circular or A donut-shaped disk-shaped adapter 15 with a rectangular or slit-shaped small hole is made of an insulating material and fitted.Meanwhile, a gas blowing pipe 13 is attached to the gas introduction pipe 14 from outside the furnace, and N2 is injected from the outside. It is characterized by having a structure in which a gas such as air is blown into the adapter 15 and the gas is ejected from a small hole in the adapter 15.

また第4図すは、多数の小穴を明けたリング状のアダプ
ター16を電極10゜11の間に嵌合し、ガス導入管1
4、ガス吹込管13よりガス吹込み、アダプター16の
小穴よりガスを噴出させる構造としたものである。
In addition, FIG. 4 shows a ring-shaped adapter 16 with many small holes fitted between the electrodes 10 and 11, and the gas introduction pipe 1
4. It has a structure in which gas is blown in from the gas blowing pipe 13 and gas is ejected from the small hole in the adapter 16.

なお、アダプター15又は16に設ける穴は、できるだ
け均等にガスが噴出するように、2TnTILφ以下と
し10個以上多数あけることが望ましい。
Note that it is preferable that the holes provided in the adapter 15 or 16 be 2TnTILφ or less and ten or more holes so that the gas can be ejected as evenly as possible.

本発明による検知ゾンデによれば、炉内ガスに混じって
飛散するコークス粉や、COガスの分解によって析出す
るCが、絶縁アダプター15又は16より噴出するガス
により炉内側に吹飛ばされ、絶縁物質12の全面に付着
しないので、電極10゜11間の絶縁が保持されて、装
入物堆積層自体の電気抵抗を長期間安定して測定するこ
とができる。
According to the detection sonde of the present invention, coke powder mixed with the furnace gas and C precipitated by decomposition of CO gas are blown away inside the furnace by the gas ejected from the insulating adapter 15 or 16, and the insulating material Since it does not adhere to the entire surface of electrodes 12, insulation between electrodes 10 and 11 is maintained, and the electrical resistance of the charge deposited layer itself can be measured stably over a long period of time.

第6図に、本発明による検知ゾンデを設置してから60
日後の測定チャート例を示すが、第3図aの設置直後の
電気抵抗値とほとんど同じ値を示していることが判る。
Figure 6 shows that 60 years have passed since the detection sonde according to the present invention was installed.
An example of a measurement chart after a few days is shown, and it can be seen that the electrical resistance value is almost the same as the electrical resistance value immediately after installation in Figure 3a.

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

第1図は、装入物の堆積層厚の測定方法を示す説明図、
第2図a、bは、従来の層厚検知ゾンデの構造例を示す
断面図、第3図は、従来の検知ゾンデを使用した場合の
電気抵抗測定値の経時変化を示す説明図、第4図a、b
は、本発明による層厚検知ゾンデの構造例を示す断面図
、第5図は、多孔質アダプターの拡大説明図、第6図は
、本発明による検知ゾンデを使用した場合のチャート例
である。 1・・・・・・ベル、2・・・・・・ムーバブルアーマ
−13・・・・・・検尺針、4・・・・・・炉壁、5・
・・・・・コークス層、6・・・・・・鉱石層、7およ
び7′・・・・・・検知ゾンデ、10および11・・・
・・・電極、12・・・・・・絶縁物質、13・・・・
・・ガス吹込管、14・・・・・・ガス導入管、15お
よび16・・・・・・多孔アダプター。
FIG. 1 is an explanatory diagram showing a method for measuring the deposited layer thickness of charges;
Figures 2a and 2b are cross-sectional views showing an example of the structure of a conventional layer thickness sensing sonde, Figure 3 is an explanatory diagram showing changes over time in electrical resistance measurements when using a conventional sensing sonde, and Figure 4 Diagram a, b
5 is an enlarged explanatory view of a porous adapter, and FIG. 6 is an example of a chart when the detection sonde according to the present invention is used. 1... Bell, 2... Movable armor 13... Measuring needle, 4... Furnace wall, 5...
...Coke layer, 6...Ore layer, 7 and 7'...Detection sonde, 10 and 11...
... Electrode, 12 ... Insulating material, 13 ...
...Gas blowing pipe, 14... Gas introduction pipe, 15 and 16... Porous adapter.

Claims (1)

【特許請求の範囲】[Claims] 1 高炉、シャフト炉などの還元溶解炉の炉壁から炉内
へ装入し炉内装入物堆積層の電気抵抗の変化を測定して
該堆積層厚を検知するゾンデにおいて、ゾンデ先端部の
一対の電極間絶縁部にドーナツ型円板状又はリング状で
多数の小穴を有するアダプターを設置し、該絶縁部内に
ガス導入管を埋設し、このガス導入管の先端を前記アダ
プターに連通ずると共に後端を炉壁外に設置したガス吹
込管と連通せしめたことを特徴とする装入物堆積層厚検
知ゾンデ。
1. In a sonde that is charged into the furnace from the furnace wall of a reduction melting furnace such as a blast furnace or shaft furnace and measures the change in electrical resistance of the deposited layer of contents in the furnace to detect the thickness of the deposited layer, a pair of A donut-shaped disk-shaped or ring-shaped adapter having a large number of small holes is installed in the inter-electrode insulation part, a gas introduction pipe is buried in the insulation part, and the tip of the gas introduction pipe is communicated with the adapter and the rear A sonde for detecting charge deposit layer thickness, characterized in that its end is connected to a gas blowing pipe installed outside the furnace wall.
JP5729276A 1976-05-20 1976-05-20 Charge deposition layer thickness detection sonde Expired JPS5832207B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5729276A JPS5832207B2 (en) 1976-05-20 1976-05-20 Charge deposition layer thickness detection sonde

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5729276A JPS5832207B2 (en) 1976-05-20 1976-05-20 Charge deposition layer thickness detection sonde

Publications (2)

Publication Number Publication Date
JPS52141257A JPS52141257A (en) 1977-11-25
JPS5832207B2 true JPS5832207B2 (en) 1983-07-12

Family

ID=13051467

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5729276A Expired JPS5832207B2 (en) 1976-05-20 1976-05-20 Charge deposition layer thickness detection sonde

Country Status (1)

Country Link
JP (1) JPS5832207B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60114623A (en) * 1983-10-21 1985-06-21 エアー.プロダクツ.アンド.ケミカルス.インコーポレーテツド Heater
JPS63113205A (en) * 1986-10-29 1988-05-18 Isuzu Motors Ltd Combustion control device for heater

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102392089A (en) * 2011-11-03 2012-03-28 江苏省沙钢钢铁研究院有限公司 Simple Measuring Device and Method for Radial Coke and Ore Layer Thickness Distribution of Blast Furnace

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60114623A (en) * 1983-10-21 1985-06-21 エアー.プロダクツ.アンド.ケミカルス.インコーポレーテツド Heater
JPS63113205A (en) * 1986-10-29 1988-05-18 Isuzu Motors Ltd Combustion control device for heater

Also Published As

Publication number Publication date
JPS52141257A (en) 1977-11-25

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