JPH0156127B2 - - Google Patents
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- Publication number
- JPH0156127B2 JPH0156127B2 JP5321682A JP5321682A JPH0156127B2 JP H0156127 B2 JPH0156127 B2 JP H0156127B2 JP 5321682 A JP5321682 A JP 5321682A JP 5321682 A JP5321682 A JP 5321682A JP H0156127 B2 JPH0156127 B2 JP H0156127B2
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- Prior art keywords
- porosity
- raw material
- sintered
- ore
- pores
- 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
本発明は、製鉄用焼結鉱製造における焼結操業
方法に関するものである。
焼結鉱は、製鉄用溶鉱炉原料として広く用いら
れている。焼結鉱の品質を判断する基準として
は、化学成分、粒度分布、冷間強度、還元粉化性
等がある。これらは溶鉱炉操業にあたつてきわめ
て重要な因子となるので、不断の管理が行われて
いる。
ところで、焼結鉱成品気孔率は成品の品質に重
要な影響を及ぼすことが知られている。ここで、
焼結鉱成品気孔率とは、JISM8716−1977の規定
にもとづいて測定されたものをいう。
さて、焼結鉱冷間強度TI(%)は、焼結鉱中の
気孔が強度欠陥となり、焼結鉱成品気孔率が高い
方が強度は低下する。一方、焼結鉱の還元反応
は、還元ガスとの接触によつて進行するので、反
応表面積の大きい、即ち焼結鉱成品気孔率の高い
方が被還元性は良好となる。還元粉化性RDI(%)
については、焼結鉱成品気孔率が高い方が還元が
進行しかつ強度的に弱いので悪くなる傾向があ
る。これらの関係を第1図に示す。
従来の焼結操業法は、焼結鉱成品気孔率の測定
を迅速に行うことが不可能であるので、焼結鉱成
品気孔率を把握せずに、直接製造した成品の品質
試験を実施し、満足すべき品質値を得るまで、原
料配合比または操業諸条件(焼結ブロワーの回転
数、風箱ダンパ開度、カツトオフ・プレートの角
度、原料層高、サージホツパ内の原料の含水率)
の変更を繰り返さなければならなかつた。したが
つて、品質目標値を得るまでに、膨大な時間を必
要とするばかりではなく、むだな原料配合や焼結
鉱製造を行わざるをえなかつた。このために、成
品品質のバラツキも大きくなる。
したがつて、本発明の目的は、焼結鉱成品気孔
率を迅速に推定することによつて焼結操業の合理
化と焼結鉱成品の品質の安定化を図ることにあ
る。
次に、第2図を参照して本発明の方法について
説明する。まず、原料充填層内の直径0.5mm以下
の気孔率を求める(1)。同時に、焼結層内の流動性
指数を求める(2)。次いで、これらの気孔率および
流動性指数にもとづいて焼結鉱成品気孔率を推定
する(3)。この推定気孔率から目標気孔率を得るよ
うに、原料配合比を制御するか(4)、または操業諸
条件を制御する(5)。
焼結ケーキ中の気孔を分類すると、所定粒度の
焼結鉱を得るために破砕したときに成品粒子見掛
表面を形成し破砕過程においては消滅する大きな
径の気孔と、焼結鉱成品中に残りJISM8716法に
より計測される小さな径の気孔に分類することが
できる。これら気孔を寸法別に分類するとすれ
ば、JISの測定法が水銀を用いていることから水
銀の浸透力で決まり、およそ0.5mmを境として分
類することができる。
さて、実際の焼結鉱製造にあつては原料を充填
した状態において種々の気孔が存在し、これらの
中にも径の大きなものと小さなものがあるが、焼
結鉱はその製造過程で鉱石粒子が溶融し、その融
液が流動冷却し鉱石間を結合させる。これを気孔
の側から表現すると、鉱石粒子が溶融し、融液が
流動化することによつて小さな気孔が集まり、よ
り大きな気孔が発生するようになるといえる。そ
して、この結果として焼結層全体の収縮が生じ
る。このように焼結層が溶融するにつれて、気孔
の小さなものが大きなものに統合され、見掛上気
孔サイズは大きく成長していく。
本発明者等はこれら気孔の変化に注目し、これ
ら気孔の変化を以下の方法により予測することが
可能であることを見い出した。焼結鉱成品気孔率
は初期の原料充填状態で存在する小さな気孔の
内、焼結溶融過程で消滅せずに残つた小さな気孔
であり、これは焼結充填層の固液相流動性によつ
て、次の(1)式のように求めることができる。
ε=ε′−ε′η ……(1)
ε:焼結鉱成品気孔率(%)
ε′:初期(焼成前)原料充填層の直径0.5mm以下
の気孔率(%)
η:焼結層内溶融時の流動性指数。
ここで、初期の小さな気孔であるが、これには
概ね次の3つに分類することができる。第3図に
示すように、原料充填層6において鉱石粒子内気
孔7、粒子間の空隙気孔のうち小さな空隙8すな
わち微粉によつて取囲まれ形成されているもの、
水によつて占められている部分9(原料の状態で
は空隙気孔ではないが焼成過程で水分が蒸発し気
孔となる。また、水は小さく入り混んでいるので
小さな気孔を発生させる。)があげられる。これ
らの量は、次の(2)〜(7)式によつて求められる。
ε3=w・ρ1 ……(2)
E=100−ε3−(100−w)・ρ1/ρ2 ……(3)
ε1=0.01×(100−E)×
〓i
(AiWi) ……(4)
ε2=R・E・(R0.5) ……(5)
ε0=ε1+ε2+ε3 ……(6)
ε′={ε0/(100−E+ε2)}×100 ……(7)
ε0:初期(焼成前)原料充填層の直径0.5mm以下
の気孔率(容器体積当り%)
ε′:初期(焼成前)原料充填層の直径0.5mm以下
の気孔率(直径0.5mm以下の空隙を除く容器体
積当り%)
E:原料充填時の全粒子間空隙気孔率(容器体積
当り%)
ε1:鉱石粒子内気孔率(容器体積当り%)
ε2:原料充填層の直径0.5mm以下の気孔率(容器
体積当り%)
ε3:水の占めている体積率(容器体積当り%)
ρ1:充填層の嵩密度(g/cm3)
ρ2:鉱石粒子の平均見掛密度(g/cm3)
Ai:銘柄鉱石の粒子内気孔率(粒子体積当り%)
Wi:銘柄鉱石の配合比(−)
R0.5:原料鉱石粒度分布中の0.5mm以下の比率%)
R:定数
w:原料中の含水分重量百分率(wt%)
(2)式は原料含水分重量百分率および原料充填嵩
密度から容器体積当りの水の占める体積率を計算
する。(3)式は原料充填層の全粒子間空隙気孔率を
原料含水分重量成分率、原料充填嵩密度および粒
子見掛密度から計算する。(4)式は粒子内気孔率を
積算し容器体積当りに換算する。(5)式は原料充填
層の全粒子間空隙気孔率から原料粒度分布を用い
て原料充填層中の直径0.5mm以下の粒子間空隙気
孔率を求める。(6)式は初期の状態で原料充填層内
に存在する直径5mm以下の気孔を積算し求める。
(7)式は、初期原料充填気孔率を、JIS法で示され
ている気孔率の意味に従つて容器体積当り%から
0.5mm以上の気孔を除く部分の体積当り%に換算
しなおす式である。なお、(5)式に関しε2とEと
R0.5との関係を第4図に示す。第4図中、×印は
R0.5=75%の場合、●印はR0.5=50%の場合、〇
印はR0.5=25%の場合をそれぞれ示す。
一方、焼結層の固体・液体を含めた流動性を表
わす指数ηは実測の焼結ケーキ収縮率または原料
化学成分および溶融率から求めることができる。
ここで、溶融率とは、後に詳述するが、一般に焼
結鉱製造過程中で溶融した履歴をもつものの焼結
ケーキ中の体積比率と定義する。これを(8)、(9)式
に示す。
η=a1SR+a2E+a3 ……(8)
η=b1Q+b2〔CaO〕+b3〔SiO2〕+b4〔Al2O3〕+b5
〔MgO〕+b4〔FeO〕……(9)
SR:焼結ケーキの収縮率(焼結後の層高/焼結
前の層高)×100(%)
E:原料充填時の全粒子間空隙気孔率(容器体積
当り%)
〔 〕:〔 〕内記号で表わした原料中の成分
(wt%)
Q:焼結層内原料粒子溶融率(%)
a1〜a3:定数
b1〜b6:定数
前述したように、焼結層内の流動性は焼結層全
体の収縮に大きな影響を及ぼし密接なる関係をも
つており、逆に焼結ケーキの収縮率を実測するこ
とにより焼結層内での流動性を求めることができ
る。
(8)式においてEの項が入つているのは充填層初
期粒子間空隙も焼結ケーキ収縮に大きな影響をも
つているので補正するためである。さて、焼結ケ
ーキ収縮率は焼成前後の層高を計測することによ
り簡単かつ迅速に、また、原料充填時の全粒子間
空隙気孔率は予め測定した原料粒子密度の演算、
水分計で測定した原料含水分率および原料装入重
量を容器体積で除した原料充填層嵩密度等の値か
ら精度よく算出することができる。
本発明者等は、流動性指数ηは(8)式とは別に溶
融率と原料化学成分値からも求めることができる
ことを見い出し、先に出願した特願昭56−133499
号に示した。すなわち、本発明者等は、実験の結
果、焼結鉱製造中の鉱石粒子の溶融現象は1100℃
以上になると、原料中のCaOが反応を起し、カル
シウム・フエライトを形成し、初期溶融液をつく
り、この溶融液が逐次鉱石粒子の外周から内側に
向かつて侵食するように溶融を進行させる反応で
あることを見い出した。
したがつて、1100℃以上の保持時間tと配合原
料の溶融率Qとは次の(10)式で表される。さらに、
1100℃以上で保持時間6分間の場合における配合
原料の溶融率は、各単味鉱石銘柄別の溶融率qj
(1100℃以上6分間)を加重平均することによつ
て(11)式のように表される。
Q=・(t/6)n ……(10)
=
〓j
(qj・wj) ……(11)
ただし、
t:1100℃以上保持時間(分)
n:定数
j:原料の各種銘柄を示すインデツクス
qj:鉱石銘柄jにおける溶融率(気孔、空隙部を
除く)
wj:配合原料中の鉱石銘柄jの体積配合率
単味鉱石銘柄別の1100℃以上で保持時間6分の
場合の溶融率qjは原料入荷時に実験室で試験的に
求めることができる。その測定結果の一例を第1
表に示す。
The present invention relates to a sintering operation method for producing sintered ore for iron manufacturing. Sintered ore is widely used as a raw material for blast furnaces for iron manufacturing. Criteria for determining the quality of sintered ore include chemical composition, particle size distribution, cold strength, reduction pulverizability, etc. These are extremely important factors when operating a blast furnace, so they are constantly managed. By the way, it is known that the porosity of sintered mineral products has an important effect on the quality of the product. here,
The sintered mineral porosity refers to the porosity measured based on the provisions of JISM8716-1977. Now, regarding the sintered ore cold strength TI (%), the pores in the sintered ore become strength defects, and the higher the porosity of the sintered ore product, the lower the strength. On the other hand, since the reduction reaction of sintered ore proceeds through contact with reducing gas, the greater the reaction surface area, that is, the higher the porosity of the sintered ore product, the better its reducibility will be. Reduction pulverizability RDI (%)
As for sintered mineral products with higher porosity, reduction progresses and the strength is weaker, so they tend to be worse. These relationships are shown in FIG. With conventional sintering operation methods, it is impossible to quickly measure the porosity of sintered ore products, so quality tests are conducted on directly manufactured products without knowing the porosity of sintered ore products. , until a satisfactory quality value is obtained, the raw material mixture ratio or operational conditions (sintering blower rotation speed, wind box damper opening, cut-off plate angle, raw material layer height, moisture content of raw material in the surge hopper)
I had to repeat the changes. Therefore, it not only takes a huge amount of time to obtain the quality target value, but also requires wasteful mixing of raw materials and manufacturing of sintered ore. This also increases the variation in product quality. Therefore, an object of the present invention is to streamline sintering operations and stabilize the quality of sintered mineral products by quickly estimating the porosity of sintered mineral products. Next, the method of the present invention will be explained with reference to FIG. First, determine the porosity of the raw material packed bed with a diameter of 0.5 mm or less (1). At the same time, the fluidity index within the sintered layer is determined (2). Next, the porosity of the sintered ore product is estimated based on these porosity and fluidity index (3). The blending ratio of raw materials is controlled (4) or the operating conditions are controlled so as to obtain the target porosity from this estimated porosity (5). The pores in the sintered cake can be classified into large-diameter pores that form the apparent surface of the product particles when crushed to obtain sintered ore of a predetermined particle size, but disappear during the crushing process, and The remaining pores can be classified into small diameter pores measured by the JISM8716 method. If these pores were to be classified by size, since the JIS measurement method uses mercury, it is determined by the penetrating power of mercury, and it is possible to classify them based on the limit of approximately 0.5 mm. Now, in the actual production of sintered ore, various pores exist in the state filled with raw materials, and some of these pores are large in diameter and some are small in diameter, but sintered ore is produced during the production process. The particles are melted, and the melt flows and cools, bonding the ores together. Expressing this from the pore side, it can be said that as the ore particles melt and the melt fluidizes, small pores gather and larger pores are generated. As a result, the entire sintered layer shrinks. As the sintered layer melts in this way, smaller pores are integrated into larger ones, and the apparent pore size grows larger. The present inventors paid attention to changes in these pores and found that these changes in pores can be predicted by the following method. The porosity of sintered ore products is the small pores that remain during the sintering and melting process among the small pores that exist in the initial raw material filling state, and this is due to the solid-liquid phase fluidity of the sintered packed bed. Therefore, it can be calculated as shown in equation (1) below. ε=ε′−ε′η ……(1) ε: Porosity of sintered mineral product (%) ε′: Porosity of the initial (before firing) raw material packed bed with a diameter of 0.5 mm or less (%) η: Sintered Fluidity index during interlayer melting. Here, the initial small pores can be roughly classified into the following three types. As shown in FIG. 3, in the raw material packed bed 6, pores 7 within the ore particles, small pores 8 among the pores between the particles, ie those surrounded by fine powder,
Portion 9 occupied by water (in the raw material state, it is not a void pore, but during the firing process, water evaporates and becomes a pore. Also, since water is small and crowded, small pores are generated). It will be done. These quantities are determined by the following equations (2) to (7). ε 3 = w・ρ 1 …(2) E=100−ε 3 −(100−w)・ρ 1 /ρ 2 …(3) ε 1 =0.01×(100−E)× 〓 i (AiWi ) ……(4) ε 2 = R・E・(R 0.5 ) ……(5) ε 0 = ε 1 + ε 2 + ε 3 ……(6) ε′={ε 0 / (100−E+ε 2 )} ×100 ……(7) ε 0 : Porosity of the initial (before firing) raw material packed bed with a diameter of 0.5 mm or less (% per container volume) ε′: Pores with a diameter of 0.5 mm or less of the initial (before firing) raw material packed bed (% per container volume excluding voids with a diameter of 0.5 mm or less) E: Porosity of all interparticle voids when filling raw materials (% per container volume) ε 1 : Porosity within ore particles (% per container volume) ε 2 : Porosity of the raw material packed bed with a diameter of 0.5 mm or less (% per container volume) ε 3 : Volume ratio occupied by water (% per container volume) ρ 1 : Bulk density of the packed bed (g/cm 3 ) ρ 2 : Average apparent density of ore particles (g/ cm3 ) Ai: Intra-particle porosity of branded ore (% per particle volume) Wi: Mixing ratio of branded ore (-) R 0.5 : 0.5 mm or less in the particle size distribution of raw ore R: Constant w: Weight percentage of water content in the raw material (wt%) Equation (2) calculates the volume ratio of water per container volume from the weight percentage of water content of the raw material and the bulk density of the raw material. Equation (3) calculates the porosity of all interparticle voids in the raw material packed bed from the water content weight component ratio of the raw material, the packed bulk density of the raw material, and the apparent density of the particles. Equation (4) integrates the intraparticle porosity and converts it per container volume. Equation (5) calculates the porosity of interparticle voids with a diameter of 0.5 mm or less in the raw material packed bed using the raw material particle size distribution from the porosity of all interparticle voids in the raw material packed bed. Equation (6) is calculated by integrating the pores with a diameter of 5 mm or less that exist in the raw material packed bed in the initial state.
Equation (7) calculates the initial raw material filling porosity from % per container volume according to the meaning of porosity shown in the JIS method.
This is a formula that converts it back to % per volume excluding pores of 0.5 mm or larger. Regarding equation (5), ε 2 and E
The relationship with R 0.5 is shown in Figure 4. In Figure 4, the x mark is
When R 0.5 = 75%, the ● mark indicates the case when R 0.5 = 50%, and the ○ mark indicates the case when R 0.5 = 25%. On the other hand, the index η representing the fluidity of the sintered layer including solid and liquid can be determined from the actually measured shrinkage rate of the sintered cake or the chemical composition of the raw material and the melting rate.
Here, the melting rate will be described in detail later, but is generally defined as the volume ratio in the sintered cake of something that has a history of melting during the sintered ore manufacturing process. This is shown in equations (8) and (9). η=a 1 SR+a 2 E+a 3 ...(8) η=b 1 Q+b 2 [CaO]+b 3 [SiO 2 ]+b 4 [Al 2 O 3 ]+b 5
[MgO] + b 4 [FeO]...(9) SR: Shrinkage rate of sintered cake (layer height after sintering/layer height before sintering) x 100 (%) E: Between all particles when filling raw materials Void porosity (% per container volume) [ ]: Components in the raw material (wt%) represented by symbols in [ ] Q: Melt rate of raw material particles in the sintered layer (%) a 1 ~ a 3 : Constant b 1 ~ b 6 : Constant As mentioned above, the fluidity within the sintered layer has a great influence on the shrinkage of the entire sintered layer and is closely related to it.Conversely, by actually measuring the shrinkage rate of the sintered cake, it is possible to Fluidity within the stratum can be determined. The term E is included in equation (8) to compensate for the fact that the initial interparticle voids in the packed bed also have a large effect on the shrinkage of the sintered cake. Now, the shrinkage rate of the sintered cake can be easily and quickly determined by measuring the layer height before and after firing, and the porosity of all the interparticles when filling the raw material can be determined by calculating the density of the raw material particles measured in advance.
It can be accurately calculated from values such as the moisture content of the raw material measured with a moisture meter and the bulk density of the raw material packed bed obtained by dividing the weight of the raw material charged by the container volume. The present inventors discovered that the fluidity index η can also be determined from the melting rate and the raw material chemical composition values, in addition to equation (8).
Shown in No. That is, as a result of experiments, the present inventors found that the melting phenomenon of ore particles during the production of sintered ore occurs at 1100℃.
At this point, CaO in the raw material reacts to form calcium ferrite, creating an initial melt, and the melt progresses as the melt gradually erodes from the outer periphery of the ore particles inward. I found that. Therefore, the holding time t at 1100° C. or higher and the melting rate Q of the blended raw materials are expressed by the following equation (10). moreover,
The melting rate of the blended raw materials when held at 1100℃ or higher for 6 minutes is the melting rate qj of each single ore brand.
(1100°C or higher for 6 minutes) is expressed as equation (11) by taking a weighted average. Q=・(t/6)n ……(10) = 〓 j (qj・wj) ……(11) Where, t: Holding time over 1100℃ (minutes) n: Constant j: Indicates various brands of raw materials Index qj: Melting rate for ore brand j (excluding pores and voids) wj: Volume proportion of ore brand j in the blended raw materials Melting rate qj for each single ore brand when held at 1100℃ or higher for 6 minutes can be determined experimentally in the laboratory when raw materials arrive. An example of the measurement results is shown in the first section.
Shown in the table.
【表】【table】
【表】
以上要約すれば、本発明の方法は予め測定した
原料諸物性値(R0.5、Ai、ρ2)、原料配合比wi、
含水分率w、充填嵩密度ρ1から初期の直径0.5mm
以下の気孔率ε′を求め、次いで焼結ケーキ収縮率
SRの実測または層内原料成分、溶融率Qの予測
から焼結層内の流動性指数ηを求め、これらの値
から焼結鉱成品気孔率εを算出し、この値が目標
値になるように原料配合比または操業諸条件を制
御する。
次に、第5図に示すDL型焼結機に本発明の方
法を適用した実施例について説明する。
実施例 1
本実施例は、原料配合比を自由にしておき、推
定焼結鉱成品気孔率(ε)を目標値になるように
操業諸条件を制御した。
DL型焼結機10の焼成ブロワ12の回転数、
風箱ダンパ13、カツトオフ・プレート14の角
度(原料層高)、サージ・ホツパ15内の原料の
含水分率を選び操業を制御した。
この操業結果を第6図および第7図に示す。第
6図は(1)式〜(7)式により焼結鉱成品気孔率εを求
め、操業諸条件を制御した結果を示す。第7図は
(1)式〜(7)式及び(9)式とから焼結鉱成品気孔率εを
求め、操業諸条件を制御した結果を示す。いずれ
の場合にも精度の高い制御結果が得られているこ
とがわかる。
実施例 2
本実施例では、操業諸条件を一定とし、推定焼
結鉱成品気孔率εを目標値になるように原料配合
比を制御した。
第2表に示す原料諸物性をもとに、推定焼結鉱
成品気孔率εが目標値になるように鉱石Dおよび
E、石灰石、粉コークス、返鉱の配合比を決定
し、焼結操業を実施した。
この操業結果を第8図に示す。さらに、従来法
と本発明法との比較を第3表に示す。この場合も
精度の高い操業結果が得られ、成品品質のばらつ
きが低減されていることがわかる。[Table] To summarize above, the method of the present invention uses pre-measured raw material physical property values (R 0.5 , Ai, ρ 2 ), raw material blending ratio wi,
Moisture content w, filling bulk density ρ 1 to initial diameter 0.5mm
Find the following porosity ε′, then the sintered cake shrinkage rate
The fluidity index η in the sintered layer is determined from the actual measurement of SR or the prediction of the raw material composition in the layer and the melting rate Q. From these values, the sintered ore product porosity ε is calculated, and this value is set to the target value. The raw material blending ratio or operating conditions are controlled accordingly. Next, an example in which the method of the present invention is applied to the DL type sintering machine shown in FIG. 5 will be described. Example 1 In this example, the raw material blending ratio was set freely, and the operating conditions were controlled so that the estimated sintered ore product porosity (ε) reached the target value. The rotation speed of the sintering blower 12 of the DL type sintering machine 10,
The operation was controlled by selecting the wind box damper 13, the angle (raw material layer height) of the cut-off plate 14, and the moisture content of the material in the surge hopper 15. The results of this operation are shown in FIGS. 6 and 7. FIG. 6 shows the results of determining the porosity ε of the sintered mineral product using equations (1) to (7) and controlling the operating conditions. Figure 7 is
The porosity ε of the sintered ore product was calculated from equations (1) to (7) and equation (9), and the results of controlling the operating conditions are shown. It can be seen that highly accurate control results are obtained in both cases. Example 2 In this example, the operating conditions were kept constant and the raw material blending ratio was controlled so that the estimated sintered ore product porosity ε was at the target value. Based on the physical properties of the raw materials shown in Table 2, the blending ratio of ores D and E, limestone, coke breeze, and return ore is determined so that the estimated sintered ore product porosity ε becomes the target value, and the sintering operation is started. was carried out. The results of this operation are shown in Figure 8. Furthermore, Table 3 shows a comparison between the conventional method and the method of the present invention. It can be seen that in this case as well, highly accurate operation results were obtained and variations in product quality were reduced.
【表】【table】
【表】【table】
第1図は焼結鉱成品気孔率と焼結鉱品質との関
係を示すグラフ。第2図は本発明の方法を示す工
程線図。第3図は原料充填層の縦断面図。第4図
は原料充填層内の空隙全気孔と小気孔との関係を
示すグラフ。第5図は本発明の方法が適用される
DL型焼結機の概略構成図。第6図は本発明の方
法の実施例を示すグラフ。第7図は第6図と同様
なグラフ。第8図は本発明の方法の別の実施例を
示すグラフ。
10:DL型焼結機、12:焼結ブロワ、1
3:風箱ダンパ、14:カツトオフ・プレート、
15:サージ・ホツパ。
FIG. 1 is a graph showing the relationship between sintered ore product porosity and sintered ore quality. FIG. 2 is a process diagram showing the method of the present invention. FIG. 3 is a longitudinal cross-sectional view of the raw material packed bed. FIG. 4 is a graph showing the relationship between all pores and small pores in the raw material packed bed. Figure 5 shows the method of the present invention being applied.
Schematic diagram of the DL type sintering machine. FIG. 6 is a graph showing an embodiment of the method of the present invention. Figure 7 is a graph similar to Figure 6. FIG. 8 is a graph showing another embodiment of the method of the present invention. 10: DL type sintering machine, 12: Sintering blower, 1
3: Wind box damper, 14: Cut-off plate,
15: Sarge Hotupa.
Claims (1)
直径0.5mm以下の気孔率を求めること、焼結層内
の流動性指数を求めること、前記気孔率および流
動性指数にもとづいて焼結鉱成品気孔率を推定す
ること、該推定気孔率から目標気孔率を得るよう
に原料配合比、焼成ブロワーの回転数、風箱ダン
パ開度、カツトオフ・プレートの角度、原料層
高、またはサージ・ホツパ内の原料の含水率を制
御することからなる焼結操業方法。1. In the manufacturing process of sintered ore, the porosity of the raw material packed bed with a diameter of 0.5 mm or less is determined, the fluidity index of the sintered bed is determined, and the sintered ore is determined based on the porosity and fluidity index. Estimate the porosity of the finished product, and adjust the raw material blend ratio, firing blower rotation speed, wind box damper opening, cut-off plate angle, raw material layer height, or surge hopper so as to obtain the target porosity from the estimated porosity. A sintering operation method consisting of controlling the moisture content of the raw materials within.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5321682A JPS58171532A (en) | 1982-03-31 | 1982-03-31 | Operating method of sintering |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5321682A JPS58171532A (en) | 1982-03-31 | 1982-03-31 | Operating method of sintering |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58171532A JPS58171532A (en) | 1983-10-08 |
| JPH0156127B2 true JPH0156127B2 (en) | 1989-11-29 |
Family
ID=12936632
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5321682A Granted JPS58171532A (en) | 1982-03-31 | 1982-03-31 | Operating method of sintering |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58171532A (en) |
-
1982
- 1982-03-31 JP JP5321682A patent/JPS58171532A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58171532A (en) | 1983-10-08 |
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