JPH11172307A - Charging method of charged material into blast furnace when being difficult to form horizontal type terrace - Google Patents
Charging method of charged material into blast furnace when being difficult to form horizontal type terraceInfo
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- JPH11172307A JPH11172307A JP34870797A JP34870797A JPH11172307A JP H11172307 A JPH11172307 A JP H11172307A JP 34870797 A JP34870797 A JP 34870797A JP 34870797 A JP34870797 A JP 34870797A JP H11172307 A JPH11172307 A JP H11172307A
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- Prior art keywords
- blast furnace
- furnace
- charging
- difficult
- coke
- Prior art date
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Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、ベルレス式高炉の
炉頂部におけるコークス、鉱石等の装入物層による水平
型テラス形成が困難時の装入物の装入方法に関するもの
である。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for charging a bell-less blast furnace when it is difficult to form a horizontal terrace with a layer of a charge such as coke or ore at the furnace top.
【0002】[0002]
【従来の技術】高炉における主な制御手段の一つとし
て、装入物分布制御がある。装入物分布制御は、炉内の
反応伝熱を左右するガス流分布および融着帯の形状を決
める唯一の手段であるため、最もよく用いられかつ最も
重要な制御手段である。ベルレス式高炉においては、高
炉炉頂部の装入物装入旋回シュート(以降旋回シュート
と呼ぶ)の先端から排出した装入物を炉内に落下させる
が、装入物は落下した位置を頂点として堆積する。した
がって、落下点が炉壁側にある場合には、装入物の堆積
プロフィルはV型になり、落下点が炉壁側から離れて炉
内側にある場合には装入物の堆積プロフィルはM型にな
る。2. Description of the Related Art Charge distribution control is one of the main control means in a blast furnace. Charge distribution control is the most commonly used and most important control means because it is the only means to determine the gas flow distribution and cohesive zone shape that govern the reaction heat transfer in the furnace. In a bellless blast furnace, the charge discharged from the tip of a charge chute (hereinafter referred to as a swirl chute) at the top of the blast furnace is dropped into the furnace. accumulate. Therefore, when the drop point is on the furnace wall side, the deposition profile of the charge is V-shaped, and when the drop point is away from the furnace wall side and inside the furnace, the deposition profile of the charge is M. Be a type.
【0003】従来の装入方法では、鉱石、コークス共に
堆積プロフィルはV型あるいはM型になるか、V型とM
型の組み合わせになる。しかして、上記堆積プロフィル
により決まる通気抵抗の半径方向分布により、炉内ガス
流分布および融着帯形状が決まってくる。しかし、V型
分布の場合には粒度偏析を最大限利用できるため中心流
の強化には適しているが、装入物の落下位置が炉壁側に
あるため炉内に装入された装入物の粉が炉壁近傍に濃縮
して堆積することになり、炉壁への付着物生成の要因と
なる可能性が大きい。[0003] In the conventional charging method, the deposition profile of both ore and coke is V-type or M-type, or V-type and M-type.
It becomes a combination of types. Thus, the gas flow distribution in the furnace and the shape of the cohesive zone are determined by the radial distribution of the ventilation resistance determined by the deposition profile. However, in the case of the V-shaped distribution, although the particle size segregation can be used to the maximum extent, it is suitable for strengthening the central flow. The material powder concentrates and accumulates near the furnace wall, which is highly likely to be a factor of the formation of deposits on the furnace wall.
【0004】M型分布の場合あるいはV型とM型の組み
合わせ分布の場合には、落下軌跡の変動に起因する装入
物頂点の半径方向位置の変化により、炉壁近傍の鉱石と
コークスの層厚比(以降O/Cと呼ぶ)が大幅に変化し
やすくなるため、炉壁近傍のガス流の不安定化を招く可
能性が大きい。In the case of the M-type distribution or the combination distribution of the V-type and the M-type, the ore and coke layers near the furnace wall are changed due to a change in the radial position of the charge apex caused by the variation of the falling trajectory. Since the thickness ratio (hereinafter, referred to as O / C) easily changes greatly, there is a large possibility that the gas flow near the furnace wall will become unstable.
【0005】図1は通常の旋回シュートによるV型とM
型の組み合わせ分布の場合の鉱石とコークスの装入状態
を示したもので、該旋回シュートの位置が同一位置にあ
っても鉱石とコークスとでは落下場所にずれを生じ、ま
た安息角の違いによって堆積する装入層の状態が異なる
ことが判る。なお、点線はコークス装入時の装入位置の
ずれを示したもので、旋回シュートの摩耗およびコーク
スの種類、粒度が異なったために炉内側に若干偏った装
入位置となったことを表している。このため炉壁側のコ
ークス量が少なくなり、不均一な装入層が形成される。FIG. 1 shows a V-shape and an M with a normal turning chute.
This shows the loading state of ore and coke in the case of the combination distribution of types, and even if the position of the turning chute is at the same position, the ore and coke fall off at the drop location, and due to the difference in the angle of repose It can be seen that the state of the charge layer to be deposited is different. Note that the dotted line shows the displacement of the charging position when charging coke, indicating that the charging position was slightly biased toward the inside of the furnace due to the difference in the wear of the turning chute and the type and grain size of coke. I have. For this reason, the coke amount on the furnace wall side is reduced, and an uneven charge layer is formed.
【0006】このような状態では炉壁部分での装入物堆
積状態が不均一となり、この不均一によって炉内通気性
が変わり、炉内のガス流分布中、特に周辺ガス流の異常
を生ずる結果、いわゆる荷下がり異常、壁付き等、炉况
異常を誘発する原因となる。したがって、粉を炉壁近傍
からできるだけ分散させ、しかも落下軌跡の変動に起因
する炉壁近傍のO/Cの大幅変動が極めて小さく、か
つ、装入層表面を水平型テラス状に形成することが望ま
しい。すなわち、図2に示すような理想型のテラスが形
成されれば均一性に優れた装入層となり、前記した装入
層の乱れによる種々の障害を克服することができる。In such a state, the state of charge accumulation on the furnace wall becomes non-uniform, and this non-uniformity changes the air permeability in the furnace, causing abnormalities in the gas flow distribution in the furnace, especially in the peripheral gas flow. As a result, this causes abnormalities in the furnace situation, such as so-called unloading abnormalities and wall attachment. Therefore, it is possible to disperse the powder from the vicinity of the furnace wall as much as possible, and to make the fluctuation of the O / C near the furnace wall extremely small due to the change of the falling trajectory, and to form the charging layer surface in a horizontal terrace shape. desirable. That is, if the ideal type terrace as shown in FIG. 2 is formed, a charged layer having excellent uniformity can be obtained, and various obstacles caused by the disturbance of the charged layer can be overcome.
【0007】従来、水平型テラスを形成する方法とし
て、例えば特開平6−145731号公報にその技術が
開示されている。その技術は特別な設備を必要とするも
ので、高炉内炉頂部の円周方向の複数位置に設けた装入
物掻き均し具により、高炉内の円周方向各位置で往復運
動させ、炉壁側の堆積装入物を炉中心方向へ押し出し、
かつ、掻き均すことによって炉壁部分に原料平坦部を所
定量形成するものである。したがって、炉円周方向での
装入物堆積状態、特に炉壁部分での装入物堆積状態を均
一化できる。Conventionally, a technique for forming a horizontal terrace has been disclosed in, for example, Japanese Patent Application Laid-Open No. 6-145731. The technology requires special equipment, and the reciprocating motion at each circumferential position in the blast furnace is performed by means of a load leveling tool provided at a plurality of circumferential positions at the top of the furnace in the blast furnace. Extruding the charge on the wall side toward the furnace center,
In addition, a predetermined amount of a raw material flat portion is formed on the furnace wall by scraping. Therefore, the charge accumulation state in the furnace circumferential direction, particularly the charge accumulation state in the furnace wall portion, can be made uniform.
【0008】このような従来方法では、高炉炉頂部の円
周方向の複数の位置に装入物を掻き均すための装置が必
要となり、高炉が大型化するに従い、それに要する設備
規模も大きくならざるを得ず、コスト的な見地からみて
も優れた方法とは言い難い。そこで本発明者らは、上記
問題点の解決を特別な設備を要さずに、目的とするコー
クス、鉱石ともに水平型のテラス形成を達成させるため
に、鋭意検討を行いその開発を試みた。その結果、単に
高炉装入時に装入物の装入パターンを操作するという簡
易な方法により上記目的を達成できることに成功し、特
願平9−269161号「高炉炉頂装入物の水平型テラ
ス形成方法」(以下、先願発明と記す)として既に出願
済みである。[0008] In such a conventional method, a device for stirring the charge at a plurality of positions in the circumferential direction of the top of the blast furnace is required, and as the size of the blast furnace increases, the required equipment scale becomes larger. Inevitably, it is hard to say that it is an excellent method from the viewpoint of cost. Accordingly, the present inventors have conducted intensive studies and attempted to develop the above-mentioned problems in order to achieve the formation of a horizontal terrace for both the target coke and the ore without special equipment. As a result, the above-mentioned object can be achieved by a simple method of simply operating the charging pattern of the charged material at the time of charging the blast furnace. Japanese Patent Application No. 9-269161, entitled “Horizontal Terrace of Blast Furnace Top Charged Material”. Forming method "(hereinafter referred to as the prior invention).
【0009】その概要を記すと、ベルレス高炉におい
て、高炉炉内の装入物装入用旋回シュートを調整するこ
とによって、炉頂部装入物層表面の傾斜角を水平に対し
て±15度の範囲内に収まり、かつ炉頂部装入物層のテ
ラス先端が炉半径で除した相対距離で高炉炉壁面から
0.1〜0.6の範囲に収まるようなテラスを形成する
こと、また、テラスの形成は炉壁側から行い、装入物の
装入をそれに合わせ旋回シュートによる装入パターンを
調整すること、さらに、テラスを形成させたい範囲にお
いて、旋回シュートの傾斜角のきざみ幅を2°以内にし
て装入物を装入すること、さらにまた、テラス形成操作
は、鉱石装入時に先立ちコークス装入にて行う等による
高炉炉頂装入物の水平型テラス形成方法にある。In summary, in a bellless blast furnace, the inclination angle of the surface of the furnace top charge layer is adjusted by ± 15 degrees with respect to the horizontal by adjusting the rotating chute for charging the charge in the blast furnace. Forming a terrace that falls within the range and that the tip of the terrace of the furnace top charge layer falls within the range of 0.1 to 0.6 from the wall of the blast furnace at a relative distance divided by the furnace radius; Is formed from the furnace wall side, and the charging pattern is adjusted by adjusting the charging pattern by the swirling chute in accordance with the charging of the charge. In addition, the charging operation and the terrace forming operation are performed in a method of forming a horizontal terrace of the blast furnace top charging by performing coke charging prior to ore charging.
【0010】[0010]
【発明が解決しようとする課題】しかし、本発明者らの
開発した前記発明を実施したところ、水平型テラス形成
の初期においては、時によって所望する水平型テラスが
得られない事態が起こることが判明した。そこで本発明
者らは、その理由を解明すべく多くの検討を重ねたとこ
ろ、現状の高微粉炭吹き込み操業下においては、高炉シ
ャフト部を上昇する羽口部から送風されるガスの上昇流
が不均一化し、高炉炉壁周辺部に偏った流れを発生し、
例えば図3に示すように炉壁側にガス上昇流の流れが強
く生ずる場合があり、高炉への装入物装入を炉壁周辺部
から行う先願発明の実施に際してはその影響を諸に受
け、炉壁周辺部への装入物の堆積をスムーズに行うのに
困難を伴う事態が発生することがある。However, when the above-mentioned invention developed by the present inventors is practiced, a situation in which a desired horizontal terrace cannot be obtained sometimes occurs at an early stage of forming a horizontal terrace. found. Accordingly, the present inventors have conducted a number of studies to elucidate the reason.Under the current high pulverized coal injection operation, the upward flow of gas blown from the tuyere section that ascends the blast furnace shaft section. Non-uniformity and uneven flow around the blast furnace wall,
For example, as shown in FIG. 3, there is a case where the flow of the gas rising flow strongly occurs on the furnace wall side, and the effects of the prior application of the present invention in which the charged material is charged into the blast furnace from the periphery of the furnace wall are variously affected. In some cases, it may be difficult to smoothly deposit the charge on the periphery of the furnace wall.
【0011】また、炉壁周辺部に装入した装入物と、炉
中心部または/および炉壁部と中心部間の装入物との間
で降下速度が異なる(装入物の降下が非常に速い場合、
逆に非常に遅い場合)場合があり、装入物の装入に対し
ては同様の影響を及ぼすことが判った。本発明は上記の
ような現象が発生したときに、高炉内での上昇ガス流の
均一化を図り、また装入物の降下速度を安定化させるた
めの適切な手段を提供することを目的とするものであ
る。[0011] Further, the rate of descent differs between the charge charged in the periphery of the furnace wall and the charge in the center of the furnace or / and between the furnace wall and the center. If very fast,
On the contrary, it was found to have a similar effect on the loading of the charge. An object of the present invention is to provide an appropriate means for stabilizing a descending speed of a charged material in order to equalize an ascending gas flow in a blast furnace when the above phenomenon occurs. Is what you do.
【0012】[0012]
【課題を解決するための手段】本発明の要旨とするとこ
ろは、下記手段にある。 (1)ベルレス高炉において、高炉炉内の装入物装入用
旋回シュートを調整することによって、高炉炉壁側から
装入物による水平型テラスを形成するに際し、所要の水
平型テラス面の形成に困難が伴う場合、高炉炉中心部所
定範囲内へ積極的にコークスを装入する高炉内水平型テ
ラス形成困難時の高炉装入物装入方法。 (2)前記高炉炉中心部の所定範囲内へ装入するコーク
スは、通常装入時とは別個にコークス装入のみを行う
(1)記載の高炉内水平型テラス形成困難時の高炉装入
物装入方法。The gist of the present invention lies in the following means. (1) In a bellless blast furnace, a required horizontal terrace surface is formed by forming a horizontal terrace from the blast furnace wall side by adjusting a rotating chute for charging a charge in the blast furnace. The method for charging a blast furnace charge when it is difficult to form a horizontal terrace inside the blast furnace, in which coke is positively charged into a predetermined area in the center of the blast furnace when difficulties arise. (2) The coke charged into the predetermined range of the central part of the blast furnace is only charged with coke separately from the normal charging. Material loading method.
【0013】(3)前記高炉炉中心部の所定範囲内を少
なくとも炉中心から炉口半径で10%の領域とした
(1)または(2)記載の高炉内水平型テラス形成困難
時の高炉装入物装入方法。 (4)前記高炉炉中心部の所定範囲内に装入するコーク
スの粒径を50mm以上とした(1)ないし(3)のい
ずれかに記載の高炉内水平型テラス形成困難時の高炉装
入物装入方法。(3) The blast furnace mounting in the case where it is difficult to form a horizontal terrace in the blast furnace according to (1) or (2), wherein a predetermined range of the center of the blast furnace is at least a region of 10% from the furnace center by a furnace opening radius. Packing method. (4) The blast furnace charging in the case where it is difficult to form a horizontal terrace in the blast furnace according to any one of (1) to (3), wherein the particle size of the coke charged into a predetermined range in the central portion of the blast furnace is 50 mm or more. Material loading method.
【0014】[0014]
【発明の実施の形態】本発明者らは前述した従来の技術
的問題点を如何にして解決を図るかにつき、種々の研
究、検討を重ねた結果、本発明の如き解決法を見出した
ものである。前記「発明が解決しようとする課題」の項
で述べたように、高炉内でのガス上昇流が不均一の場合
は、その不均一な流れを早急に解消してやらねば目的と
する高炉装入物による水平型テラスの形成が、前記先願
発明に記した装入方法を採用しても安定した水平型テラ
スの形成に時間を要し、高炉操業上多くの不都合な事態
が惹起する恐れがある。BEST MODE FOR CARRYING OUT THE INVENTION The present inventors have conducted various studies and studies on how to solve the above-mentioned conventional technical problems, and as a result, have found a solution as in the present invention. It is. As described in the section of “Problems to be Solved by the Invention”, when the gas ascending flow in the blast furnace is not uniform, the target blast furnace charge must be eliminated as soon as the uneven flow is eliminated. The formation of a horizontal terrace by the method requires time to form a stable horizontal terrace even if the charging method described in the invention of the prior application is adopted, and many inconveniences may occur in the operation of the blast furnace. .
【0015】そこで本発明者らは、先ず、高炉炉壁周辺
部を多量に流れる上昇ガス流を抑制するためには、ガス
流れに対する抵抗の少ないコークスを炉中心部に多く装
入することにより、上昇ガス流の流れが容易な部分を炉
中心部に作り込み、その部分での上昇ガス流れを一時的
に多くさせることによって、炉壁周辺部に流れていた大
量の上昇ガス流を短期間で阻止し、炉内全体のガス流れ
をほぼ均一な状態に確保してやることができるとの結論
を得、それを高炉への装入物装入時に適用することによ
って、前記先願発明の実施を滞りなく行うことができる
ことを確認し、本発明の開発をみるに至った。The inventors of the present invention first introduced a large amount of coke having a low resistance to gas flow into the furnace center in order to suppress a rising gas flow flowing in a large amount around the blast furnace wall. A large part of the rising gas flow flowing around the furnace wall can be reduced in a short period of time by creating a part where the flow of the rising gas flow is easy at the center of the furnace and temporarily increasing the rising gas flow in that part. It was concluded that it was possible to prevent the gas flow in the entire furnace in a substantially uniform state, and to apply it when charging the blast furnace with the charge, which hindered the implementation of the invention of the earlier application. It has been confirmed that the present invention can be carried out without any problems, and the development of the present invention has been reached.
【0016】高炉中心部へ装入するコークスの装入方法
については特に限定しないが、通常の装入物装入時に意
図的にコークスのみが炉中心部に多く装入できるように
旋回シュートの位置、装入時期、装入量等を調整するこ
とによって行うこともでき、また、コークス装入のみを
通常装入とは別個に行うことも可能である。The method of charging coke to be charged into the center of the blast furnace is not particularly limited. However, the position of the swirling chute is set so that only the coke can be intentionally charged into the center of the furnace at the time of normal charging. The charging can be performed by adjusting the charging timing, the charging amount, and the like, and it is also possible to perform only the coke charging separately from the normal charging.
【0017】高炉中心部に装入するコークスの装入範囲
は少なくとも炉中心部から炉口半径で10%の領域が好
ましく、また、コークスの粒度については、ガス上昇流
の抵抗度を小さくするという見地からは50mm以上の
粒度が好ましい。これら高炉中心部に装入するコークス
は、装入物全体のO/Cの決められた範囲内でその量を
調整し、装入物全体のO/Cを維持するよう考慮すべき
である。The charging range of the coke to be charged into the center of the blast furnace is preferably at least a region of 10% in the furnace opening radius from the center of the furnace, and the particle size of the coke is to reduce the resistance of the gas ascending flow. From a viewpoint, a particle size of 50 mm or more is preferable. The amount of coke charged to these blast furnace centers should be adjusted to maintain the overall charge O / C within a fixed range of the overall charge O / C.
【0018】高炉内上昇ガス流が不安定でかつ不均一で
ある場合には、本発明方法を実施することにより、安定
かつ均一な上昇ガス流の分布状態を得ることが可能とな
るので、その後は、上記した先願発明に記載された装入
物の装入方法により水平型テラスの形成を極めて容易に
行うことができる。When the rising gas flow in the blast furnace is unstable and non-uniform, it is possible to obtain a stable and uniform distribution of the rising gas flow by implementing the method of the present invention. According to the method, the horizontal terrace can be formed extremely easily by the charging method of the charging material described in the above-mentioned prior application invention.
【0019】[0019]
【実施例】以下、本発明について稼動中の高炉において
実施し、その効果の確認を行ったのでその例について説
明する。操業を行った高炉は、微粉炭の吹き込みを実施
中の3280m3 の内容積を有するベルレス高炉であ
り、先願発明での装入物による水平型テラスの形成が期
待していたような形状に形成されなかったので、本発明
の実施に踏み切った。そこで通常の旋回シュートによる
高炉装入物の装入時に、通常の装入とは別個に高炉中心
部(炉中心から炉半径でほぼ10%)にコークスの投入
を試みた。コークスの粒度は約70mm(平均粒径)で
あり、それを10チャージ繰り返して行った(約2時間
にわたって)ところ、以後の装入物の装入による水平型
テラス形成が目的とする所定範囲内に収めることができ
るようになった。DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, the present invention was carried out in a blast furnace in operation, and its effects were confirmed. The blast furnace that was operated was a bellless blast furnace having an internal volume of 3280 m 3 in which pulverized coal was being injected. Since it was not formed, the implementation of the present invention was started. Therefore, at the time of charging the blast furnace charge with a normal swirling chute, an attempt was made to charge coke into the center of the blast furnace (about 10% of the furnace radius from the furnace center) separately from the normal charging. The particle size of the coke was about 70 mm (average particle size), and the charging was repeated 10 times (over about 2 hours). Can be stored in
【0020】この効果の確認として、シャフトゾンデに
よる高炉炉壁周辺部のηCOの変化状況を時系列で図4に
示した。本発明の実施により2時間後からその変化が小
さくなり、安定していることが図からも明らかである。
なお、本発明において記述したテラスの形成状態の判断
は何れも炉頂に設置されたプロフィルメーターで測定し
た得られた堆積プロフィルの検知結果に基づくものであ
る。As a confirmation of this effect, FIG. 4 shows a time series of changes in η CO around the blast furnace wall due to the shaft sonde. It is clear from the figure that the change is small and stable after 2 hours by implementing the present invention.
The judgment of the formation state of the terrace described in the present invention is based on the detection result of the obtained deposition profile measured by the profile meter installed on the furnace top.
【0021】[0021]
【発明の効果】以上に説明したように、本発明法の装入
方法によれば、水平型テラスの形成が困難時にその効果
を発揮することができる。本発明実施後は水平型テラス
を確実に形成させることができ、炉壁近傍の装入物の堆
積形状の安定性を確保できるため、円周方向に安定した
周辺ガス流を形成させることが容易となり、高炉操業に
おいて格段の優位性を保つことが可能となった。As described above, according to the charging method of the present invention, the effect can be exhibited when it is difficult to form a horizontal terrace. After implementation of the present invention, the horizontal terrace can be reliably formed, and the stability of the deposited shape of the charge in the vicinity of the furnace wall can be ensured. Therefore, it is easy to form a stable peripheral gas flow in the circumferential direction. As a result, it became possible to maintain a significant advantage in blast furnace operation.
【図1】通常の装入による装入物の堆積状態の一例を示
す図FIG. 1 is a diagram showing an example of a state of accumulation of a charge by normal charging.
【図2】理想型の水平型テラスの形成を示す図FIG. 2 is a view showing formation of an ideal horizontal terrace;
【図3】上昇ガスが偏流し炉壁面を多く流れる状況を示
す図FIG. 3 is a diagram showing a situation in which rising gas is deflected and flows much on the furnace wall surface.
【図4】本発明実施前・後のシャフトゾンデによる炉周
辺部のηCO変化を示す図FIG. 4 is a diagram showing a change in η CO around a furnace due to a shaft sonde before and after implementation of the present invention.
Claims (4)
物装入用旋回シュートを調整することによって、高炉炉
壁側から装入物による水平型テラスを形成するに際し、
所要の水平型テラス面の形成に困難が伴う場合、高炉炉
中心部所定範囲内へ積極的にコークスを装入することを
特徴とする高炉内水平型テラス形成困難時の高炉装入物
装入方法。In a bellless blast furnace, when a swirling chute for charging a charge in a blast furnace is adjusted, when forming a horizontal terrace by a charge from the blast furnace wall side,
When it is difficult to form the required horizontal terrace, the coke is positively charged into a predetermined area in the center of the blast furnace. Method.
るコークスは、通常装入時とは別個にコークス装入のみ
を行うことを特徴とする請求項1記載の高炉内水平型テ
ラス形成困難時の高炉装入物装入方法。2. The horizontal terrace in a blast furnace according to claim 1, wherein the coke charged into a predetermined area in the central portion of the blast furnace is only charged with coke separately from the normal charging. Blast furnace charging method when forming is difficult.
とも炉中心から炉口半径で10%の領域としたことを特
徴とする請求項1または請求項2記載の高炉内水平型テ
ラス形成困難時の高炉装入物装入方法。3. A blast furnace horizontal terrace formation is difficult according to claim 1 or 2, wherein a predetermined range of the blast furnace central portion is at least a region of 10% in a furnace opening radius from the furnace center. Blast furnace charging method at the time.
るコークスの粒径を50mm以上としたことを特徴とす
る請求項1ないし請求項3のいずれかに記載の高炉内水
平型テラス形成困難時の高炉装入物装入方法。4. A horizontal terrace in a blast furnace according to claim 1, wherein the particle size of the coke charged in a predetermined range in the central part of the blast furnace is 50 mm or more. Blast furnace charging method when forming is difficult.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP34870797A JPH11172307A (en) | 1997-12-04 | 1997-12-04 | Charging method of charged material into blast furnace when being difficult to form horizontal type terrace |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP34870797A JPH11172307A (en) | 1997-12-04 | 1997-12-04 | Charging method of charged material into blast furnace when being difficult to form horizontal type terrace |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH11172307A true JPH11172307A (en) | 1999-06-29 |
Family
ID=18398830
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP34870797A Withdrawn JPH11172307A (en) | 1997-12-04 | 1997-12-04 | Charging method of charged material into blast furnace when being difficult to form horizontal type terrace |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH11172307A (en) |
-
1997
- 1997-12-04 JP JP34870797A patent/JPH11172307A/en not_active Withdrawn
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