JPH0811804B2 - Charging method for different materials of bellless blast furnace - Google Patents
Charging method for different materials of bellless blast furnaceInfo
- Publication number
- JPH0811804B2 JPH0811804B2 JP61136449A JP13644986A JPH0811804B2 JP H0811804 B2 JPH0811804 B2 JP H0811804B2 JP 61136449 A JP61136449 A JP 61136449A JP 13644986 A JP13644986 A JP 13644986A JP H0811804 B2 JPH0811804 B2 JP H0811804B2
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- Japan
- Prior art keywords
- charging
- furnace
- fine
- raw material
- grained
- 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.)
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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、ベルレス式高炉に異種原料を装入する方法
に関するものであり、より詳細には、粒径及び/又は性
状の異なる複数種類の鉄源及び/又は還元剤を分割して
高炉内の所定の位置に装入する際に、装入後の前記原料
の半径方向及び/又は円周方向の堆積量の分布の制御性
を向上させることを目的とした異種原料装入方法に関す
るものである。Description: TECHNICAL FIELD The present invention relates to a method for charging different raw materials into a bellless blast furnace, and more specifically, to a plurality of types having different particle sizes and / or properties. When the iron source and / or the reducing agent are divided and charged at a predetermined position in the blast furnace, the controllability of the distribution of the amount of the deposited raw material in the radial direction and / or the circumferential direction after the charging is improved. The present invention relates to a method for charging different raw materials for the purpose.
(従来の技術) 高炉操業においては、高炉炉頂部における鉄源と還元
剤の重量比(以下「O/C」と略記する)、粒径等の半径
方向の分布を適正に制御して、炉内における半径方向の
ガス流分布、熱流比分布を所定の範囲に維持し、鉱石の
還元・溶解を安定に行なう必要がある。(Prior art) In the operation of a blast furnace, the weight ratio of the iron source and the reducing agent (hereinafter abbreviated as "O / C") at the top of the blast furnace, the radial distribution of the particle size, etc. are properly controlled to It is necessary to maintain the radial gas flow distribution and heat flow ratio distribution within a predetermined range to stably reduce or dissolve the ore.
近年、半径方向のガス流分布の制御性の向上を、半径
方向の粒径分布の制御性の改善によって達成することお
よび安価な細粒原料の使用比率の増加によって銑鉄コス
トを低下させることを目的として、鉄源及び/又は還元
剤を事前に粗粒と細粒に分級し、これらを高炉内に各々
分割して装入するいわゆる粒度別装入法が開発され、ベ
ルレス式高炉にも適用されてきている。In recent years, it has been aimed to improve the controllability of the gas flow distribution in the radial direction by improving the controllability of the particle size distribution in the radial direction and to lower the pig iron cost by increasing the usage ratio of inexpensive fine-grain raw materials. As a result, a so-called particle size-specific charging method has been developed in which an iron source and / or a reducing agent is classified into coarse particles and fine particles in advance, and these are separately charged into a blast furnace, and is also applied to a bellless blast furnace. Is coming.
郷農等は、鉄源として使用する焼結鉱を高炉炉頂部へ
搬送する前に鉱石庫庫上で粗粒と細粒に篩分けして粗粒
焼結鉱と細粒焼結鉱に分割し、高炉内の所定位置に装入
する焼結鉱粒度別装入法について報告している(「鉄と
鋼」第69巻、1983年第4号S59頁)。Prior to transporting the sintered ore used as an iron source to the top of the blast furnace, Gono, etc. screened it into coarse and fine particles in the ore warehouse and divided it into coarse-grained ore and fine-grained ore. However, it has been reported about the charging method according to the particle size of the sintered ore which is charged into a predetermined position in the blast furnace ("Iron and Steel", Vol. 69, 1983, No. 4, S59).
彼等の粒度別装入法においては、粗粒焼結鉱とペレッ
トを混合して鉱石の2分割装入の第1の装入時に用い、
これを高炉内の中間部から中心部に堆積せしめて中心ガ
ス流を確保し、他方、小径のため通気性は悪いものの被
還元性・伝熱性に優れる細粒焼結鉱を鉱石の2分割装入
の第2の装入時に用い、これを高炉の炉壁部に堆積せし
めて炉壁ガス流を適度に抑制しつつ炉下部の不活性化を
防止せんとしている。In their grain size-specific charging method, coarse-grained sinter and pellets are mixed and used in the first charging of ore in two-part charging,
This is deposited from the middle part to the center part in the blast furnace to secure the central gas flow. On the other hand, the fine-grained sintered ore, which has a small diameter and is poor in permeability but has excellent reducibility and heat transfer properties, is divided into two parts. It is used during the second charging of the charging, and is deposited on the furnace wall of the blast furnace to appropriately suppress the furnace wall gas flow and prevent the inactivation of the lower part of the furnace.
従来のベルレス式高炉の粒度別装入法を第6図を用い
て説明する。高炉1の炉頂部へベルトコンベア2によっ
て搬送された粗粒焼結鉱3および細粒焼結鉱3′は、各
々上部ゲート弁4、4′および上部シール弁5、5′を
経て一旦炉頂バンカー6、6′に貯蔵され、高炉内に既
に装入されているコークス7が荷下がりして所定のスト
ックレベル8に到達すると、先ず粗粒焼結鉱3を貯蔵し
ている炉頂バンカー6側の下部ゲート弁9および下部シ
ール弁10を開操作し、粗粒焼結鉱3を分配シュート11を
介して炉内に装入する。そして、粗粒焼結鉱3の炉内装
入が完了すると下部ゲート弁9および下部シール弁10を
閉操作する。The charging method according to the particle size of the conventional bellless blast furnace will be described with reference to FIG. The coarse-grained sintered ore 3 and the fine-grained sintered ore 3'conveyed to the furnace top of the blast furnace 1 by the belt conveyor 2 pass through the upper gate valves 4, 4'and the upper seal valves 5, 5 ', respectively, and once When the coke 7 stored in the bunker 6, 6 ′ and already charged in the blast furnace is unloaded and reaches a predetermined stock level 8, first, the furnace top bunker 6 storing the coarse-grained sintered ore 3 is first stored. The lower gate valve 9 and the lower seal valve 10 on the side are opened, and the coarse-grained sintered ore 3 is charged into the furnace through the distribution chute 11. Then, when the introduction of the coarse-grained sintered ore 3 into the furnace is completed, the lower gate valve 9 and the lower seal valve 10 are closed.
次に細粒焼結鉱3′を貯蔵している炉頂バンカー6′
側の下部ゲート弁9′および下部シール弁10′を開操作
し、細粒焼結鉱3′を分配シュート11を介して炉内に装
入するのである。Next, the furnace top bunker 6'that stores the fine-grained sintered ore 3 '
The lower gate valve 9'and the lower seal valve 10 'on the side are opened, and the fine-grained sintered ore 3'is charged into the furnace through the distribution chute 11.
(発明が解決しようとする問題点) しかしながら、従来の粒度別装入方法においては、細
粒原料の装入法に制約があり、半径方向の粒径分布を高
精度に制御することができなかった。すなわち、細粒
原料の半径方向の装入位置が炉壁部に限定される。細
粒原料の使用量が限定される。という理由に基づくもの
であり、その各々について以下に詳述する。(Problems to be Solved by the Invention) However, in the conventional charging method according to particle size, there is a restriction in the charging method of the fine grain raw material, and the particle size distribution in the radial direction cannot be controlled with high accuracy. It was That is, the charging position in the radial direction of the fine-grain raw material is limited to the furnace wall. The amount of fine grain raw material used is limited. The reason is as follows, and each of them will be described in detail below.
先ず、第1の問題点である細粒原料の装入位置の限定
について述べる。First, the limitation of the charging position of the fine-grain raw material, which is the first problem, will be described.
従来の粒度別装入方法においては、分配シュートの傾
動角度(第6図中のθ:分配シュートの底面と高炉の炉
軸とのなす角度)を所定の角度から順次減少させて、原
料を炉壁部から順次炉中心部に向けて装入していた。従
って、ほとんどの場合、装入後の原料の表面形状は第6
図に示すようなV型かあるいはM型の形状を成してお
り、いずれも斜面を形成していた。このため細粒焼結鉱
をコークス層上に装入した場合、細粒焼結鉱装入位置近
傍のコークス層の表層部の一部が細粒焼結鉱の所有する
衝撃エネルギーによって削りとられて炉中心方向に移動
し、炉中心部にまで細粒焼結鉱とコークスの混合層が形
成されるのである。加えて、細粒焼結鉱の堆積角はコー
クスのそれより小さく、装入時にコークス層の斜面上で
移動することによって細粒焼結鉱を高炉内の所定の半径
方向位置に高精度に装入することは困難であった。In the conventional charging method according to grain size, the tilt angle of the distribution chute (θ in FIG. 6: angle formed by the bottom surface of the distribution chute and the furnace shaft of the blast furnace) is gradually decreased from a predetermined angle to feed the raw material into the furnace. It was charged from the wall toward the center of the furnace. Therefore, in most cases, the surface shape of the raw material after charging is 6th.
As shown in the figure, it has a V-shape or an M-shape, and each has a slope. Therefore, when the fine-grained sinter is charged on the coke layer, part of the surface layer of the coke layer near the charging position of the fine-grained sinter is scraped off by the impact energy possessed by the fine-grained sinter. Moving toward the center of the furnace, a mixed layer of fine-grained sintered ore and coke is formed even in the center of the furnace. In addition, the deposition angle of fine-grained sinter is smaller than that of coke, and the fine-grained sinter is loaded at a predetermined radial position in the blast furnace with high accuracy by moving on the slope of the coke layer during charging. It was difficult to enter.
そこで、前述した郷農等は、細粒焼結鉱を鉱石の分割
装入の1回目ではなく2回目(最後)に使用することに
よって細粒焼結鉱を装入位置に堆積させることを意図し
た。すなわち、鉱石の分割装入の1回目には粗粒焼結鉱
を用い、かつ、分配シュートの傾動角度のスケジュール
を制御して粗粒焼結鉱装入後の表面形状をM型形状とな
らしめ、炉壁と粗粒焼結鉱層との間に窪部を形成させた
のである。そして、鉱石の分割装入の2回目に細粒焼結
鉱を使用して分配シュートの傾動角度のスケジュールを
制御し、当該窪部に細粒焼結鉱を装入したのである。Therefore, the above-mentioned Gono, etc. intended to deposit the fine-grained sinter at the charging position by using the fine-grained sinter at the second (last) time of the ore division charging instead of the first time. did. That is, coarse grained ore is used for the first time of the ore division charging, and the tilt angle schedule of the distribution chute is controlled so that the surface shape after the coarse grained ore charging is not M-shaped. That is, a recess was formed between the furnace wall and the coarse-grained sintered ore layer. Then, the schedule of the tilt angle of the distribution chute was controlled by using the fine-grained sintered ore at the second time of the divided charging of the ore, and the fine-grained sintered ore was charged into the depression.
従って、鉱石装入時の鉱石とコークスの混合層形成は
第1回目装入に用いた粗粒焼結鉱装入時に形成され、細
粒焼結鉱は関与しないこととなる。また、細粒焼結鉱が
装入される窪部はコークスではなく粗粒焼結鉱で形成さ
れるため、細粒焼結鉱装入時の層変形抵抗が大きく、細
粒焼結鉱は装入位置に堆積することとなる。Therefore, the mixed layer formation of the ore and the coke at the time of charging the ore is formed at the time of charging the coarse-grained sintered ore used for the first charging, and the fine-grained sintered ore is not involved. In addition, since the recesses in which the fine-grained sintered ore is charged are formed by coarse-grained sintered ore instead of coke, the layer deformation resistance when charging the fine-grained sintered ore is large, and the fine-grained sintered ore is It will be deposited at the charging position.
このように、細粒焼結鉱の装入位置を炉壁部に限定す
れば、従来方法でも十分粒度別装入が可能ではあるが、
前述の窪部を他の半径方向位置に形成せしめることは、
粗粒焼結鉱装入時間の制約からして困難である。すなわ
ち、従来の粒度別装入法においては、分配シュートの傾
動角度を所定の角度から順次減少させていたため、装入
後の原料は斜面を形成し、この斜面の影響を抑制するた
めに細粒焼結鉱の装入位置は炉壁部に限定されていたの
である。In this way, if the charging position of the fine-grained sintered ore is limited to the furnace wall portion, it is possible to charge the particles by sufficient grain size even with the conventional method,
Forming the aforementioned recesses at other radial positions
It is difficult due to the restriction of the charging time of coarse-grained sintered ore. That is, in the conventional charging method by particle size, since the tilt angle of the distribution chute is gradually decreased from a predetermined angle, the raw material after charging forms a slope, and in order to suppress the influence of this slope, fine particles are added. The charging position of the sinter was limited to the furnace wall.
第2の問題点は細粒原料使用量の制約である。 The second problem is the restriction on the amount of fine grain raw material used.
前述のように従来の粒度別装入法においては、コーク
ス層斜面の上に粗粒焼結鉱を装入し、粗粒焼結鉱層と高
炉炉壁との間に形成される窪部に細粒焼結鉱を装入して
いた。従って、当該窪部の体積量に相当する細粒焼結鉱
量が、細粒焼結鉱使用量の上限となり、それ以上に細粒
焼結鉱量を増加すると、細粒焼結鉱の一部は窪部に堆積
できず、炉中間部から炉中心方向へ移動することになっ
て細粒焼結鉱の半径方向の堆積分布を高精度に制御する
ことは困難である。As described above, in the conventional charging method according to the grain size, coarse grained ore is charged on the slope of the coke layer, and fine grains are formed in the recess formed between the coarse grained ore layer and the blast furnace wall. It was charged with grain sinter. Therefore, the amount of fine-grained sinter corresponding to the volume of the depression becomes the upper limit of the amount of fine-grained sinter used, and if the amount of fine-grained sinter is increased beyond that, the amount of fine-grained sinter becomes larger. The part cannot be deposited in the recess, and it moves from the middle part of the furnace toward the center of the furnace, and it is difficult to control the deposition distribution of the fine-grained sintered ore in the radial direction with high accuracy.
なお、当該窪部の体積量を増加するために粗粒焼結鉱
装入時の分配シュート傾動角度のスケジュールを制御す
ることも可能であるが、この方法では不可避的に半径方
向のO/C分布が変化するために望ましくない。It is also possible to control the schedule of the tilt angle of the distribution chute at the time of charging coarse-grained sintered ore in order to increase the volume of the depression, but this method inevitably causes O / C in the radial direction. Undesirable due to varying distribution.
以上説明したように従来の粒度別装入法においては、
分配シュートの傾動角度を所定の角度から順次減少さ
せ、装入後の原料の表面が斜面を形成していたため、細
粒原料の半径方向の装入位置が炉壁部に限定されるこ
と、および細粒原料使用量に制約があった。As described above, in the conventional charging method according to particle size,
The tilt angle of the distribution chute is gradually reduced from a predetermined angle, and since the surface of the raw material after charging formed a slope, the charging position in the radial direction of the fine-grain raw material is limited to the furnace wall portion, and There was a limit to the amount of fine grain raw material used.
同様の問題は粒径だけでなく、塩基度の異なる焼結鉱
を炉内半径方向の所定の位置に区別して装入する場合な
どのように性状の異なる原料の装入方法においても生じ
ていた。Similar problems have occurred not only in the grain size but also in the charging method of raw materials having different properties, such as when charging differently basic sinters at different positions in the furnace radial direction. .
本発明は上記した従来方法の問題点を解消するために
なされたものであり、従来の粒度別装入法の前記問題点
が、炉内に装入された原料が斜面を形成するために生じ
ていることに注目し、炉内装入後の原料の堆積角が0度
を超えかつ20度を超えないような粒度別装入法を提供せ
んとするものである。The present invention has been made to solve the above-mentioned problems of the conventional method, and the above-mentioned problems of the conventional charging method according to particle size occur because the raw materials charged in the furnace form slopes. In view of the above, it is intended to provide a charging method according to particle size so that the deposition angle of the raw material after entering the furnace interior exceeds 0 degree and does not exceed 20 degrees.
(問題点を解決するための手段) 本発明は、ベルレス式高炉の炉内所定位置に、粒径及
び/又は性状の異なる複数種類の鉄源及び/又は還元剤
を分割して装入する方法において、炉中心部から炉壁方
向に向かって前記原料を装入すべく分配シュートの傾動
角度を制御すると共に、装入後の原料表面の堆積角が0
度を超えかつ20度を超えないように前記分配シュートの
傾動角度、各傾動角度における旋回数、下部ゲート弁の
開部のうちの少なくとも一つを制御することを要旨とす
るものである。(Means for Solving the Problems) The present invention is a method of dividing and charging a plurality of types of iron sources and / or reducing agents having different particle sizes and / or properties at predetermined positions in a furnace of a bellless blast furnace. In, the tilt angle of the distribution chute is controlled so as to charge the raw material from the center of the furnace toward the furnace wall, and the deposition angle of the raw material surface after charging is 0.
The gist is to control at least one of the tilt angle of the distribution chute, the number of revolutions at each tilt angle, and the opening of the lower gate valve so as not to exceed 20 degrees and more than 20 degrees.
本発明の構成を焼結鉱粒度別装入の例について第1図
に基づいて説明する。粗粒原料3および細粒原料3′が
ベルトコンベア2によって炉頂に搬送され、上部ゲート
弁4、4′および上部シール弁5、5′を経て一旦炉頂
バンカー6、6′に貯蔵され、既装入原料7が荷下がり
して所定のストックレベル8に到達すると、まず粗粒原
料3を貯蔵している炉頂バンカー6側の下部ゲート弁9
および下部シール弁10を開操作し、粗粒原料3を分配シ
ュート11を介して炉内に装入し、粗粒原料3の炉内装入
が完了したら下部ゲート弁9および下部シール弁10を閉
操作する。次に細粒原料3′を貯蔵している炉頂バンカ
ー6′側の下部ゲート弁9′および下部シール弁10′を
開操作し、細粒原料3′を分配シュート11を介して炉内
に装入する。以上の原料のフローは従来方法と同一であ
る。The structure of the present invention will be described with reference to FIG. The coarse-grain raw material 3 and the fine-grain raw material 3'are conveyed to the furnace top by the belt conveyor 2 and once stored in the furnace-top bunker 6, 6'through the upper gate valves 4, 4'and the upper seal valves 5, 5 '. When the already charged raw material 7 is unloaded and reaches a predetermined stock level 8, first, the lower gate valve 9 on the side of the bunker 6 that stores the coarse-grained raw material 3 is stored.
And the lower seal valve 10 is opened to load the coarse grain raw material 3 into the furnace through the distribution chute 11, and when the coarse grain raw material 3 has been placed inside the furnace, the lower gate valve 9 and the lower seal valve 10 are closed. Manipulate. Next, the lower gate valve 9'and the lower seal valve 10 'on the side of the furnace top bunker 6'which stores the fine-grained raw material 3'are opened, and the fine-grained raw material 3'is introduced into the furnace through the distribution chute 11. Charge. The flow of the above raw materials is the same as the conventional method.
ところで、本発明においては、前記した従来の粒度別
装入法における問題点である装入後の原料が斜面を形成
することを防止するために次のような方法を採用した。By the way, in the present invention, the following method is adopted in order to prevent the raw material after charging from forming a slope, which is a problem in the above-mentioned conventional charging method according to particle size.
第1に原料を炉中心部から炉壁に向かって装入するこ
とである。このために分配シュートの傾動角度を小から
大に順次増加するスケジュールを設定する。First, the raw material is charged from the center of the furnace toward the furnace wall. For this reason, a schedule is set in which the tilt angle of the distribution chute is sequentially increased from small to large.
第1図中に示す矢印が分配シュートの傾動角度の動き
を示している。このように分配シュートの傾動角度を従
来の大から小に順次減少するのではなく、小から大に順
次増加すれば、炉内装入後の原料の表面形状は平坦にな
り易くなる。The arrow shown in FIG. 1 indicates the movement of the tilt angle of the distribution chute. As described above, if the tilt angle of the distribution chute is not decreased from the large size to the small size in the related art, but is gradually increased from the small size to the large size, the surface shape of the raw material after the furnace interior is easily flattened.
第2に前記分配シュート傾動角度の運動方向の変更だ
けでは装入後の原料の表面形状を充分、平坦にはできな
いので、分配シュートの傾動角度、各傾動角度における
旋回数、下部ゲート弁開度のうちの少なくとも一つを制
御することを併用する。Secondly, since the surface shape of the raw material after charging cannot be made sufficiently flat only by changing the movement direction of the distribution chute tilt angle, the tilt angle of the distribution chute, the number of turns at each tilt angle, and the lower gate valve opening degree. Controlling at least one of the above.
なお、本発明において装入後の原料が「充分、平坦」
とは、装入後の原料の重心の移動距離が30cm以内である
ことをいうものとする。In the present invention, the raw material after charging is "sufficiently flat".
Means that the moving distance of the center of gravity of the raw material after charging is within 30 cm.
本発明者らは炉外に実物大模型を制作し、コークス層
の堆積角を種々変更し、細粒焼結鉱をコークス層の上に
装入して装入後の細粒焼結鉱の堆積重心位置と装入位置
間の距離を実測した。The present inventors produced a full-scale model outside the furnace, changed the deposition angle of the coke layer variously, charged the fine-grained sinter on the coke layer, and The distance between the center of gravity and the charging position was measured.
その結果を第2図に示す。同図より明らかな如く、コ
ークス層堆積角が20度を超えなければ、細粒焼結鉱の堆
積重心位置と装入位置間の距離を30cm以内に維持できる
ことが判明した。従って、装入後の原料の堆積角が20度
を超えないようにすれば、原料の表面形状は充分平坦と
みなすことができる。 原料の堆積角を0度にするため
には、分配シュートの傾動角度、各傾動角度における旋
回数を限定する必要があり、高炉の種々の目的に応じた
装入物分布制御を自在に実施することは困難である。そ
こで、本発明では0度を除き(0度を超え)20度を超え
ないようにすることで、「十分平坦な」形状をつくるの
である。The results are shown in FIG. As is clear from the figure, it was found that the distance between the center of gravity of the fine-grained ore and the charging position can be maintained within 30 cm as long as the coke layer deposition angle does not exceed 20 degrees. Therefore, if the deposition angle of the raw material after charging does not exceed 20 degrees, the surface shape of the raw material can be considered to be sufficiently flat. In order to set the deposition angle of the raw material to 0 degree, it is necessary to limit the tilt angle of the distribution chute and the number of turns in each tilt angle, and to freely control the distribution of the charge according to various purposes of the blast furnace. Is difficult. Therefore, in the present invention, a “sufficiently flat” shape is created by excluding 0 degrees (exceeding 0 degrees) and not exceeding 20 degrees.
なお、本発明のよる分割装入方法は、原料の粒径だけ
でなく、性状の異なる原料を分割して、炉内の所定位置
に装入する場合にも適用できることはいうまでもない。
ここで、「性状の異なる原料」における性状の一例とし
ては焼結鉱の塩基度が挙げられる。Needless to say, the divided charging method according to the present invention can be applied not only to the particle size of the raw material but also to dividing the raw material having different properties and charging the raw material at a predetermined position in the furnace.
Here, the basicity of sinter is mentioned as an example of the property in "raw materials with different properties".
すなわち、高炉操業においては、炉壁部に塩基度を上
昇させた焼結鉱を装入し、焼結鉱の高温性状を改善して
融着帯根部を安定に形成させ、荷下がりの安定化や溶銑
中Si濃度の低下を図ることがあるからである。That is, in blast furnace operation, sinter ore with increased basicity is charged into the furnace wall to improve the high-temperature properties of the sinter and form a cohesive zone root stably to stabilize unloading. This is because the Si concentration in the hot metal may be reduced.
また、本発明方法では分配シュートの傾動角度を順次
大きくしてゆくのであるが、これはいかに当業者といえ
ども容易に発明できるものではない。Further, in the method of the present invention, the tilt angle of the distribution chute is gradually increased, but this cannot be easily invented by any person skilled in the art.
すなわち、分配シュートの傾動角度を順次小さくして
ゆく従来法にあっては、分配シュート荷重および分配シ
ュート上の原料荷重によって生じるモーメントの方向
と、分配シュートの傾動方向が同一であるため、傾動モ
ータにかかる軸トルクが小さく、従って、モータの定格
トルク許容範囲内である。これに対し、分配シュートの
傾動角度を順次大きくしてゆく本発明方法では、分配シ
ュート荷重および分配シュート上の原料の荷重によって
生じるモーメントの方向と分配シュートの傾動方向が逆
である。従って傾動モータにかかる軸トルクが大きく、
モータの定格トルクを超えることが予想されたため、分
配シュートの傾動角度を順次大きくしてゆく本発明の如
き発明がなされていなかったのである。That is, in the conventional method in which the tilt angle of the distribution chute is gradually decreased, the direction of the moment generated by the distribution chute load and the raw material load on the distribution chute and the tilt direction of the distribution chute are the same. The shaft torque applied to the motor is small, and thus is within the rated torque allowable range of the motor. On the other hand, in the method of the present invention in which the tilt angle of the distribution chute is gradually increased, the direction of the moment generated by the distribution chute load and the load of the raw material on the distribution chute is opposite to the tilt direction of the distribution chute. Therefore, the axial torque applied to the tilt motor is large,
Since it was expected that the rated torque of the motor would be exceeded, the invention such as the present invention in which the tilt angle of the distribution chute was gradually increased was not made.
しかし、本発明をするにあたり、分配シュートの傾動
角度を順次大きくしてゆく場合のモータ軸の必要トルク
を実測したところ第3図に示すように従来のモータ容量
を20%程度増加すれば常用する分配シュート傾動角度範
囲において、分配シュートの傾動角度を順次大きくして
ゆけることが判明した。However, in carrying out the present invention, the required torque of the motor shaft was actually measured when the tilt angle of the distribution chute was gradually increased, and as shown in FIG. 3, it was normally used if the conventional motor capacity was increased by about 20%. It was found that the tilt angle of the distribution chute can be gradually increased within the tilt angle range of the distribution chute.
従って小額の投資で分配シュートの傾動角度を順次大
きくしてゆく本発明が実施できるのである。Therefore, the present invention can be implemented in which the tilt angle of the distribution chute is gradually increased with a small investment.
(作用) 本発明は、ベルレス式高炉の炉内所定位置に、粒径及
び/又は性状の異なる複数種類の鉄源及び/又は還元剤
を分割して装入する方法において、炉中心部から炉壁方
向に向かって前記原料を装入すべく分配シュートの傾動
角度を制御すると共に、装入後の原料表面の堆積角が0
度を超えかつ20度を超えないように前記分配シュートの
傾動角度、各傾動角度における旋回数、下部ゲート弁の
開度のうちの少なくとも一つを制御するものである為、
粒径及び/又は性状の異なる複数種類の鉄源及び/又は
還元剤を分割して高炉内の所定位置に装入する際に、装
入後の前記原料の半径方向及び/又は円周方向の堆積量
の分布の制御性が向上する。(Operation) The present invention is a method of dividing and charging a plurality of types of iron sources and / or reducing agents having different particle sizes and / or properties into predetermined positions in a furnace of a bellless blast furnace, and The tilt angle of the distribution chute is controlled to charge the raw material toward the wall, and the deposition angle of the raw material surface after charging is 0.
In order to control at least one of the tilt angle of the distribution chute, the number of turns in each tilt angle, and the opening degree of the lower gate valve so as not to exceed 20 degrees and more than 20 degrees,
When a plurality of types of iron sources and / or reducing agents having different particle diameters and / or properties are divided and charged at a predetermined position in the blast furnace, the raw material in the radial direction and / or the circumferential direction of the raw material after the charging is divided. The controllability of the distribution of the deposited amount is improved.
(実 施 例) 本発明の効果を確認するため、炉外において製作した
実物大模型を使用して装入物分布試験を実施した。試験
に使用した粒度別の鉄源および還元剤は実炉で使用して
いる粒度別の焼結鉱およびコークスである。また、試験
における原料の装入条件は、荷下がりがないことおよび
送風がないことを除けば、実炉と同一の条件である。ま
た、半径方向の細粒原料の堆積分布は装入前にサンプリ
ング袋を設置し、原料装入後にサンプリング袋をひきあ
げ、サンプリング袋中の細粒原料割合を測定して求め
た。(Actual Example) In order to confirm the effect of the present invention, a charge distribution test was conducted using a full-scale model manufactured outside the furnace. The iron source and reducing agent for each particle size used in the test are the sinter and coke for each particle size used in the actual furnace. In addition, the charging conditions of the raw materials in the test are the same as those of the actual furnace, except that there is no unloading and no blowing. Further, the deposition distribution of the fine-grain raw material in the radial direction was obtained by installing a sampling bag before charging, pulling up the sampling bag after charging the raw material, and measuring the proportion of the fine-grain raw material in the sampling bag.
試験結果を第4図に示す。従来の焼結鉱粒度別装入で
は、分配シュートの傾動角度のスケジュールは粗粒焼結
鉱に対し(3344556677)、細粒焼結鉱に対し(1112)で
実施した。ここで( )内は分配シュートの大きさと順
序を示しており、数字が小さい方が分配シュート傾動角
度を大きく設定してある。旋回数は粗粒焼結鉱で10旋
回、細粒焼結鉱で4旋回、焼結鉱トータルで14旋回であ
る。これに対して本発明による焼結鉱粒度別装入は次の
2つのケースについて実施した。ケース1は従来発明と
同じく炉壁部に細粒焼結鉱を装入する場合、ケース2は
本発明の特色を生かして、炉中間部に細焼結鉱を装入す
る場合である。ケース1の分配シュートの傾動角度のス
ケジュールは粗粒焼結鉱に対し(1099876543)、細粒焼
結鉱に対し(22111)とした。そして、ケース1では細
粒焼結鉱の使用量を従来発明より25%増加させた。ま
た、ケース2の分配シュートの傾動角度のスケジュール
は粗粒焼結鉱に対し(1099822111)、細粒焼結鉱に対し
(76543)とした。細粒焼結鉱の使用量は従来発明より2
5%増加させた。The test results are shown in FIG. In the conventional charging of sinter grain size, the tilt angle of the distribution chute was set to (3344556677) for coarse-grained sinter and (1112) for fine-grained sinter. Here, the size and order of the distribution chutes are shown in parentheses, and the smaller the number, the larger the tilt angle of the distribution chutes. The number of turns is 10 for coarse-grained ore, 4 for fine-grained ore, and 14 for total ore. On the other hand, the charging of the sintered ore according to the present invention was carried out for the following two cases. Case 1 is the case where the fine-grained sinter is charged into the furnace wall as in the case of the conventional invention, and Case 2 is the case where the fine-sintered ore is charged into the middle of the furnace by taking advantage of the features of the present invention. The tilt angles of the distribution chute in Case 1 were set to (1099876543) for coarse-grained ore and (22111) for fine-grained ore. In Case 1, the amount of fine-grained ore used was increased by 25% compared to the conventional invention. In addition, the schedule of the tilt angle of the distribution chute of case 2 was set to (1099822111) for coarse-grained ore and (76543) for fine-grained ore. The amount of fine-grained sinter used is 2 compared to the conventional invention
Increased by 5%.
なお、実物大模型では試験は行なわなかったが、ケー
ス2の装入法として、焼結鉱を3分割装入する方法もあ
る。即ち、粗粒焼結鉱を(10998)で装入後、下部ゲー
ト弁9および下部シール弁10を一旦閉操作し、直ちに下
部ゲート弁9′および下部シール弁10′を開操作して細
粒焼結鉱を(76543)で装入し、装入が完了すると下部
ゲート弁9′および下部シール弁10′を閉操作し、直ち
に下部ゲート弁9および下部シール弁10を開操作して粗
粒焼結鉱を(22111)で装入する方法である。Although the test was not conducted on the full-scale model, there is also a method of charging the sinter in three parts as a method of charging the case 2. That is, after charging the coarse-grained sinter with (10998), the lower gate valve 9 and the lower seal valve 10 were once closed, and immediately the lower gate valve 9'and the lower seal valve 10 'were opened to fine-grained. Sinter ore was charged with (76543), and when the charging was completed, the lower gate valve 9'and the lower seal valve 10 'were closed, and immediately the lower gate valve 9 and the lower seal valve 10 were opened to obtain coarse particles. This is a method of charging sinter with (22111).
第4図は半径方向の細粒焼結鉱の堆積分布を示すもの
であり、図中aは従来方法による粒度別装入を示すが、
細粒焼結鉱は炉壁部に装入されているものの、堆積して
いる半径方向の位置は広範囲にわたっている。一方bに
示す本発明によって細粒焼結鉱を炉壁部へ装入するケー
ス1では、細粒焼結鉱の使用量が増加しているにもかか
わらず、細粒焼結鉱の半径方向の堆積位置は、従来方法
よりも範囲は狭くなっている。つまり本発明によって高
炉内の所定の位置に高精度で所定の原料を装入すること
ができた。FIG. 4 shows the deposition distribution of the fine-grained sintered ore in the radial direction. In FIG. 4, a shows the charging according to the grain size by the conventional method.
Although the fine-grained sinter is charged into the furnace wall, the radial position where it is deposited is wide. On the other hand, in the case 1 in which the fine-grained sintered ore is charged into the furnace wall portion according to the present invention shown in b, the radial direction of the fine-grained sintered ore is increased even though the amount of the fine-grained sintered ore used is increased. The range of the deposition position of is smaller than that of the conventional method. That is, according to the present invention, it is possible to charge a predetermined raw material with high accuracy at a predetermined position in the blast furnace.
また第4図中cは従来方法では達成できなかった、炉
中間部への細粒焼結鉱の本発明による装入試験結果を示
す。本発明によって、炉中間部へも細粒原料を高精度で
装入できることが確認された。Further, c in FIG. 4 shows the result of the charging test according to the present invention of the fine-grained sintered ore into the middle part of the furnace, which could not be achieved by the conventional method. It was confirmed by the present invention that the fine-grain raw material can be charged into the middle part of the furnace with high accuracy.
次に、実物大模型を使用して塩基度2.0の焼結鉱65tを
炉壁部に、また、塩基度1.8の焼結鉱65tを中間部から中
心部に装入する分布試験を実施した。Next, using a full-scale model, a distribution test was carried out in which 65 tons of basicity 2.0 sinter ore and 65 tons of basicity 1.8 sinter were charged from the middle part to the center part.
試験結果を第5図に示す。従来法による分配シュート
の傾動角度のスケジュールは、塩基度1.8の焼結鉱に対
しては(4556677)とし、塩基度1.8の焼結鉱を前記スケ
ジュールで装入後、塩基度2.0の焼結鉱を(1112334)の
スケジュールで装入した。The test results are shown in FIG. The schedule of the tilt angle of the distribution chute according to the conventional method is (4556677) for the sinter having the basicity of 1.8, and after the sinter having the basicity of 1.8 is charged according to the above schedule, the sinter of the basicity of 2.0 is charged. Was charged on the schedule of (1112334).
そして、本発明によって炉壁部に精度よく塩基度2.0
の焼結鉱を装入するため、次の分配シュートの傾動角度
のスケジュールを採用した。まず塩基度1.8の焼結鉱を
(10998765)のスケジュールで中心部から順次中間部に
装入し、次に塩基度2.0の焼結鉱を(4322111)のスケジ
ュールで炉壁部に装入した。Further, according to the present invention, the basicity of the furnace wall portion can be 2.0 accurately.
The following schedule for the tilt angle of the distribution chute was adopted to charge the sintered ore of First, a sinter having a basicity of 1.8 was charged into the middle part in sequence from the central part on a schedule of (10998765), and then a sinter having a basicity of 2.0 was charged to the furnace wall part on a schedule of (4322111).
第5図は塩基度2.0の焼結鉱の半径方向の堆積状況を
示すものであり、図中aに示す従来法では塩基度2.0の
焼結鉱は、分割して炉壁部に装入したにもかかわらず、
塩基度1.8の焼結鉱装入時に形成される堆積斜面の影響
をうけて、半径方向の広範囲にわたって堆積している。
これに対して本発明では、塩基度1.8の焼結鉱装入時に
堆積斜面が形成されないので、塩基度2.0の焼結鉱の堆
積位置と塩基度1.8の焼結鉱の堆積位置との境界は極め
て明確であり、塩基度2.0の焼結鉱を半径方向の所定位
置に精度良く装入できることが確認された。Fig. 5 shows the state of radial accumulation of sinter having a basicity of 2.0. In the conventional method shown in a in the figure, the sinter having a basicity of 2.0 was divided and charged into the furnace wall. in spite of,
Deposited over a wide area in the radial direction under the influence of the sedimentary slope formed during the charging of a sinter with a basicity of 1.8.
On the other hand, in the present invention, since the sedimentary slope is not formed during the charging of the basic ore sinter of 1.8, the boundary between the basic ore 2.0 sinter and the basic 1.8 sinter is not defined. It was extremely clear, and it was confirmed that a sintered ore with a basicity of 2.0 could be charged accurately at a predetermined position in the radial direction.
(発明の効果) 以上説明したように本発明は、ベルレス式高炉の炉内
所定位置に、粒径及び/又は性状の異なる複数種類の鉄
源及び/又は還元剤を分割して装入する方法において、
炉中心部から炉壁方向に向かって前記原料を装入すべく
分配シュートの傾動角度を制御すると共に、装入後の原
料表面の堆積角が0度を超えかつ20度を超えないように
前記分配シュートの傾動角度、各傾動角度における旋回
数、下部ゲート弁の開度のうちの少なくとも一つを制御
するものである為、粒径及び/又は性状の異なる複数種
類の鉄源及び/又は還元剤を分割して高炉内の所定位置
に装入する際に、装入後の前記原料の半径方向及び/又
は円周方向の堆積量の分布の制御性が向上する。従っ
て、高炉の安定操業に大なる効果を有する。(Effects of the Invention) As described above, the present invention is a method of dividing and charging a plurality of types of iron sources and / or reducing agents having different particle sizes and / or properties at predetermined positions in the furnace of a bellless blast furnace. At
The tilt angle of the distribution chute is controlled so as to charge the raw material from the center of the furnace toward the furnace wall, and the deposition angle on the surface of the raw material after the charging exceeds 0 degrees and does not exceed 20 degrees. Since at least one of the tilt angle of the distribution chute, the number of turns at each tilt angle, and the opening degree of the lower gate valve is controlled, a plurality of types of iron sources and / or reductions having different particle sizes and / or properties When the agent is divided and charged into a predetermined position in the blast furnace, the controllability of the distribution of the deposited amount of the raw material after charging in the radial direction and / or the circumferential direction is improved. Therefore, it has a great effect on the stable operation of the blast furnace.
第1図は本発明方法の説明図、第2図はコークス層の堆
積角と細粒焼結鉱の装入後の移動距離との関係図、第3
図は分配シュートの傾動角度とモータ軸トルクとの関係
図、第4図は高炉中心からの距離と細粒焼結鉱割合との
関係図、第5図は高炉中心からの距離と塩基度2.0の焼
結鉱割合との関係図、第6図は従来方法の説明図であ
る。 1は高炉、3は粗粒原料、3′は細粒原料、9、9′は
下部ゲート弁、11は分配シュート。FIG. 1 is an explanatory view of the method of the present invention, FIG. 2 is a relationship diagram between a deposition angle of a coke layer and a moving distance after charging of fine-grained sintered ore, and FIG.
The figure shows the relationship between the tilt angle of the distribution chute and the motor shaft torque. Figure 4 shows the relationship between the distance from the blast furnace center and the fine-grained sinter ratio. Figure 5 shows the distance from the blast furnace center and basicity 2.0. FIG. 6 is an explanatory view of the conventional method, and FIG. 1 is a blast furnace, 3 is a coarse grain raw material, 3'is a fine grain raw material, 9 and 9'is a lower gate valve, and 11 is a distribution chute.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 網永 洋一 茨城県鹿島郡鹿島町大字光3番地 住友金 属工業株式会社鹿島製鉄所内 (56)参考文献 特開 昭50−74504(JP,A) 特開 昭52−66806(JP,A) 特開 昭56−47506(JP,A) 特開 昭60−208404(JP,A) ─────────────────────────────────────────────────── ─── Continuation of front page (72) Yoichi Aminaga Yoichi Amanaga, No. 3, Hikari, Kashima-cho, Kashima-cho, Kashima-gun, Ibaraki Sumitomo Metal Industries, Ltd. Kashima Works (56) Reference JP-A-50-74504 (JP, A) JP-A-52-66806 (JP, A) JP-A-56-47506 (JP, A) JP-A-60-208404 (JP, A)
Claims (1)
び/又は性状の異なる複数種類の鉄源及び/又は還元剤
を分割して装入する方法において、炉中心部から炉壁方
向に向かって前記原料を装入すべく分配シュートの傾動
角度を制御すると共に、装入後の原料表面の堆積角が0
度を超えかつ20度を超えないように前記分配シュートの
傾動角度、各傾動角度における旋回数、下部ゲート弁の
開度のうちの少なくとも一つを制御することを特徴とす
るベルレス式高炉の異種原料装入方法。1. A method of dividing and charging a plurality of types of iron sources and / or reducing agents having different particle sizes and / or properties into a predetermined position in a furnace of a bellless blast furnace, the furnace wall being located at the center of the furnace. The tilt angle of the distribution chute is controlled so as to charge the raw material toward the direction, and the deposition angle of the raw material surface after charging is 0.
Of at least one of the tilting angle of the distribution chute, the number of turns at each tilting angle, and the opening of the lower gate valve so as not to exceed 20 degrees and more than 20 degrees. Raw material charging method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61136449A JPH0811804B2 (en) | 1986-06-11 | 1986-06-11 | Charging method for different materials of bellless blast furnace |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61136449A JPH0811804B2 (en) | 1986-06-11 | 1986-06-11 | Charging method for different materials of bellless blast furnace |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62290810A JPS62290810A (en) | 1987-12-17 |
| JPH0811804B2 true JPH0811804B2 (en) | 1996-02-07 |
Family
ID=15175368
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61136449A Expired - Lifetime JPH0811804B2 (en) | 1986-06-11 | 1986-06-11 | Charging method for different materials of bellless blast furnace |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0811804B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2016053201A (en) * | 2014-09-04 | 2016-04-14 | Jfeスチール株式会社 | Blast furnace raw material charging method |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5266806A (en) * | 1975-09-01 | 1977-06-02 | Mitsubishi Electric Corp | Control device of rotating chute for blast furnace |
| JPS5647506A (en) * | 1979-09-28 | 1981-04-30 | Nippon Steel Corp | Controlling raw material charging into blast furnace |
-
1986
- 1986-06-11 JP JP61136449A patent/JPH0811804B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62290810A (en) | 1987-12-17 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |