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JPH0447003B2 - - Google Patents
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JPH0447003B2 - - Google Patents

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Publication number
JPH0447003B2
JPH0447003B2 JP28088484A JP28088484A JPH0447003B2 JP H0447003 B2 JPH0447003 B2 JP H0447003B2 JP 28088484 A JP28088484 A JP 28088484A JP 28088484 A JP28088484 A JP 28088484A JP H0447003 B2 JPH0447003 B2 JP H0447003B2
Authority
JP
Japan
Prior art keywords
fluidization
electrical resistance
charge
furnace
detection
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
JP28088484A
Other languages
Japanese (ja)
Other versions
JPS61153221A (en
Inventor
Kanji Takeda
Seiji Taguchi
Emi Murakawa
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.)
JFE Steel Corp
Original Assignee
Kawasaki 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 Kawasaki Steel Corp filed Critical Kawasaki Steel Corp
Priority to JP28088484A priority Critical patent/JPS61153221A/en
Publication of JPS61153221A publication Critical patent/JPS61153221A/en
Publication of JPH0447003B2 publication Critical patent/JPH0447003B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は装入物流動化検知方法およびその装置
に関し、高炉の操業上重要な装入物の安定な降下
に対する阻害現象である流動化を検知する技術で
あり、シヤフト炉を用いた冶金用炉に適用でき
る。
[Detailed Description of the Invention] [Industrial Field of Application] The present invention relates to a method and device for detecting fluidization of a burden, and is a method for detecting fluidization, which is a phenomenon that inhibits stable descent of a burden, which is important in the operation of a blast furnace. This is a detection technology that can be applied to metallurgical furnaces using shaft furnaces.

〔従来の技術〕[Conventional technology]

高炉操業にとつて安定な装入物降下は欠くこと
のできない条件である。高炉内のガス流速が小さ
い間は、ガス装入物を浮上させる浮力は装入物の
自重より小さく、装入物の降下に何ら影響を与え
ない。ガスによる装入物の浮力はガス流速の1.7
乗に比例して増大するためガス流速が増加するに
つれ急激に増加する。ガスによる浮力が装入物の
自重に打ち勝つようになると装入物が流動化を開
始し、円滑な装入物降下が望めなくなる。
Stable burden descent is an essential condition for blast furnace operation. While the gas flow rate in the blast furnace is low, the buoyancy force that floats the gas charge is smaller than the weight of the charge itself, and has no effect on the descent of the charge. The buoyancy of the charge due to gas is 1.7 of the gas flow rate.
Since it increases in proportion to the power of the gas flow rate, it increases rapidly as the gas flow rate increases. When the buoyancy caused by the gas begins to overcome the weight of the charge, the charge begins to fluidize, making it impossible to expect the charge to descend smoothly.

このような流動化を検知するため、従来はシヤ
フト部に取付けられた圧力計の測定値が用いられ
ていた(特公昭53−19217)。
In order to detect such fluidization, the measured value of a pressure gauge attached to the shaft was conventionally used (Japanese Patent Publication No. 53-19217).

この検知方法は高炉の高さ方向のある一定区間
の圧力損失〓P/〓Lとその間の装入物の自重と
の比を求め、この比が1以上となつたら流動化状
態にあると判断する方法である。装入物が均一
で、かつ圧力損失が高炉の高さ方向に一定である
場合にはこの従来法でも正確に検知できる。
This detection method calculates the ratio between the pressure loss 〓P/〓L in a certain section in the height direction of the blast furnace and the dead weight of the charge in that section, and when this ratio is 1 or more, it is judged that the fluidization state is present. This is the way to do it. If the charge is uniform and the pressure loss is constant in the height direction of the blast furnace, accurate detection can be achieved with this conventional method.

しかし、高炉内には通常通気抵抗の異なる鉱
石、コークスが層状に装入され、半径方向にも粒
径(通気抵抗)が異なるため、圧力損失と自重と
の比が1以下であつても炉内装入物は局部的に流
動化を開始する。したがつて、実際の流動化検知
には、圧力損失と自重との比が1以下のある基準
値を越えたら流動化と判定している。すなわち炉
内おける流動化という現象を従来は圧力損失の大
きさから間接的に求めていたことになる。基準値
の設定は装入物降下状態と圧力損失の関係を操業
データから求めて経験的に定められている。しか
し通常は圧力損失と降下状態の間には明確な対応
が認められず、またこの関係の中には流動化以外
の他の因子の影響も含まれてくるという欠点を有
していいた。一方、高炉装入物内に電極を2本入
れ、その間の抵抗を測定する方法は、特開昭52−
14447、あるいは特開昭53−18408に示されてい
る。主として鉱石、コークスの電気気抵抗の差を
利用して各層の層厚や降下速度を求める技術であ
る。
However, ores and coke with different ventilation resistances are usually charged in layers in a blast furnace, and the grain sizes (airflow resistance) also differ in the radial direction, so even if the ratio of pressure loss to dead weight is less than 1, The internal contents start to fluidize locally. Therefore, in actual fluidization detection, fluidization is determined when the ratio of pressure loss to dead weight exceeds a certain reference value of 1 or less. In other words, the phenomenon of fluidization in the furnace has conventionally been determined indirectly from the magnitude of pressure loss. The reference value is determined empirically by determining the relationship between the burden descent state and pressure loss from operational data. However, there is usually no clear correspondence between the pressure loss and the falling state, and this relationship has the disadvantage that it includes the influence of factors other than fluidization. On the other hand, a method of inserting two electrodes into the blast furnace charge and measuring the resistance between them was published in JP-A-52-
14447, or as shown in Japanese Patent Application Laid-Open No. 53-18408. This is a technology that primarily uses the difference in electrical resistance between ore and coke to determine the thickness and rate of descent of each layer.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

本発明は高炉内装入物の流動化状態を、上述の
ような圧力損失のような間接的な方法ではなく、
装入物内に挿入した電極によつて直接検知し、炉
内における局部的な流動化を早期に発見、改善す
ることを目的とするものである。
The present invention maintains the fluidization state of the contents in the blast furnace, rather than using indirect methods such as pressure loss as described above.
The purpose of this is to detect and improve localized fluidization in the furnace at an early stage by directly detecting it with an electrode inserted into the charge.

〔問題点を解決するための手段〕[Means for solving problems]

流動化という現象を直接捕えるためには高炉内
の流動化の特徴を利用する必要がある。発明者ら
は模型実験により種々検討した結果、高炉のよう
に粗粒で、しかも層高が高い層において流動化し
た場合には、スラツキング状態となる事を見出し
た。スラツキング状態とは大きな空隙が周期的に
発生、上昇、消滅を繰り返す状態である。
In order to directly capture the phenomenon of fluidization, it is necessary to utilize the characteristics of fluidization inside the blast furnace. As a result of various studies conducted through model experiments, the inventors found that when fluidized in a layer with coarse grains and a high layer height, such as in a blast furnace, a slugging state occurs. The slugging state is a state in which large voids repeatedly appear, rise, and disappear periodically.

本発明は流動化のこの特徴を、層内に挿入した
電極間の電気抵抗の変化により捕えることを特徴
的技術手段とするものである。すなわち本発明方
法は高炉内に特定の1対の電極を挿入し、この電
極間の電気抵抗の変化を解析し、この解析値と基
準値とを比較することによつて炉内装入物の流動
化現象の発生を判定する。そのためには、 (1) 炉内の状態の変化を明確に捕えることのでき
る、ある限度以上の大きさの電極を用い、 (2) 得られた電気信号を処理して流動化の特徴を
抽出して流動化を判定すること、 が必要となつてくる。
The characteristic technical means of the present invention is to capture this characteristic of fluidization by changing the electrical resistance between electrodes inserted within the layer. In other words, the method of the present invention inserts a specific pair of electrodes into a blast furnace, analyzes changes in electrical resistance between the electrodes, and compares the analyzed value with a reference value to determine the flow of the contents in the furnace. Determine the occurrence of oxidation phenomenon. To do this, (1) use electrodes larger than a certain limit that can clearly capture changes in the state inside the furnace, and (2) process the obtained electrical signals to extract the characteristics of fluidization. It becomes necessary to determine fluidization based on

本発明では、流動化に伴う層構造の周期的な変
化を電気抵抗で捕える。このため十分に大きな接
地用電極と、一定の大きさの検知用電極とを組合
せてその電極間の電気抵抗を測定する。
In the present invention, periodic changes in the layer structure accompanying fluidization are captured by electrical resistance. For this purpose, a sufficiently large grounding electrode and a detection electrode of a certain size are combined and the electrical resistance between the electrodes is measured.

第1図は本発明方法を好適に実施することので
きる第1の本発明の装置の実施例のブロツク図で
ある。
FIG. 1 is a block diagram of a first embodiment of the apparatus of the present invention, which can suitably carry out the method of the present invention.

検知用電極1と接地用電極3とは絶縁体2を介
して一体に形成してあり、炉壁から炉内に容易に
挿入できるように例えば棒状の測定端子を形成し
ている。
The detection electrode 1 and the grounding electrode 3 are integrally formed with an insulator 2 in between, and form a rod-shaped measurement terminal, for example, so that it can be easily inserted into the furnace from the furnace wall.

この検知用電極1と接地用電極3との間に直流
電圧を負荷し、両端子間の抵抗を測定する抵抗測
定器10が結線されている。炉内に挿入された検
知用電極1と接地用電極3との間には、図示しな
いコークスや鉱石などから成る導電性のある粒子
が抵抗をもつた電気回路を形成している。これら
の粒子と十分な接触を保つために検知用電極の露
出面の広さは後述のように一定値以上となつてい
る。
A resistance measuring device 10 is connected between the detection electrode 1 and the grounding electrode 3 to apply a DC voltage and measure the resistance between both terminals. Between the detection electrode 1 inserted into the furnace and the grounding electrode 3, conductive particles made of coke, ore, etc. (not shown) form an electrical circuit with resistance. In order to maintain sufficient contact with these particles, the width of the exposed surface of the sensing electrode is set to a certain value or more, as will be described later.

抵抗測定器10が測定した抵抗値は周波数解析
装置11に入力される。周波数解析装置としては
公知の装置を用いればよい。この周波数解析装置
11は入力された電気抵抗の変化をスペクトル解
析する。そのスペクトル解析された出力の0.05〜
5Hzの間に存在する電気抵抗波形のエネルギー密
度の高値を流動化判定装置12が検出し、流動化
状態を把握する。
The resistance value measured by the resistance measuring device 10 is input to the frequency analysis device 11. A known device may be used as the frequency analysis device. This frequency analysis device 11 spectrally analyzes changes in the input electrical resistance. 0.05 of its spectrally analyzed output
The fluidization determination device 12 detects the high value of energy density of the electrical resistance waveform that exists between 5 Hz and grasps the fluidization state.

本発明方法を好適に実施することのできる第2
の本発明装置は、上記第1の装置の周波数解析装
置の代りにパルス発生装置を備え、流動化判定装
置はこのパルスを解析して判定する。すなわち、
パルス発生装置は抵抗測定装置10の測定値を入
力として受入れ、電気抵抗が一定以上の高値とな
つた値をパルスとして出力する。流動化判定装置
はこのパルスが例えば3回/分以上となつたとき
流動化の生起を判定する。
A second method that can suitably carry out the method of the present invention
The device of the present invention includes a pulse generator instead of the frequency analyzer of the first device, and the fluidization determining device analyzes and determines this pulse. That is,
The pulse generator receives the measured value of the resistance measuring device 10 as input, and outputs as a pulse the value when the electrical resistance is higher than a certain value. The fluidization determining device determines the occurrence of fluidization when the pulse rate is, for example, 3 times/min or more.

上記第1、第2の本発明の装置において検知用
電極1が炉内装入物と好適な接触を保ち、本発明
装置の測定精度を確保するためには、検知用電極
1が一定以上の表面積を有する必要があり、高炉
装入物の導電性粒体の調和平均径の0.5〜10倍の
直径および露出長さを有する丸棒であると優れた
効果を示す。
In the first and second devices of the present invention, in order for the detection electrode 1 to maintain suitable contact with the contents in the furnace and to ensure the measurement accuracy of the device of the present invention, the detection electrode 1 must have a surface area of at least a certain level. A round bar with a diameter and exposed length that is 0.5 to 10 times the harmonic mean diameter of the conductive particles in the blast furnace charge exhibits an excellent effect.

第2図aには、通常状態のコークス層の電気抵
抗の変化を、第2図bには流動化時の電気抵抗の
変化を、第2図cには不十分な大きさの電極を用
いた場合の電気抵抗変化をそれぞれ示す。
Figure 2a shows the change in electrical resistance of the coke layer under normal conditions, Figure 2b shows the change in electrical resistance during fluidization, and Figure 2c shows the change in electrical resistance when an insufficiently large electrode is used. The electrical resistance changes are shown for each case.

〔作用〕[Effect]

次に本発明方法およびその装置の作用について
第2図乃至第5図を用いて説明する。
Next, the operation of the method and apparatus of the present invention will be explained using FIGS. 2 to 5.

炉内のコークス層が通常状態にある場合、すな
わち、流動化していないときは、第2図aに示さ
れるように検知用電極と接地用電極との間はコー
クスによつて電気的に導通しており、あるレベル
の電気抵抗を定常的に示している。しかしコーク
ス層が流動化すると第2図bに示すように、間欠
的に極めて高い抵抗値のピークを示すようにな
る。電極の大きさが不十分なときは、第2図cの
ような抵抗変化を示し、通常状態が流動状態かの
判定はできない。
When the coke layer in the furnace is in a normal state, that is, when it is not fluidized, there is electrical continuity between the sensing electrode and the grounding electrode due to the coke, as shown in Figure 2a. It constantly exhibits a certain level of electrical resistance. However, when the coke layer becomes fluidized, as shown in FIG. 2b, it begins to exhibit extremely high resistance peaks intermittently. When the size of the electrode is insufficient, a resistance change as shown in FIG. 2c occurs, and it is not possible to determine whether the normal state is a flowing state.

第2図a,bの2つの状態を明確に区別しうる
電極の大きさを求めるため検知用電極の長さ、コ
ークスの径を種々変更して実験したところ第3図
の関係があることがわかつた。第3図中白丸は第
2図a,bの2つの状態を区別できる場合を示し
ている。流動化を検知するには検知用電極の大き
さ、あるいは太さとしてコークス径の0.5倍から
10倍の範囲が適当である。さらに、コークス径の
1〜5倍の範囲が最も望ましいことが明らかにな
つた。0.5倍未満の寸法の電極ではコークス層の
電気抵抗が安定的に測定できず、10倍よりも大き
な電極では周期性が現われない。第2図bのよう
な周期的な電気抵抗の変化は流動化時特有のもの
であり、鉱石層、混合層の電気抵抗変化と容易に
見分けがつく。このことを電気信号処理により定
量的に評価する方法および装置としては以下の2
つがある。
In order to determine the size of the electrode that can clearly distinguish between the two states shown in Figure 2 a and b, experiments were conducted by varying the length of the detection electrode and the diameter of the coke, and the relationship shown in Figure 3 was found. I understand. The white circles in FIG. 3 indicate the case where the two states a and b in FIG. 2 can be distinguished. To detect fluidization, the size or thickness of the detection electrode should be 0.5 times the coke diameter.
A range of 10x is appropriate. Furthermore, it has become clear that a range of 1 to 5 times the coke diameter is most desirable. If the electrode size is less than 0.5 times, the electrical resistance of the coke layer cannot be stably measured, and if the electrode size is larger than 10 times, periodicity will not appear. The periodic change in electrical resistance as shown in FIG. 2b is unique to fluidization and can be easily distinguished from changes in electrical resistance in ore layers and mixed layers. The following two methods and devices are used to quantitatively evaluate this using electrical signal processing.
There is one.

(1) 電気信号のスペクトル解析装置を用いて解析
を行うと第4図のようなスペクトルが得られ
る。第4図に示されるように、高炉内装入物が
流動化した時は、0.05〜5Hzの間に特徴的なピ
ークが現われる。このピークの現われる周波数
は流動化領域の径により異なり、第5図に示さ
れるような関係にある。通常の高炉の大きさを
考えると0.05〜5Hzという範囲のピークを対象
にすれば良いことがわかる。また、この第5図
より周波数が小さい方が大きい方より流動化領
域の径が大きいことが分る。この間のスペクト
ルのピークを基準となる値と比較することによ
り高炉内の装入物の流動化を定量的に判定する
ことができる。
(1) When an electrical signal is analyzed using a spectrum analyzer, a spectrum as shown in Figure 4 is obtained. As shown in FIG. 4, when the contents in the blast furnace are fluidized, a characteristic peak appears between 0.05 and 5 Hz. The frequency at which this peak appears varies depending on the diameter of the fluidized region, and has a relationship as shown in FIG. Considering the size of a normal blast furnace, it can be seen that the peak in the range of 0.05 to 5 Hz should be targeted. Furthermore, it can be seen from FIG. 5 that the diameter of the fluidized region is larger when the frequency is smaller than when the frequency is larger. By comparing the peak of the spectrum during this period with a reference value, fluidization of the charge in the blast furnace can be quantitatively determined.

(2) 電気信号を処理するもう一つの方法はスペク
トル解析を行なわずに、電極間の抵抗の高値に
応じてパルスを出力し、この周期的な信号を直
接計数し、、その係数値を基準値と比較するこ
とにより炉内のコークスの流動化を定量的に判
定する。
(2) Another method of processing electrical signals is to output pulses according to the high value of the resistance between the electrodes, directly count this periodic signal, and use the coefficient value as the standard, without performing spectrum analysis. The fluidization of coke in the furnace is determined quantitatively by comparing the values.

〔実施例〕〔Example〕

実施例 1 本発明に係る電極を水平ゾンデと呼ばれる高炉
内半径方向の測定棒にセツトして本発明を実施し
た例を第6図に示す。先端部が検知用電極1であ
り、接地用電極3はこの場合測定棒自体となつて
いる。検知用電極1の径は炉内のコークスの調和
平均径20mmの1.5倍の30mm、長さは2.5倍の50mmと
している。検知用電極1の根元には、接地電極3
との短絡を防止するための耐火物2を溶射してあ
る。絶縁処理をしたシース電線7により接地電極
との短絡を防止しながら、炉外の電気抵抗測定装
置10に接続している。コークス粉による電極間
の短絡を防止するためゾンデ内にはN2パージ5
をしている。
Example 1 FIG. 6 shows an example in which the present invention was carried out by setting the electrode according to the present invention on a measuring rod called a horizontal sonde in the radial direction inside the blast furnace. The tip is the sensing electrode 1, and the grounding electrode 3 is the measuring rod itself in this case. The diameter of the detection electrode 1 is 30 mm, which is 1.5 times the harmonic mean diameter of 20 mm of the coke in the furnace, and the length is 50 mm, which is 2.5 times the harmonic mean diameter of the coke in the furnace. A ground electrode 3 is located at the base of the detection electrode 1.
A refractory material 2 is thermally sprayed to prevent short circuits. It is connected to an electrical resistance measuring device 10 outside the furnace using an insulated sheathed wire 7 while preventing a short circuit with a ground electrode. N2 purge inside the sonde to prevent short circuit between electrodes due to coke powder
doing.

このゾンデをシヤフト部の炉中心と炉壁周辺に
挿入し流動化検知を行なつた例を第7図に示す。
FIG. 7 shows an example in which this sonde was inserted into the shaft portion of the furnace center and around the furnace wall to detect fluidization.

この場合には、周波数スペクトルのピークは
0.5Hz近傍に現われたので、このピークの推移を
示している。送風量増加以前は、中心部周辺部と
もに0.05〜5Hz間にはピーク値が現われていな
い。送風量を増加したところ中心では、0.5Hz近
傍にピークが現われ、ピーク値も急激に大きくな
つた。一方周辺部ではそのままピークは現われて
いない。中心部のピークはその後送風量の減少に
より消減した。波形解析装置にノイズ防止のため
一定のバイアスをもたせた基準値を設定したとこ
ろ、自動的に中心部の流動化を明確に検知するこ
とができた。
In this case, the peak of the frequency spectrum is
Since it appeared near 0.5Hz, it shows the transition of this peak. Before the air flow rate was increased, no peak values appeared between 0.05 and 5 Hz in both the center and periphery areas. When the air flow rate was increased, a peak appeared around 0.5Hz at the center, and the peak value also increased rapidly. On the other hand, no peak appears in the peripheral area. The peak in the center then disappeared due to a decrease in air flow. By setting a reference value with a certain bias in the waveform analyzer to prevent noise, we were able to automatically and clearly detect fluidization in the center.

実施例 2 第8図には、スペクトル解析を行なわず、周期
的な信号を直接計数することにより流動化検知を
行つた結果について示す。電極、および電気抵抗
の測定装置は、第6図に示した実施例と同じもの
を用い、周波数解析装置のかわりに、一定の抵抗
値以上になつた時パルスを発生するパルス発生装
置およびパルスを計数し、基準回数と比較する判
定装置を取付けた。
Example 2 FIG. 8 shows the results of fluidization detection by directly counting periodic signals without performing spectrum analysis. The electrodes and the electrical resistance measuring device are the same as in the embodiment shown in Figure 6, and instead of the frequency analyzer, a pulse generator that generates a pulse when the resistance exceeds a certain value and a pulse generating device are used. A judgment device was installed to count and compare with the standard number of times.

第8図に抵抗値の実測値および、実測値に対し
て50〓を基準値として出力したパルスを示す。
10sec間に15回のパルスが出ていて、このうち1
回を除いて流動化時特有のピーク値に対応してい
る。第9図には長時間パルスを計数した結果の推
移を示す。測定開始後10時間後に測定回数が急激
に増加し、炉内が流動化したことを検知してい
る。
Fig. 8 shows the actual measured value of the resistance value and the pulse outputted with 50〓 of the actual measured value as a reference value.
15 pulses are emitted in 10 seconds, and 1 of these
This corresponds to the peak value unique to fluidization, except for times. FIG. 9 shows the transition of the results of counting long-term pulses. Ten hours after the start of measurements, the number of measurements increased rapidly, and it was detected that the inside of the furnace had become fluidized.

第2図aに示されるように通常の場合のベース
線のコークスの電気抵抗は数〓から10〓程度であ
る。これに対し、流動化により生ずる電気抵抗の
変化は、コークス層の電気抵抗と、絶縁状態の抵
抗(数M〓)との間を周期的に変化する。前述の
スペクトル解析からも分るように、この周期は
0.05〜5Hzの間にある。したがつて、コークス層
の電気抵抗に一定の定数(例えば20程度)を乗じ
た値を基準抵抗値とし、この基準値を越えて抵抗
が変化する回数を計数する。周期が0.05〜5Hzと
いうことは最小3回/分以上計数されると流動化
と判定できることを示している。つまりコークス
層の抵抗値に一定の値を乗じた基準抵抗値を定
め、単位時間内にこの基準抵抗値以上となつた回
数を計数し、その値を3回/分以上の基準回数と
比較することにより炉内の流動化を検知すること
ができる。この方法はパルス発生装置によつて実
現することができ、上記1の方法のように波形解
析装置により安価となる利点がある。
As shown in FIG. 2a, the electrical resistance of coke at the base line in the normal case is about 10 to 10. On the other hand, the change in electrical resistance caused by fluidization periodically changes between the electrical resistance of the coke layer and the resistance of the insulating state (several M〓). As can be seen from the spectrum analysis mentioned above, this period is
It is between 0.05 and 5Hz. Therefore, a value obtained by multiplying the electrical resistance of the coke layer by a certain constant (for example, about 20) is set as a reference resistance value, and the number of times the resistance changes beyond this reference value is counted. The fact that the period is 0.05 to 5 Hz indicates that fluidization can be determined if the count is at least 3 times/minute or more. In other words, a reference resistance value is determined by multiplying the resistance value of the coke layer by a certain value, the number of times the resistance value exceeds this reference value within a unit time is counted, and that value is compared with the reference number of times of 3 times/minute or more. This makes it possible to detect fluidization within the furnace. This method can be realized by a pulse generator, and has the advantage of being inexpensive because it uses a waveform analyzer like method 1 above.

以上の説明では高炉について述べたが、本発明
は、導電体が充填された移動層型の反応器、例え
ばコークス充填層を用いた鉄の直接還元やFe−
Crの還元装置の流動化の検知に適用することが
できる。また、シヤフト炉を用いた直接還元炉の
炉下部(金属鉄が出る領域)の流動化の検知にも
適用することができる。
In the above explanation, a blast furnace has been described, but the present invention is also applicable to direct reduction of iron using a moving bed type reactor filled with a conductor, such as a coke packed bed.
It can be applied to detecting fluidization in Cr reduction equipment. It can also be applied to detecting fluidization in the lower part of a direct reduction furnace using a shaft furnace (the area where metallic iron comes out).

〔発明の効果〕〔Effect of the invention〕

本発明によれば、従来の方法および装置では不
可能だつた高炉内における 流動化の直接検知 局部的流動化の検知 が可能となつた。篭流動化検知により早期に流動
化防止アクシヨンをとることが可能となり、高炉
操業のトラブルを未然に防止できる。
According to the present invention, it has become possible to directly detect fluidization and detect local fluidization in a blast furnace, which was impossible with conventional methods and devices. Detection of cage fluidization makes it possible to take early action to prevent fluidization, thereby preventing problems in blast furnace operation.

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

第1図は本発明の装置構成を示すブロツク図、
第2図は電気抵抗波形の種類を示すグラフ、第3
図は適正な電極の大きさを示すグラフ、第4図は
周波数解析例のグラフ、第5図はピーク位置と流
動化域の大きさを示すグラフ、第6図は実施例の
ブロツク図、第7図は流動化検知例のグラフ、第
8図は実施例のチヤート、第9図は実施例のグラ
フである。 1……検知用電極、2……絶縁体、3……接地
用電極、4……給排水、5……N2パージ、6…
…シリンダー、7……シース電線。
FIG. 1 is a block diagram showing the configuration of the device of the present invention;
Figure 2 is a graph showing the types of electrical resistance waveforms;
Figure 4 is a graph showing an appropriate electrode size, Figure 4 is a graph showing an example of frequency analysis, Figure 5 is a graph showing the peak position and the size of the fluidized region, Figure 6 is a block diagram of an example, and Figure 6 is a graph showing an example of frequency analysis. FIG. 7 is a graph of an example of fluidization detection, FIG. 8 is a chart of an example, and FIG. 9 is a graph of an example. 1...Detection electrode, 2...Insulator, 3...Grounding electrode, 4...Water supply and drainage, 5... N2 purge, 6...
...Cylinder, 7...Sheathed electric wire.

Claims (1)

【特許請求の範囲】 1 高炉内に挿入した1対の電極間の電気抵抗の
変化を解析し、該解析値から炉内装入物の流動化
現象を判定することを特徴とする装入物流動化検
知方法。 2 検知用電極および接地用電極を絶縁体を介し
て一体に形成した炉内挿入測定端子と、該測定端
子に直流電圧を負荷して電気抵抗を測定する装置
と、該電気抵抗の変化をスペクトル解析する周波
数解析装置と、その0.05〜5Hz間に存在する電気
抵抗波形のエネルギー密度の高値を検出する流動
化判定装置とから成ることを特徴とする装入物流
動化検知装置。 3 検知用電極が高炉装入物の導電性粒体の調和
平均径の0.5〜10倍の直径および長さである特許
請求の範囲第2項に記載の流動化検知装置。 4 検知用電極および接地用電極を絶縁体を介し
て一体に形成した炉内挿入測定端子と、該測定端
子に直流電圧を負荷して電気抵抗を測定する装置
と、電気抵抗の高値となつた値をパルスに変換し
て出力するパルス発生装置と、このパルスが3
回/分以上となつたときに流動化を判定する流動
化判定装置とからなることを特徴とする装入物流
動化検知装置。 5 検知用電極が高炉装入物の導電性粒体の調和
平均径の0.5〜10倍の直径および長さである特許
請求の範囲第4項に記載の流動化検知装置。
[Claims] 1. A charge flow method characterized by analyzing changes in electrical resistance between a pair of electrodes inserted into a blast furnace, and determining a fluidization phenomenon of a charge in the furnace from the analyzed value. Detection method. 2. A measurement terminal inserted into the furnace, in which a detection electrode and a grounding electrode are integrally formed via an insulator, a device for measuring electrical resistance by applying a DC voltage to the measurement terminal, and a spectrometer for measuring changes in electrical resistance. A charge fluidization detection device comprising a frequency analysis device for analysis and a fluidization determination device for detecting a high value of energy density of an electrical resistance waveform existing between 0.05 and 5 Hz. 3. The fluidization detection device according to claim 2, wherein the detection electrode has a diameter and length that are 0.5 to 10 times the harmonic mean diameter of the conductive particles of the blast furnace charge. 4. A measurement terminal inserted into the furnace in which a detection electrode and a grounding electrode are integrally formed via an insulator, a device that measures electrical resistance by applying a DC voltage to the measurement terminal, and a device that measures electrical resistance by applying a DC voltage to the measurement terminal. A pulse generator that converts a value into a pulse and outputs it, and this pulse
1. A charge fluidization detection device comprising: a fluidization determination device that determines fluidization when the rate is equal to or higher than times per minute. 5. The fluidization detection device according to claim 4, wherein the detection electrode has a diameter and length that are 0.5 to 10 times the harmonic mean diameter of the conductive particles of the blast furnace charge.
JP28088484A 1984-12-27 1984-12-27 Method and device for detecting fluidization of charge Granted JPS61153221A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28088484A JPS61153221A (en) 1984-12-27 1984-12-27 Method and device for detecting fluidization of charge

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28088484A JPS61153221A (en) 1984-12-27 1984-12-27 Method and device for detecting fluidization of charge

Publications (2)

Publication Number Publication Date
JPS61153221A JPS61153221A (en) 1986-07-11
JPH0447003B2 true JPH0447003B2 (en) 1992-07-31

Family

ID=17631284

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28088484A Granted JPS61153221A (en) 1984-12-27 1984-12-27 Method and device for detecting fluidization of charge

Country Status (1)

Country Link
JP (1) JPS61153221A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102023104407A1 (en) 2023-02-23 2024-08-29 Thyssenkrupp Steel Europe Ag Method for operating a direct reduction plant

Also Published As

Publication number Publication date
JPS61153221A (en) 1986-07-11

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