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JP2889088B2 - Blast furnace operation method - Google Patents
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JP2889088B2 - Blast furnace operation method - Google Patents

Blast furnace operation method

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Publication number
JP2889088B2
JP2889088B2 JP19187593A JP19187593A JP2889088B2 JP 2889088 B2 JP2889088 B2 JP 2889088B2 JP 19187593 A JP19187593 A JP 19187593A JP 19187593 A JP19187593 A JP 19187593A JP 2889088 B2 JP2889088 B2 JP 2889088B2
Authority
JP
Japan
Prior art keywords
furnace
blast furnace
amount
tuyere
iron source
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 - Fee Related
Application number
JP19187593A
Other languages
Japanese (ja)
Other versions
JPH0718311A (en
Inventor
忍 森本
宗之 樋口
徹三 芳我
芳幸 松岡
正義 高尾
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
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Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP19187593A priority Critical patent/JP2889088B2/en
Publication of JPH0718311A publication Critical patent/JPH0718311A/en
Application granted granted Critical
Publication of JP2889088B2 publication Critical patent/JP2889088B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は安定した高炉の操業を行
う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 operating a stable blast furnace.

【0002】[0002]

【従来の技術】高炉々内には、炉頂部から焼結鉱、鉄鉱
石、ペレット等の鉄源とコークスを交互に層状に装入
し、高炉炉下部のボッシュ部に設けた羽口から高温の空
気(熱風)を吹込んでいる。この熱風により、羽口先部
分に生じたレースウェーでコークスが燃焼して、高温の
還元ガスが発生する。そして、この発生した高温還元ガ
スはボッシュ部から炉頂に向かって上昇する。炉内を上
昇する高温還元ガスは前記炉頂部から装入した上記鉄源
とコークス等の原料と向流接触することにより、該鉄源
は加熱及び還元反応を受けつつ炉内を降下する。
2. Description of the Related Art In a blast furnace, iron sources such as sinter, iron ore, and pellets and coke are charged alternately in layers from the top of the furnace. The air (hot air) is blown. This hot air causes coke to burn on the raceway generated at the tuyere tip, generating high-temperature reducing gas. Then, the generated high-temperature reducing gas rises from the Bosch portion toward the furnace top. The high-temperature reducing gas ascending in the furnace comes in countercurrent contact with the iron source charged from the furnace top and a raw material such as coke, so that the iron source descends in the furnace while undergoing a heating and reduction reaction.

【0003】次いで、この鉄源は炉下部の高温域で軟
化、融着して融着帯を形成する。更に、この高温域では
この融着帯が溶融滴下し、銑鉄とスラグとに分離して高
炉々底の湯溜部に溜まる。この湯溜部に溜まった銑鉄と
スラグを定期的又は連続的に出銑口から炉外に抽出する
ものである。
Next, the iron source softens and fuses in a high temperature region at the lower part of the furnace to form a cohesive zone. Further, in this high temperature range, the cohesive zone melts and drops, and is separated into pig iron and slag and stored in the basin at the bottom of each blast furnace. The pig iron and slag accumulated in the basin are extracted regularly or continuously from the taphole to the outside of the furnace.

【0004】このような高炉に於いて、低燃料比で安定
した高炉の操業を行うために従来より、例えば特公昭5
7−51443号公報で提案のように、高炉々壁の円周
方向及び高さ方向のおける温度分布、または炉壁の熱負
荷分布を測定することにより前記融着帯の形状、位置を
検知し、その融着帯を操業状態に合った形状、位置に制
御する方法が一般的に行われている。
[0004] In such a blast furnace, in order to operate the blast furnace stably with a low fuel ratio, a conventional blast furnace has been used, for example, in Japanese Patent Publication No. Sho.
As proposed in Japanese Patent Application Laid-Open No. 7-51443, the shape and position of the cohesive zone are detected by measuring the temperature distribution in the circumferential and height directions of the blast furnace walls or the heat load distribution of the furnace wall. In general, a method of controlling the cohesive zone to a shape and a position suitable for the operation state is generally performed.

【0005】[0005]

【発明が解決しようとする課題】しかし、この融着帯の
形状、位置を制御する方法は通常操業の場合は非常に有
効な手段であるが、操業変動時(休風立ち上げ時、増産
移行時、減産移行時等)は有効に対応できないものであ
る。即ち、この融着帯の制御は、主として、炉内に装入
する装入物の装入分布を調整して、炉内ガス流分布を変
更することによって行われることから、その変化速度は
緩やかである。このため、前記操業状態に合った融着帯
に造り込むまでには長時間を有するものであった。
However, the method of controlling the shape and position of the cohesive zone is a very effective means in the case of normal operation. Time, transition to reduced production, etc.) cannot be handled effectively. That is, since the control of the cohesive zone is mainly performed by adjusting the charging distribution of the charging materials to be charged into the furnace and changing the gas flow distribution in the furnace, the rate of change is moderate. It is. For this reason, it takes a long time to build a cohesive zone suitable for the above-mentioned operating condition.

【0006】しかして、高炉において操業変動がある
と、前記融着帯をその変動した操業状態に適した形状、
位置に早急に造り込むことが、生産性良く、且つ、低燃
料比で高炉を操業する上で重要である。しかし、融着帯
の形状、位置は千差万別に変化することから、この変化
する状態に対応して、それに適した操業状態にすること
は困難であることから、融着帯の形状、位置の組み合せ
を数個に区分し、この区分を基に装入物の装入分布を調
整しており、調整制御が粗いものであった。
[0006] Thus, when there is a fluctuation in the operation of the blast furnace, the cohesive zone is formed in a shape suitable for the fluctuated operation state.
It is important to quickly build the blast furnace at the position in order to operate the blast furnace with good productivity and low fuel ratio. However, since the shape and position of the cohesive zone vary widely, it is difficult to achieve an operating state suitable for the changing state. Was divided into several parts, and the charging distribution of the charged materials was adjusted based on this classification, and the adjustment control was coarse.

【0007】本発明は、高炉において操業変動があった
場合、短時間で、且つ、精度良く、その変動に応じた炉
況にすることにより、生産性良く、低燃料比で高炉を操
業する事を課題とするものである。
The present invention provides a method for operating a blast furnace with good productivity and a low fuel ratio by setting the furnace condition according to the fluctuation in a short time and with high accuracy when there is a fluctuation in the operation of the blast furnace. Is the subject.

【0008】[0008]

【課題を解決するための手段】本発明は上記課題を解決
するためになされたものであり、その手段1は炉頂部か
ら焼結鉱、鉄鉱石、ペレット等の鉄源とコークスを交互
に装入し、且つ、炉下部の羽口から熱風を吹き込みつつ
高炉を操業する方法において、前記炉頂部からの鉄源投
入量から決まる炉内装入鉄源の平均層厚、前記羽口先に
おける温度、ボッシュ部におけるガス量の1つ、又は、
複数を調整して下記(1)式で求まる値を16〜20に
維持する高炉の操業方法である。
Means for Solving the Problems The present invention has been made to solve the above-mentioned problems. Means 1 is to alternately load iron sources such as sintered ore, iron ore, pellets and coke from the furnace top. And operating the blast furnace while blowing hot air from the tuyere at the bottom of the furnace, wherein the average layer thickness of the furnace interior iron source determined from the amount of iron source charged from the furnace top, the temperature at the tuyere tip, Bosch One of the gas volumes in the part, or
This is a method for operating a blast furnace in which a plurality is adjusted to maintain the value obtained by the following equation (1) at 16 to 20.

【0009】K・Tf・WBG/TO ・・・(1) 但し、Tf:羽口先温度(℃)、WBG:ボッシュガス量
(Nm3 /分)、TO :炉内装入鉄源の平均層厚(m
m)、K:高炉の送風羽口からストックラインまでの高
炉内容積(実行内容積)の逆数。
K · Tf · W BG / T O (1) where Tf: tuyere temperature (° C.), W BG : amount of Bosch gas (Nm 3 / min), T O : source of iron in furnace interior Average layer thickness (m
m), K: Reciprocal of the blast furnace internal volume (execution internal volume) from the blast furnace tuyere to the stock line.

【0010】なお、前記炉内装入鉄源の平均層厚TO
(1チャージの鉄源装入重量×比重)/(高炉の炉腹部
の横断面積)から求めたものである。また、前記羽口先
温度Tfは羽口先に生じるレースウェーの温度であり、
これは送風量VB、送風湿分量VBH2O 、酸素富化量O
2 、微粉炭吹込み量PC、送風温度TBを制御因子とす
るものであって、特別な式を使用することなく公知の
式、例えば、下式(a)で求めることができる。 Tf=1559+0.84×TB−6.0×VBH2O
4972×(O2 /VB)−K1 ×PC・・・(a) 但し、K1 :微粉炭の銘柄により変わる発熱係数であ
る。
The average layer thickness T O of the iron source inside the furnace is obtained from (weight of iron source charged per charge × specific gravity) / (cross-sectional area of the abdomen of the blast furnace). The tuyere tip temperature Tf is the temperature of the raceway generated at the tuyere tip,
This is the amount of blown air VB, the amount of blown moisture VB H2O , the amount of oxygen enrichment O
2. The pulverized coal injection amount PC and the blowing temperature TB are used as control factors, and can be obtained by a known formula, for example, the following formula (a) without using a special formula. Tf = 1559 + 0.84 × TB−6.0 × VB H2O +
4972 × (O 2 / VB) −K 1 × PC (a) where K 1 is a heat generation coefficient that varies depending on the brand of pulverized coal.

【0011】更に、ボッシュガス量WBGはボッシュ部を
上昇するガス量であり、これは送風量VB、酸素富化量
2 、送風湿分VBH2O 、富化酸素湿分OH2O 、吹込み
微粉炭湿分PCH2O 、微粉炭中の窒素分PCN2と水素分
PCH2と酸素分PCO2、装入コークス中の窒素分CN2
制御因子とするものであって、特別な式を使用すること
なく公知の式、例えば、下式(b)で求めることができ
る。 WBG=2VB+2O2 +(VB*VBH2O +O2 *O
H2O +PC*PCH2O )*(22.4/18)+PCN2
*VB*(22.4/28)+PCH2*VB*(22.
4/2)+PCO2*VB*(22.4/16)・・・
(b)
Further, the Bosch gas amount W BG is a gas amount that rises in the Bosch portion, which is the blowing amount VB, the oxygen enriched amount O 2 , the blowing humidity VB H2O , the enriched oxygen humidity O H2O , Controlling factors are pulverized coal moisture PC H2O , nitrogen content PC N2 , hydrogen content PC H2 and oxygen content PC O2 in pulverized coal, and nitrogen content C N2 in charged coke. It can be obtained by a known formula, for example, the following formula (b) without performing the above. W BG = 2VB + 2O 2 + (VB * VB H2O + O 2 * O
H2O + PC * PC H2O ) * (22.4 / 18) + PC N2
* VB * (22.4 / 28) + PC H2 * VB * (22.4 / 28)
4/2) + PC O2 * VB * (22.4 / 16)
(B)

【0012】本発明者は安定した高炉操業を行うため
に、種々実験・検討した結果、上記(1)式で求めた値
(以下M値と称する)に着目し、例えば、減産移行時
は、送風量・富化酸素量を減じるため、炉下部から持ち
込まれる溶融還元能力(羽口先温度Tf×ボッシュガス
量WBG)は低下し、高炉々頂から装入鉄源量、即ち、平
均層厚TO が一定ならばM値は低下する。このままの状
態で操業すると、減産移行後、1〜2ヶ月は持ちこたえ
ているが、その後、炉下部・炉芯が不活性となり、炉状
況が悪化することが殆どであることが判明した。これは
炉内装入鉄源の平均層厚が前記溶融還元能力に対して過
大のため、鉄源の溶融還元が遅れ、融着帯根部が肥大化
して垂れ下がり通気性悪化、荷下がり悪化、炉芯の汚れ
(炉芯内に溶銑、スラグが混在している現象)に繋がり
炉況不調の原因となるものと推察される。
The present inventor has conducted various experiments and studies in order to carry out stable blast furnace operation. As a result, the present inventors focused on the value (hereinafter referred to as M value) obtained by the above equation (1). In order to reduce the amount of air blown and the amount of enriched oxygen, the smelting reduction capability (tuyere temperature Tf × Bosch gas amount W BG ) brought in from the lower part of the furnace decreases, and the amount of iron source charged from the blast furnace tops, that is, the average layer thickness if T O is constant M value is reduced. It was found that if the operation was continued in this state, the furnace had held for one to two months after the shift to reduced production, but then the lower part of the furnace and the wick became inactive, and the furnace condition was mostly deteriorated. This is because the average layer thickness of the furnace interior iron source is excessively large with respect to the smelting reduction ability, so that the smelting reduction of the iron source is delayed, the root of the cohesive zone becomes large and sags, air permeability deteriorates, unloading deteriorates, It is presumed that this leads to contamination of the furnace core (a phenomenon in which hot metal and slag coexist in the furnace core) and causes a furnace condition malfunction.

【0013】一方、増産時になると、送風量及び/又は
酸素富化量を増加し、燃料比を低減して、その分鉄源の
装入量を増加することで対応しているが、この結果、炉
内装入鉄源の平均層厚TO が前記溶融還元能力に対し少
なくなり過ぎて炉体熱負荷上昇、通気性悪化、荷下がり
が悪化するものと推察される。又、燃料比低減を指向し
た操業時は、1チャージのコークス量を低減して、鉄源
量を増加する結果、前記同様に炉内溶融還元能力に対し
て炉内装入鉄源の平均層厚が極端に大きくなりソリュー
ションロスカーボン(SLC)が上昇すると共に水素利
用率ηH2 が低下し、炉下部が不活性となり炉況が悪化
する。更に、特に、M値が低下している局面で休風を行
い、その休風立ち上がりにおいて、鉄源の平均層厚が極
端に厚いと、炉内への熱風の入り状態が悪く、溶融還元
能力が大幅に低下することから、上記M値が大幅に低下
する結果、炉況は元の安定した状態に戻らず炉況不調を
惹起させるものと推察される。
On the other hand, when the production is increased, the amount of air blown and / or the amount of oxygen enrichment is increased, the fuel ratio is reduced, and the amount of iron source charged is increased. It is presumed that the average layer thickness T O of the furnace interior iron source becomes too small with respect to the smelting reduction ability, and that the furnace body heat load rises, air permeability deteriorates, and unloading deteriorates. Also, when the operation is aimed at reducing the fuel ratio, the amount of coke per charge is reduced and the amount of iron source is increased. Becomes extremely large, the solution loss carbon (SLC) increases, the hydrogen utilization rate ηH 2 decreases, the lower part of the furnace becomes inactive, and the furnace condition deteriorates. Furthermore, especially when the M value is decreasing, the wind is stopped, and when the average layer thickness of the iron source is extremely thick at the start of the wind, the state of hot air entering the furnace is poor, and the smelting reduction ability is reduced. It is supposed that the reactor value does not return to the original stable state and causes a reactor condition malfunction because the M value greatly decreases.

【0014】このように、減産・増産・休風立上時等の
操業変動があった場合に関わらず、通常の操業状態にお
いても安定した状態で高炉の操業を行うためには、適正
M値を見つける必要がある。このため、本発明者は図1
に示す様に、高炉炉内の装入物のスリップとM値との関
係を調査した。この結果、M値が16未満、又は、20
を越えると装入物のスリップ回数が急激に増加すること
が判明した。更に、図2に示すように、炉内の水素ガス
利用率ηH2 と上記M値の関係を調査した結果、M値が
16未満になると急激に水素ガス利用率ηH2 が低下す
ることが判明した。
As described above, in order to operate the blast furnace in a stable state even in the normal operation state regardless of the fluctuations in the operation such as when the production is reduced, increased, or when the wind is shut off, an appropriate M value is required. Need to find out. For this reason, the inventor of FIG.
As shown in the figure, the relationship between the slip of the charge in the blast furnace and the M value was investigated. As a result, the M value is less than 16 or 20
It was found that the number of slips of the charge increased sharply when exceeding. Further, as shown in FIG. 2, as a result of investigating the relationship between the hydrogen gas utilization rate ηH 2 in the furnace and the above M value, it was found that when the M value was less than 16, the hydrogen gas utilization rate ηH 2 rapidly decreased. did.

【0015】この結果、M値を16〜20に維持するこ
とが、操業変動があった際にも、経済的に、しかも、早
急に安定した炉況にすることができることを見出した。
そして、このM値を16〜20に維持するために、前記
(1)式に示すように炉内に装入する鉄源の平均層厚、
ボッシュガス量、羽口先温度を単独又は複合して調整す
るものである。そして、この調整のための具体的手段と
しては、上記(a)式、(b)式で示した制御因子を用
いるものである。
As a result, it has been found that maintaining the M value at 16 to 20 makes it possible to quickly and economically stabilize the furnace condition even when there is a fluctuation in the operation.
Then, in order to maintain the M value at 16 to 20, the average layer thickness of the iron source charged into the furnace as shown in the above equation (1),
The amount of Bosch gas and the temperature of the tuyere are adjusted individually or in combination. As a specific means for this adjustment, the control factors shown in the above equations (a) and (b) are used.

【0016】[0016]

【実施例】本発明の実施例を表1を参照して詳細に説明
する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Embodiments of the present invention will be described in detail with reference to Table 1.

【0017】[0017]

【表1】 [Table 1]

【0018】本例は有効内容積が5245m3 、送風羽
口からストックラインまでの実行内容積が4312m3
(前記K=2.3×10-4)で、羽口から110kg/
t−pigの微粉炭を吹込んでいる高炉に適用した例で
ある。
In this embodiment, the effective internal volume is 5245 m 3 , and the effective internal volume from the tuyere to the stock line is 4312 m 3.
(K = 2.3 × 10 −4 ) and 110 kg /
This is an example in which the invention is applied to a blast furnace in which t-pig pulverized coal is blown.

【0019】実施例1は通常の操業状態において、M値
が15となって炉況が不安定となったので送風温度を1
50℃高くし、羽口先温度を上昇させM値を17として
操業することにより、ソリューションロスカーボン(S
LC)が10kg/t−pig低減して炉内の還元反応
が良好となり、かつ、水素利用率が4%向上して炉況が
安定し、燃料比が低下した例である。
In the first embodiment, the M value was 15 and the furnace condition became unstable in a normal operation state.
By increasing the tuyere temperature by 50 ° C and raising the M value to 17, the solution loss carbon (S
This is an example in which LC) was reduced by 10 kg / t-pig, the reduction reaction in the furnace became good, and the hydrogen utilization was improved by 4%, the furnace condition was stabilized, and the fuel ratio was lowered.

【0020】実施例2はM値が15.2となり炉況が不
安定となったため、1チャージの鉄源量を低減し、更
に、1チャージのコークス量を低減すると共に送風量及
び酸素富化量を増加し、且つ、鉄源炉内平均層厚を20
mm薄くすると共にボッシュガス量を増加し、羽口先温
度を高くすることにより、M値を19.5として操業す
ることにより、ソリューションロスカーボン(SLC)
が10kg/t−pig低減し、更に、水素利用率が4
%向上して炉況が安定し、燃料比が10Kg低減した例
である。
In Example 2, since the M value was 15.2 and the furnace condition became unstable, the amount of iron source for one charge was reduced, the amount of coke for one charge was reduced, and the air flow and oxygen enrichment were reduced. And increase the average layer thickness in the iron source furnace to 20
The solution loss carbon (SLC) can be obtained by operating the M value at 19.5 by reducing the thickness and increasing the amount of Bosch gas and increasing the tuyere temperature.
Is reduced by 10 kg / t-pig, and the hydrogen utilization rate is
This is an example in which the furnace condition is stabilized by improving the fuel ratio by 10% and the fuel ratio is reduced by 10 kg.

【0021】実施例3はM値が24.5と高くなり炉況
が不安定となったため、1チャージの鉄源量を増加して
鉄源炉内平均層厚を70mm厚くし、M値を20として
操業することにより、実施例2同様にソリューションロ
スカーボン(SLC)及び水素利用率が向上して、炉況
が安定した例である。
In Example 3, since the M value was increased to 24.5 and the furnace condition became unstable, the amount of iron source per charge was increased to increase the average layer thickness in the iron source furnace by 70 mm, and the M value was increased. 20 is an example in which the solution loss carbon (SLC) and hydrogen utilization rates are improved and the furnace condition is stabilized as in the second embodiment.

【0022】実施例4はM値が15.3と低くなり炉況
が不安定となったため、送風量を増加してボッシュガス
量を増加することにより、M値を19.1として操業し
た結果、炉況が安定した例である。
In Example 4, since the M value was reduced to 15.3 and the furnace condition became unstable, the operation was carried out with the M value set to 19.1 by increasing the air supply and the Bosch gas amount. This is an example where the furnace condition is stable.

【0023】実施例5は休風立ち上げ途中を示すもので
あり、この休風立ち上げ途中でM値が10.9と低くな
り炉況が不安定になったので、酸素富化量を3000N
3/H増加し、羽口先温度を高くすると共にボッシュ
ガス量を増加することにより、M値を16として操業す
ることにより炉況が安定化し、短時間にして立ち上げを
完了できた例である。
Example 5 shows the process during the start-up of the calm. The M value was reduced to 10.9 during the start-up of the calm, and the furnace condition became unstable.
By increasing m 3 / H, raising the tuyere tip temperature and increasing the amount of Bosch gas, the furnace condition was stabilized by operating at an M value of 16, and startup was completed in a short time. is there.

【0024】[0024]

【発明の効果】本発明により、高炉に操業変動があった
場合、短時間で、且つ、精度良く、その変動に応じた高
炉々況を早期に造り込んで安定した炉況を維持する事が
できるので、生産性良く、低燃料比で高炉を操業するこ
とが可能となる等の多大な効果を奏するものである。
According to the present invention, when there is a fluctuation in the operation of the blast furnace, the blast furnace conditions corresponding to the fluctuation can be quickly and accurately produced in a short time to maintain a stable furnace condition. As a result, it is possible to operate the blast furnace with high productivity at a low fuel ratio, and to achieve a great effect.

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

【図1】M値とスリップ回数の関係を示した図FIG. 1 is a diagram showing a relationship between an M value and the number of slips.

【図2】M値と水素ガス利用率の関係を示した図FIG. 2 is a diagram showing a relationship between an M value and a hydrogen gas utilization rate.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 松岡 芳幸 大分県大分市大字西ノ洲1番地 新日本 製鐵株式会社 大分製鐵所内 (72)発明者 高尾 正義 大分県大分市大字西ノ洲1番地 新日本 製鐵株式会社 大分製鐵所内 (58)調査した分野(Int.Cl.6,DB名) C21B 5/00 ──────────────────────────────────────────────────の Continuing on the front page (72) Inventor Yoshiyuki Matsuoka Oita, Oita City, Oishi Nishi-no-su, 1 Nippon Steel Corporation Inside Oita Works (72) Inventor Masayoshi Takao 1, Oita-shi, Oita, Oita, Oaza Nishi-no-su New Japan (58) Investigated field (Int. Cl. 6 , DB name) C21B 5/00

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 炉頂部から焼結鉱、鉄鉱石、ペレット等
の鉄源とコークスを交互に装入し、且つ、炉下部の羽口
から熱風を吹き込みつつ高炉を操業する方法において、
前記炉頂部から装入する鉄源量から決まる鉄源の平均層
厚、前記羽口先における温度、ボッシュ部におけるガス
量の1つ、又は、複数を調整して下式で求まる値を16
〜20に維持することを特徴とする高炉の操業方法。 K・Tf・WBG/TO 但し、Tf:羽口温度、WBG:ボッシュガス量、TO
炉内装入鉄源の平均層厚、K:高炉の送風羽口からスト
ックラインまでの高炉内容積の逆数。
A method of operating a blast furnace while alternately charging coke and iron sources such as sinter, iron ore, and pellets from a furnace top, and blowing hot air from a tuyere at a lower part of the furnace.
By adjusting one or more of the average layer thickness of the iron source determined from the amount of the iron source charged from the furnace top, the temperature at the tuyere tip, and the gas amount at the Bosch section, the value obtained by the following equation is 16
A method of operating a blast furnace, wherein the method is maintained at -20. K · Tf · W BG / T O, where Tf: tuyere temperature, W BG : amount of Bosch gas, T O :
Average layer thickness of furnace internal iron source, K: reciprocal of blast furnace internal volume from blast furnace tuyere to stock line.
JP19187593A 1993-07-07 1993-07-07 Blast furnace operation method Expired - Fee Related JP2889088B2 (en)

Priority Applications (1)

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JP19187593A JP2889088B2 (en) 1993-07-07 1993-07-07 Blast furnace operation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19187593A JP2889088B2 (en) 1993-07-07 1993-07-07 Blast furnace operation method

Publications (2)

Publication Number Publication Date
JPH0718311A JPH0718311A (en) 1995-01-20
JP2889088B2 true JP2889088B2 (en) 1999-05-10

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JP (1) JP2889088B2 (en)

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JP5971165B2 (en) * 2012-07-12 2016-08-17 Jfeスチール株式会社 Blast furnace operation method

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