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JPS6210284B2 - - Google Patents
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JPS6210284B2 - - Google Patents

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Publication number
JPS6210284B2
JPS6210284B2 JP2859383A JP2859383A JPS6210284B2 JP S6210284 B2 JPS6210284 B2 JP S6210284B2 JP 2859383 A JP2859383 A JP 2859383A JP 2859383 A JP2859383 A JP 2859383A JP S6210284 B2 JPS6210284 B2 JP S6210284B2
Authority
JP
Japan
Prior art keywords
blowing
converter
tuyere
line
furnace
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP2859383A
Other languages
Japanese (ja)
Other versions
JPS59157212A (en
Inventor
Nobuo Harada
Yoshihide Kato
Tsutomu Nozaki
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
JFE Steel Corp
Original Assignee
Kawasaki Steel Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Kawasaki Steel Corp filed Critical Kawasaki Steel Corp
Priority to JP2859383A priority Critical patent/JPS59157212A/en
Publication of JPS59157212A publication Critical patent/JPS59157212A/en
Publication of JPS6210284B2 publication Critical patent/JPS6210284B2/ja
Granted legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21CPROCESSING OF PIG-IRON, e.g. REFINING, MANUFACTURE OF WROUGHT-IRON OR STEEL; TREATMENT IN MOLTEN STATE OF FERROUS ALLOYS
    • C21C5/00Manufacture of carbon-steel, e.g. plain mild steel, medium carbon steel or cast steel or stainless steel
    • C21C5/28Manufacture of steel in the converter
    • C21C5/30Regulating or controlling the blowing
    • C21C5/35Blowing from above and through the bath

Landscapes

  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Manufacturing & Machinery (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)

Description

【発明の詳細な説明】 本発明は上底吹き転炉、または底吹転炉の底吹
き羽口を合理的に配設した、底吹き機能を持つ転
炉に関するものである。 底吹き機能を有する転炉は、吹錬中炉内装入物
が激しく撹拌されるため、製鋼精錬の際にはスラ
グ中の鉄分濃度(T.Fe)がLD転炉に比較して著
しく低くなり鉄歩留りが向上する利点があり、こ
れに加えて特に低炭域での脱炭速度も高く、さら
に脱硫能にも優れるなどの長所がある。 しかし、底吹き羽口から吹込まれたガスは前述
のように鋼浴を激しく撹拌するため、鋼浴に一定
周期の大きな振動を引き起こす。そのため一般に
第1図に示すような底吹き専用転炉では、鋼浴の
振動により転炉全体が大きく同期振動することを
防止するめ、転炉の支持機構に各種の振動防止対
策が講じられている。 一方、従来の純酸素上吹き転炉においては鋼浴
全体の周期的な振動は殆ど生じないから、純酸素
上吹き転炉製鋼用の既存の多くの転炉では、転炉
自体の振動について底吹き専用転炉の場合ほどに
は大きな考慮が払われた設計がなされていない。
そのため既存の上吹き転炉をそのまま底吹き転炉
に改造して純酸素底吹き転炉として用いた場合、
転炉自体が大きく振動して操業が不安定となると
ともに、支持機構が転炉の大きな振動に堪えられ
ずに破損したり、または早期に劣化して重大な事
故に至るおそれがある。これを防止するためには
転炉の支持機構をも改造すれば良いが、その改造
は極めて大がかりとなつてコストが著しく嵩み、
底吹き転炉を最初から製造する場合とコスト的に
は余り変らないこととなり、既存の上吹き転炉を
改造することによる経済的メリツトが失なわれて
しまう。これらの理由から従来は既存の上吹き転
炉を改造して底吹き転炉とすることは殆ど行われ
ておらず、そのため底吹き転炉の長所は認識され
ていながら、底吹き転炉に転換することは遅々と
して進んでいなかつたのが実状である。 さらに底吹き転炉においては、底吹きガスによ
る鋼浴の周期的な大振動によつて、吹錬中の溶鉄
が出鋼口から流出したり、サブランスプローブが
損傷するなどの問題もあつた。 また一方、第2図に示すように既存の上吹き転
炉に底吹き転炉の長所を取入れるため、上吹きラ
ンスからの吹込みと底吹き羽口からの吹込みとを
併用する上底吹き転炉製鋼も試られている。この
場合底吹き羽口からの吹込みガス流量は純底吹き
転炉の場合と比較しかなり少ないため、鋼浴の振
動も小さい。しかしながら上吹き転炉と比較すれ
ば鋼浴の周期的振動は相当に大きく、従つて転炉
もかなり振動するから、程度の差はあれ、前記同
様の問題がある。 底吹き機能を持つ転炉はまた周期的な振動によ
り炉底れんがが損耗し、その結果耐火物原単価が
上昇するという欠点がある。 本発明は底吹き機能を持つ転炉の振動、すなわ
ち鋼浴振動を、底吹き羽口の配列を適正にするこ
とによつて抑制し、耐火物コストを低減し、既存
の上吹き転炉を底吹き転炉や上底吹き転炉に容易
に改造して底吹き機能を持たせることができるよ
うにするための方策を提供することを目的とする
ものである。 本発明者らは底吹き機能を持つ転炉の炉内撹拌
効果を減退させることなく鋼浴振動を減少させ、
炉体振動の低減を図るべく開発研究に当つた。 本発明はいわゆる転炉の水モデルを用いて、底
吹き羽口の配列が浴の振動強度に大きく影響する
という因果関係を実験により確かめ、これをもと
にホツトモデル実炉の測定結果から完成されたも
のである。 水モデル実験について次に説明する。 80トン底吹き転炉の1/10相当の縮少水モデルに
おいて透明アクリル製モデル水槽内に生じる浴の
振動挙動を測定した。第3図に示した炉底径Dが
365mmの水槽底壁に数本の噴気管を一定の炉底直
径線と平行な線上に配設し、上吹き153/
min、底吹き51/minの同時吹込みを行つた。 水槽底壁の噴気管の配設は、底壁のある一定の
直径線に平行でその直径線からの水平距離がl2
ある2本の線上に、最大配列領域L1,L2、非配
列領域l1に配置し、モデル槽内に生じる振動強度
を測定した。L1,L2,l1,l2を種々変化させて試
験を行つた。また、同様の羽口配列を用いて炉内
撹拌強度の目安となる浴内の均一混合時間も併せ
て測定し、第1表に示す結果を得た。 この基礎実験の結果、 L1/Dが0.38〜0.80 l1/Dが0.19〜0.58 L2/Dが0.28〜0.69 ならびに、 l2/Dが0.025〜0.30 となる場合に振動強度が小さく、かつ撹拌能は減
退しないことが発見された。 第1表より、鋼浴振動強度は、羽口配置位置を
炉心から遠ざけるほど小さくなることが明らかで
ある。 一方、浴の撹拌強度の目安となる均一混合時間
は、 L2/Dが0.73以上の場合にはいずれも20sec
以上であり撹拌能は良くない。 L2/Dが0.69以下の場合、l2/Dの値が0.01
の場合やl2/Dの値が0.35の場合においても撹
拌能は良くない。 前記L2/Dが0.69以下で、かつl2/Dが0.025
〜0.30の場合に優れた撹拌能を示す。これは上
吹きランスからのガスジエツトと底吹き羽口か
らのガスジエツトとの干渉効果により撹拌能が
助長されたからと推定される。 次に5t上底吹き実験転炉における実施例を示
す。第2図に示す炉底径が1000mmの炉底壁1を脱
着自在とし、前記L1,L2およびl1,l2の値が種々
に異なるように底吹き羽口2をカセツト式として
差し変えを行つた。この底吹き羽口2は、内径8
mmφの2重管羽口を用いて底吹き酸素量は
5.0Nm3/minとし、また上吹きランス3による上
吹き酸素量を7.5Nm3/minに定め、試験吹錬を行
つた。 吹錬スタート後、第4図に示す方法で鋼浴の均
一混合時間を側定した。鋼浴の均一混合時間は長
くても1〜2分であるので連続的なサンプリング
による方法で鋼浴の濃度変化を調べるのは困難で
ある。よつて、異なつた場所で同時にサンプリン
グを行つてトレーサーを添加してからサンプリン
グした時刻で均一か否かの判定をして均一混合時
間を求めた。 トレーサーとして太さ1mmのCu線を用い、試
料採取は第5図に示す幅wが450mmで3個のボン
ブ8からなるサンプラー7によつて行つた。第6
図にその測定例を示す。第6図は横軸にトレーサ
ー添加後の時間を取り、縦軸はCu添加前の鋼中
Cu濃度をCuo、時間tにおける鋼中Cu濃度を
Cut、完全混合後の鋼中Cu濃度をCufとし、(Cut
―Cuo)/(Cuf―Cuo)の値をとつてある。 また、同時に各吹錬後における炉底のれんが損
耗量も測定した。 各試験吹錬の結果を L1/Dが0.38〜0.80 l1/Dが0.19〜0.58 L2/Dが0.28〜0.69 の場合について、l2/Dが均一混合時間および炉
底れんが損耗量に及ぼす影響を第7図に示した。 また、l2/Dが0.025〜0.30の範囲について、
L1/Dが均一混合時間および炉底れんが損耗量
にもたらす傾向を第8図に示した。 まず、第7図のl2/Dの変動に伴なう均一混合
時間の推移をみると、 l2/D=0、すなわち底吹き羽口2を炉底の
直径上に沿つて配列したとき均一混合時間は約
40秒である。 l2/Dを0.025〜0.30に偏心させると均一混合
時間は約22〜26秒の値を示す。 l2/Dが0.30を越え0.35に至ると均一混合時
間は約40〜42秒と長くなる。 一方炉底れんが損耗量については、 (イ) l2/D=0のとき約5mm/ヒートと大きい値
を示す。 (ロ) l2/Dが0.025を越え0.30に至る間は約2〜3
mm/ヒートと急減する。 (ハ) l2/Dが0.30を越え0.35の間においてもほぼ
一定値を示した。 次に、第8図によれば、L1/Dが均一混合時
間および炉底れんが損耗量に及ぼす影響は、
L1/Dが0.38〜0.80の範囲において均一混合時間
が小さく、かつ炉底れんが損耗量も小さいことが
確認された。 以上の確認実験の結果、上述の水モデル実験の
制振成積が、実炉操業にほぼそのまま反映され、
第2図に示すような元来胴長のLD転炉に底吹き
機能を付加した場合においてすら、炉体振動の有
効な低減が本発明によつて確実にもたらされ得る
ことが験証されたのである。 従つて、本発明の底吹き羽口配列を採用するこ
とによつて、底吹き転炉において激しい振動に耐
えるための支持架構および基礎を簡略化すること
が可能となつた。また本発明によつて、LD転炉
に底吹き機能を付加する第2図のような場合に、
上底吹き吹錬のために従来必要とされた支持架構
の補強が事実上不要となつた。 本発明は以上のように、転炉の振動抑制に著し
い卓効を奏し、また炉体および炉低れんがの損耗
を著しく低減させる効果を併せもたらすものであ
る。 【表】
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a top-bottom blowing converter or a bottom-blowing converter having a bottom-blowing function in which the bottom-blowing tuyeres of the converter are rationally arranged. In a converter with a bottom-blowing function, the contents inside the furnace are vigorously stirred during blowing, so during steelmaking and refining, the iron concentration (T.Fe) in the slag is significantly lower than in an LD converter. It has the advantage of improving iron yield, and in addition, has a high decarburization rate especially in the low coal range, and also has excellent desulfurization ability. However, the gas blown in from the bottom blowing tuyeres violently agitates the steel bath as described above, causing large vibrations in the steel bath at a constant period. Therefore, in a bottom-blowing converter as shown in Figure 1, various anti-vibration measures are taken in the support mechanism of the converter in order to prevent the entire converter from undergoing large synchronous vibrations due to vibrations in the steel bath. . On the other hand, in conventional pure oxygen top-blown converters, there is almost no periodic vibration of the entire steel bath. Not as much consideration has been given to the design as in the case of blow-only converters.
Therefore, if an existing top-blowing converter is converted into a bottom-blowing converter and used as a pure oxygen bottom-blowing converter,
The converter itself vibrates greatly, making operation unstable, and the support mechanism may not be able to withstand the large vibrations of the converter and may be damaged or deteriorate early, leading to a serious accident. In order to prevent this, it would be possible to modify the support mechanism of the converter, but such modification would be extremely large-scale and the cost would increase significantly.
The cost is not much different from manufacturing a bottom-blown converter from scratch, and the economic benefits of modifying an existing top-blowing converter are lost. For these reasons, conventionally, existing top-blown converters have rarely been modified to become bottom-blown converters, and although the advantages of bottom-blowing converters are recognized, conversion to bottom-blowing converters has been difficult. The reality is that progress has been slow. Furthermore, in bottom-blown converters, there were problems such as molten iron being blown flowing out of the tapping port and damage to the sub-lance probe due to large periodic vibrations in the steel bath caused by bottom-blowing gas. . On the other hand, as shown in Figure 2, in order to incorporate the advantages of a bottom-blowing converter into an existing top-blowing converter, a top-bottomed converter that uses a combination of blowing from the top-blowing lance and blowing from the bottom-blowing tuyere. Blown converter steelmaking is also being tried. In this case, the flow rate of the blown gas from the bottom-blowing tuyeres is considerably smaller than in the case of a pure bottom-blowing converter, so the vibration of the steel bath is also small. However, compared to a top-blown converter, the periodic vibration of the steel bath is considerably large, and the converter also vibrates considerably, so there are problems similar to those described above, albeit to a different degree. A converter with a bottom-blowing function also has the disadvantage that the bottom bricks are worn out due to periodic vibrations, resulting in an increase in the unit cost of refractories. The present invention suppresses the vibration of a converter with a bottom-blowing function, that is, the steel bath vibration, by optimizing the arrangement of bottom-blowing tuyeres, reduces the cost of refractories, and reduces the cost of existing top-blowing converters. The object of the present invention is to provide a measure for easily modifying a bottom-blowing converter or a top-bottom blowing converter to provide a bottom-blowing function. The present inventors reduced the steel bath vibration without reducing the in-furnace stirring effect of a converter with a bottom-blowing function.
We conducted development research to reduce furnace body vibration. The present invention uses a so-called converter water model to confirm through experiments the causal relationship that the arrangement of bottom blowing tuyere greatly affects the vibration intensity of the bath. It is something that The water model experiment will be explained next. The vibration behavior of the bath generated in a transparent acrylic model water tank was measured in a reduced water model equivalent to 1/10 of an 80-ton bottom-blown converter. The furnace bottom diameter D shown in Figure 3 is
Several fumarole pipes are arranged on the bottom wall of the 365 mm water tank on a line parallel to the constant diameter line of the bottom of the furnace, and the top blowing 153/
Simultaneous blowing was carried out at a rate of 51/min and bottom blowing at 51/min. The fumarole pipes on the bottom wall of the aquarium are arranged on two lines that are parallel to a certain diameter line of the bottom wall and whose horizontal distance from the diameter line is l 2 , with the maximum arrangement areas L 1 , L 2 , non- It was placed in the array area l1 , and the vibration intensity generated in the model tank was measured. Tests were conducted with various changes in L 1 , L 2 , l 1 , and l 2 . Furthermore, using the same tuyere arrangement, the uniform mixing time in the bath, which is a measure of the stirring intensity in the furnace, was also measured, and the results shown in Table 1 were obtained. As a result of this basic experiment, the vibration intensity is small when L 1 /D is 0.38 to 0.80, l 1 /D is 0.19 to 0.58, L 2 /D is 0.28 to 0.69, and l 2 /D is 0.025 to 0.30. It was discovered that the stirring capacity was not reduced. From Table 1, it is clear that the steel bath vibration intensity decreases as the tuyere arrangement position moves away from the core. On the other hand, the uniform mixing time, which is a guideline for the stirring strength of the bath, is 20 seconds when L 2 /D is 0.73 or more.
This is the above, and the stirring ability is not good. If L 2 /D is 0.69 or less, the value of l 2 /D is 0.01
Even when the value of l 2 /D is 0.35, the stirring performance is not good. The above L 2 /D is 0.69 or less, and l 2 /D is 0.025
-0.30 shows excellent stirring ability. This is presumed to be due to the interference effect between the gas jet from the top blowing lance and the gas jet from the bottom blowing tuyere, which promoted the stirring ability. Next, an example of a 5t top-bottom blowing experimental converter will be shown. The furnace bottom wall 1 with a furnace bottom diameter of 1000 mm as shown in Fig. 2 is made removable, and the bottom blowing tuyere 2 is installed as a cassette type so that the values of L 1 , L 2 and l 1 , l 2 are different. I made a change. This bottom blowing tuyere 2 has an inner diameter of 8
The amount of bottom-blown oxygen using mmφ double tube tuyere is
Test blowing was conducted with the oxygen flow rate set at 5.0Nm 3 /min and the amount of top-blown oxygen by the top-blowing lance 3 set at 7.5Nm 3 /min. After the start of blowing, the uniform mixing time of the steel bath was determined by the method shown in FIG. Since the uniform mixing time of the steel bath is 1 to 2 minutes at most, it is difficult to examine changes in the concentration of the steel bath by continuous sampling. Therefore, the uniform mixing time was determined by sampling at different locations at the same time, adding the tracer, and determining whether or not it was uniform based on the sampling time. A Cu wire with a thickness of 1 mm was used as a tracer, and sample collection was performed using a sampler 7 having a width w of 450 mm and consisting of three bombs 8 as shown in FIG. 6th
The figure shows an example of the measurement. In Figure 6, the horizontal axis shows the time after tracer addition, and the vertical axis shows the time in the steel before adding Cu.
Cu concentration is Cuo, Cu concentration in steel at time t is
Cut, Cu concentration in steel after complete mixing is Cuf, (Cut
-Cuo)/(Cuf-Cuo). At the same time, the amount of brick loss at the bottom of the furnace after each blowing process was also measured. The results of each test blowing are as follows: L 1 /D is 0.38 to 0.80 L 1 /D is 0.19 to 0.58 L 2 /D is 0.28 to 0.69 Figure 7 shows the effects. Also, for l 2 /D in the range of 0.025 to 0.30,
FIG. 8 shows the tendency that L 1 /D has on the uniform mixing time and the amount of wear of the furnace bottom bricks. First, looking at the change in uniform mixing time as l 2 /D fluctuates in Figure 7, when l 2 /D = 0, that is, when the bottom blowing tuyeres 2 are arranged along the diameter of the hearth bottom, Uniform mixing time is approx.
It is 40 seconds. When l 2 /D is eccentric to 0.025 to 0.30, the uniform mixing time shows a value of about 22 to 26 seconds. When l 2 /D exceeds 0.30 and reaches 0.35, the uniform mixing time increases to about 40 to 42 seconds. On the other hand, the amount of wear on the furnace bottom bricks shows a large value of approximately 5 mm/heat when (a) l 2 /D=0. (b) When l 2 /D exceeds 0.025 and reaches 0.30, it is approximately 2 to 3
It rapidly decreases to mm/heat. (c) Even when l 2 /D exceeded 0.30 and was within 0.35, it remained almost constant. Next, according to Fig. 8, the influence of L 1 /D on the uniform mixing time and the amount of wear of the furnace bottom bricks is as follows:
It was confirmed that when L 1 /D is in the range of 0.38 to 0.80, the uniform mixing time is short and the amount of wear of the furnace bottom bricks is also small. As a result of the above confirmation experiment, the damping buildup of the water model experiment described above is reflected almost directly in the actual reactor operation.
It has been experimentally demonstrated that the present invention can reliably reduce furnace body vibration even when a bottom blowing function is added to an LD converter that originally has a long body as shown in Figure 2. It was. Therefore, by employing the bottom-blowing tuyere arrangement of the present invention, it has become possible to simplify the support structure and foundation for withstanding severe vibrations in the bottom-blowing converter. Furthermore, according to the present invention, in the case of adding a bottom blowing function to an LD converter as shown in Fig. 2,
Reinforcement of the support frame, which was conventionally required for top-bottom blowing, is virtually unnecessary. As described above, the present invention is extremely effective in suppressing converter vibrations, and also brings about the effect of significantly reducing wear and tear on the furnace body and furnace bottom bricks. 【table】

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

第1図は底吹き転炉の縦断面図、第2図はLD
転炉炉体を活用した上底吹き転炉の縦断面図、第
3図は炉底平面図、第4図は均一混合時間の測定
方法を示す転炉の模式断面図、第5図はサンプラ
ーの側面図、第6図は均一混合時間の測定例を示
すグラフ、第7図はl2/Dが均一混合時間、炉底
れんが損耗量に及ぼす影響を示すグラフ、第8図
はl1/Dが均一混合時間、炉底れんが損耗量に及
ぼす影響示すグラフである。 1……炉底、2……底吹き羽口、3……ラン
ス、4……鋼浴、5……スラグ、6……火点、7
……サンプラー、8……ボンブ。
Figure 1 is a vertical cross-sectional view of a bottom blowing converter, Figure 2 is a LD
A vertical cross-sectional view of a top-bottom blowing converter utilizing a converter body, Figure 3 is a plan view of the furnace bottom, Figure 4 is a schematic cross-sectional view of a converter showing a method for measuring uniform mixing time, and Figure 5 is a sampler. Fig. 6 is a graph showing an example of measurement of uniform mixing time, Fig. 7 is a graph showing the effect of l 2 /D on uniform mixing time and the amount of wear of furnace bottom bricks, and Fig. 8 is a graph showing an example of measurement of uniform mixing time. It is a graph showing the influence of D on the uniform mixing time and the amount of wear of furnace bottom bricks. 1... Hearth bottom, 2... Bottom blowing tuyere, 3... Lance, 4... Steel bath, 5... Slag, 6... Flash point, 7
... Sampler, 8... Bomb.

Claims (1)

【特許請求の範囲】 1 上底吹き転炉または底吹き転炉において、底
吹き羽口を炉底の直径線と平行な線上に、次の条
件を満足するように配設したことを特徴とする底
吹き機能を持つ転炉。 (1) 0.38≦L1/D≦0.80 (2) 0.19≦l1/D≦0.58 (3) 0.28≦L2/D≦0.69 (4) 0.025≦l2/D≦0.30 ここに、 D:炉体のトラニオン軸と平行な炉底径 l2:トラニオン軸と平行な炉底直径線と羽口配
設線との水平距離 L1:炉底の直径線と平行で、かつ、出鋼側へl2
相当偏心配置した羽口配設線上の羽口の最
大領域幅 l1:炉底の直径線と平行で、かつ、出鋼側へl2
相当偏心配置した羽口配設線上の羽口の最
大領域幅内の羽口の非配置幅 L2:炉底の直径線と平行で、かつ、装入側へl2
当偏心配置した羽口配設線上の羽口の最大
領域幅
[Claims] 1. A top-bottom blowing converter or a bottom-blowing converter, characterized in that the bottom blowing tuyere is arranged on a line parallel to the diameter line of the hearth bottom so as to satisfy the following conditions: A converter with a bottom blowing function. (1) 0.38≦L 1 /D≦0.80 (2) 0.19≦l 1 /D≦0.58 (3) 0.28≦L 2 /D≦0.69 (4) 0.025≦l 2 /D≦0.30 where, D: Furnace Diameter of the hearth bottom parallel to the trunnion axis of the body L 2 : Horizontal distance between the hearth bottom diameter line parallel to the trunnion axis and the tuyere installation line L 1 : Parallel to the hearth bottom diameter line and toward the tapping side l 2
The maximum area width of the tuyere on the tuyere installation line with a fairly eccentric arrangement l 1 : Parallel to the diameter line of the furnace bottom and toward the tapping side l 2
Non-disposed width of the tuyere within the maximum area width of the tuyere on the tuyere arrangement line L2 : A tuyere that is parallel to the diameter line of the hearth bottom and eccentrically arranged to the charging side by L2 Maximum area width of tuyere on installation line
JP2859383A 1983-02-24 1983-02-24 Converter having bottom blowing function Granted JPS59157212A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2859383A JPS59157212A (en) 1983-02-24 1983-02-24 Converter having bottom blowing function

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2859383A JPS59157212A (en) 1983-02-24 1983-02-24 Converter having bottom blowing function

Publications (2)

Publication Number Publication Date
JPS59157212A JPS59157212A (en) 1984-09-06
JPS6210284B2 true JPS6210284B2 (en) 1987-03-05

Family

ID=12252887

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2859383A Granted JPS59157212A (en) 1983-02-24 1983-02-24 Converter having bottom blowing function

Country Status (1)

Country Link
JP (1) JPS59157212A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5282396B2 (en) * 2007-11-30 2013-09-04 Jfeスチール株式会社 Top-bottom blowing converter

Also Published As

Publication number Publication date
JPS59157212A (en) 1984-09-06

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