JPH0637653B2 - Operation method of fluidized-ore reduction furnace for fine ore - Google Patents
Operation method of fluidized-ore reduction furnace for fine oreInfo
- Publication number
- JPH0637653B2 JPH0637653B2 JP23963889A JP23963889A JPH0637653B2 JP H0637653 B2 JPH0637653 B2 JP H0637653B2 JP 23963889 A JP23963889 A JP 23963889A JP 23963889 A JP23963889 A JP 23963889A JP H0637653 B2 JPH0637653 B2 JP H0637653B2
- Authority
- JP
- Japan
- Prior art keywords
- fluidized
- ore
- reduction
- volume fraction
- fluidized bed
- 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 - Lifetime
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- Manufacture Of Iron (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、鉱石、とくに鉄鉱石の流動層還元炉の高効率
操業を維持するための方法に関する。Description: FIELD OF THE INVENTION The present invention relates to a method for maintaining high efficiency operation of a fluidized bed reduction furnace for ores, especially iron ores.
近年、従前の高炉による製鉄法が設備投資額が大きく、
また、良質の塊成鉱やコークスを必要とする原料選択上
の制約等の問題点を解消した溶融還元製鉄法が出現し
た。溶融還元製鉄プロセスは、溶融還元炉と予備還元炉
との2の大きなユニットにより構成され、予備還元炉に
は粒子循環装置を有する流動層を応用する方法が一般的
である。この流動還元炉は基本的には、鉄鉱石、還元ガ
スを装入する流動層反応塔と、反応塔からガスと共に排
出された鉱石を、気体−固体分離のためのサイクロンで
捕集し、反応塔の下部に再度装入する下降連結管とから
なる構造を有する。In recent years, the steelmaking method using the conventional blast furnace has a large amount of capital investment,
In addition, a smelting reduction ironmaking method has emerged that has solved problems such as restrictions on raw material selection that require high quality agglomerated ore and coke. The smelting reduction ironmaking process is composed of two large units, a smelting reduction furnace and a preliminary reduction furnace, and a method of applying a fluidized bed having a particle circulation device to the preliminary reduction furnace is common. This fluidized-bed reduction furnace basically collects iron ore and a fluidized bed reaction tower into which a reducing gas is charged, and ore discharged together with gas from the reaction tower with a cyclone for gas-solid separation, and a reaction. It has a structure consisting of a descending connecting pipe that is recharged at the bottom of the tower.
しかしながら、かかる流動還元炉は、粉鉱石を浮遊せし
めた希薄な流動層において反応させるために、還元ガス
の利用効率が悪く反応塔の容積当たりの生産性が低く、
また安定した還元率を有する成品を得るのが困難である
という欠点がある。However, since such a fluidized-bed reduction reactor reacts in a dilute fluidized bed in which fine ore is suspended, the utilization efficiency of the reducing gas is poor and the productivity per volume of the reaction tower is low,
There is also a drawback that it is difficult to obtain a product having a stable reduction rate.
そのため、上記流動還元炉において生産性を確保すると
共に安定した還元率の成品を得るための操業法が種々提
案されている。Therefore, various operating methods have been proposed for securing productivity in the fluidized-bed reduction furnace and obtaining a product with a stable reduction rate.
例えば、特開昭63-57709号公報には、製品抽出速度,鉱
石循環流量,還元ガス供給量,還元ガス入口化度を変更
することによって還元率を制御する方が開示されてい
る。For example, Japanese Patent Laid-Open No. 63-57709 discloses a method of controlling the reduction rate by changing the product extraction rate, ore circulation flow rate, reducing gas supply rate, and reducing gas inlet degree.
また、特開平1-115447号公報には、循環ガスの流速ある
いは粒子循環速度を制御することによって、操業条件の
変動や変更に対して流動状態を安定的に維持する方法が
開示されている。Further, Japanese Patent Application Laid-Open No. 1-115447 discloses a method of controlling a flow rate of a circulating gas or a particle circulation rate to stably maintain a fluid state against fluctuations and changes in operating conditions.
これら開示された操業法によって、装入鉱石の還元率や
流動状態に大きな変化を与えないように操業状態を維持
することは可能となる。By these disclosed operation methods, it is possible to maintain the operation state so as not to make a large change in the reduction rate and the flow state of the charged ore.
ところが、かかる制御方法は、単に炉の安定操業を目的
とするだけで、還元炉の処理容量をフルに用いた効率の
高い操業状態を得ることは考慮されておらず、結果的に
操業効率の劣る操作が継続されることになる。However, such a control method is merely aimed at stable operation of the furnace, and is not considered to obtain a highly efficient operating state in which the processing capacity of the reduction furnace is fully used. Inferior operation will continue.
本発明において解決すべき課題は、安定操業は勿論、そ
の容量と導入還元ガスの還元機能を最大に利用できる循
環流動還元炉の高効率操業法を確立することにある。The problem to be solved in the present invention is to establish a highly efficient operation method of a circulating fluidized-bed reduction reactor which can maximize the capacity and the reducing function of the introduced reducing gas as well as the stable operation.
本発明は、流動還元炉の流動層における粒子体積分率を
特定範囲に維持することによって、流動層に導入される
還元ガスを鉱石の還元に最も有効に利用することがで
き、生産性が向上するという知見に基づいて完成したも
ので、流動還元炉のガス流速、粒子循環流量の何れか、
もしくは両方を制御して粒子体積分率を略4〜15%の
範囲内に保持するものである。INDUSTRIAL APPLICABILITY According to the present invention, by maintaining the particle volume fraction in the fluidized bed of a fluidized-bed reduction reactor within a specific range, the reducing gas introduced into the fluidized bed can be most effectively used for the reduction of ores, and the productivity is improved. It was completed based on the knowledge that
Alternatively, both are controlled to maintain the particle volume fraction within the range of approximately 4 to 15%.
流動層内に導入される還元ガスの利用率によって表わさ
れる還元炉の操業効率は、反応流動層内の鉱石粒子体積
分率が特定範囲内にあるとき、高い値を示す。The operation efficiency of the reducing furnace, which is represented by the utilization rate of the reducing gas introduced into the fluidized bed, shows a high value when the ore particle volume fraction in the reaction fluidized bed is within a specific range.
鉱石粒子体積分率が小さい場合には、還元ガスと反応す
る粒子が流動層内に少ないためにガスが充分に反応せず
に炉外へ排出され、効率が急激に低下する。その許容限
界は略4%である。When the volume fraction of the ore particles is small, there are few particles that react with the reducing gas in the fluidized bed, so the gas does not react sufficiently and is discharged out of the furnace, resulting in a sharp drop in efficiency. The allowable limit is about 4%.
また、流動層内の粒子体積分率が大きい場合は、流動層
内の粒子量は多いが、粒子の分散が悪くなって粒子集合
体が偏在することになり、その間をガスが吹き抜けて固
気接触が不十分となるため、ガスが充分に鉄粒子と反応
せずに炉外へ排出され効率が急激に低下する。その許容
限界は略15%である。When the volume fraction of particles in the fluidized bed is large, the amount of particles in the fluidized bed is large, but the dispersion of the particles becomes poor and the particle aggregates are unevenly distributed. Due to insufficient contact, the gas does not react sufficiently with the iron particles and is discharged outside the furnace, resulting in a sharp drop in efficiency. The allowable limit is about 15%.
そして、かかる鉱石粒子体積分率のその範囲内での維持
は、流動還元炉のガス流速、粒子循環流量の何れか、も
しくは両方を調整することによって可能となる。Then, the ore particle volume fraction can be maintained within that range by adjusting either or both of the gas flow rate of the fluidized-bed reduction reactor and the particle circulation flow rate.
第1図は本発明の操業形態を模図的に示す図である。流
動還元炉10は反応層を形成する上昇管1と部分還元粒
子を再度上昇管1に戻すルートを形成する下降管2とか
らなる。FIG. 1 is a diagram schematically showing an operating form of the present invention. The fluidized-bed reduction furnace 10 is composed of a rising pipe 1 forming a reaction layer and a descending pipe 2 forming a route for returning the partially reduced particles to the rising pipe 1 again.
同図を参照して、原料供給口3より供給された粉鉱石4
は上昇管1の下方から供給される還元ガス5により流動
層を形成して還元される。反応後の還元ガス5はサイク
ロン6に入り、ガスに同伴された粒子は下降管2を介し
て上昇管1に戻る。Referring to the figure, the powdered ore 4 supplied from the raw material supply port 3
Is reduced by forming a fluidized bed by the reducing gas 5 supplied from below the rising pipe 1. After the reaction, the reducing gas 5 enters the cyclone 6, and the particles entrained in the gas return to the ascending pipe 1 via the descending pipe 2.
その過程で一部は成品として下降管2の取り出し口7、
もしくは流動層下部の成品取り出し口8から回収され
る。操業に際しての上昇管1の下部と上部の圧力はそれ
ぞれの箇所に取付けられた圧力検出器9a,9bによっ
て検出される。In the process, a part of the product is taken out of the downcomer 2 as a product 7,
Alternatively, it is collected from the product outlet 8 at the bottom of the fluidized bed. The pressures of the lower part and the upper part of the rising pipe 1 during the operation are detected by the pressure detectors 9a and 9b attached at the respective positions.
かかる流動還元炉における流動層内の粒子体積分率は次
式によって推定される。The particle volume fraction in the fluidized bed in such a fluidized-bed reduction reactor is estimated by the following equation.
粒子体積分率(%)=100(P1-P2)/L/ρs ただし、P1:上昇管下部圧力(kg/m2) P2:上昇管上部圧力(kg/2) L:圧力検出端9aと9bとの距離(m) ρs:流動層内粒子密度(kg/3) である。Particle volume fraction (%) = 100 (P1-P2) / L / ρs where P1: rising tube lower pressure (kg / m 2 ) P2: rising tube upper pressure (kg / 2 ) L: pressure detecting end 9a Distance from 9b (m) ρs: Particle density in the fluidized bed (kg / 3 ).
第2図は第1図に示す流動還元炉の流動層内における鉱
石粒子の体積分率とガス利用率との関係を示す図であ
る。FIG. 2 is a diagram showing the relationship between the gas utilization rate and the volume fraction of ore particles in the fluidized bed of the fluidized-bed reduction reactor shown in FIG.
同図に示すガス利用率は流動層入口と出口の還元ガスの
酸化度すなわち、 〔(CO2+H2O)/(CO+CO2+H2+H2O)〕 の差として示されるもので、還元ガスが還元に有効に利
用された効率の指標とすることができる。The gas utilization rate shown in the figure is shown as the difference between the oxidation degree of the reducing gas at the inlet and outlet of the fluidized bed, that is, [(CO 2 + H 2 O) / (CO + CO 2 + H 2 + H 2 O)]. Can be used as an index of efficiency effectively used for reduction.
このときの主要な操業条件は、流動層内の温度820〜
860℃、入口ガスの酸化度12〜18%、製品還元率
40〜50%、粒子循環速度50〜250kg/m2/s、
ガス流速5〜9m/sである。The main operating conditions at this time are temperature 820 to 820 in the fluidized bed.
860 ° C., degree of oxidation of inlet gas 12-18%, product reduction rate 40-50%, particle circulation speed 50-250 kg / m 2 / s,
The gas flow rate is 5 to 9 m / s.
流動層内の粒子体積分率が特定範囲A内においては、ガ
ス利用率は13〜18%、生産速度は5〜9t−Fe/
m2/hが得られた。これらの値はいずれも特定範囲A外
の1.5倍以上であった。When the particle volume fraction in the fluidized bed is within the specific range A, the gas utilization rate is 13 to 18% and the production rate is 5 to 9t-Fe /
m 2 / h was obtained. All of these values were 1.5 times or more outside the specific range A.
高いガス利用率や生産速度を得る粒子体積分率の範囲
は、いかなるディメンジョンの炉、あるいはいかなる条
件の下での操業においても、略4%と略15%の範囲内
にある。すなわち、粒子体積分率の特定範囲A内にある
ときのガス利用率は、特定範囲A外にあるときに比べて
いずれの場合も1.5倍以上であり、生産速度も2t−F
e/m2/h以上が得られる。The range of particle volume fraction for obtaining high gas utilization rate and production rate is in the range of approximately 4% and approximately 15% in any dimension furnace or operation under any conditions. That is, the gas utilization rate when the particle volume fraction is within the specific range A is 1.5 times or more as compared with when it is outside the specific range A, and the production rate is 2 t-F.
e / m 2 / h or more can be obtained.
他方、流動還元炉における流動層内の鉱石粒子の体積分
率は流動層内のガス流速と鉱石の循環流量とそれぞれ一
義的な関係を有する。第3図は粒子体積分率と流動層内
のガス流速、それに鉱石の循環流量の関係を示す。同図
に示すように、ガス流速の低下により流動層内の粒子体
積分率は増加し、逆の場合は減少する。また、粒子循環
流量が増大すれば粒子体積分率は増大する。On the other hand, the volume fraction of the ore particles in the fluidized bed in the fluidized-bed reduction reactor has a unique relationship with the gas flow velocity in the fluidized bed and the circulating flow rate of the ore. FIG. 3 shows the relationship between the particle volume fraction, the gas flow velocity in the fluidized bed, and the circulating flow rate of ore. As shown in the figure, the particle volume fraction in the fluidized bed increases due to the decrease in the gas flow velocity, and decreases in the opposite case. Further, the particle volume fraction increases as the particle circulation flow rate increases.
したがって、第2図と第3図の関係から、流動層内のガ
ス流速と鉱石の循環流量あるいは両方の因子を、上記の
高い操業効率を得るための粒子体積分率の特定範囲A内
に維持するための制御因子とすることができる。Therefore, from the relationship between FIG. 2 and FIG. 3, the factors of the gas flow velocity in the fluidized bed and the circulating flow rate of the ore or both are maintained within the specific range A of the particle volume fraction for obtaining the above high operation efficiency. Can be a controlling factor for
第4図は第1図に示す構造を有する流動還元炉の操業列
を示すもので、鉱石粒子の循環流量とガス流速、それに
よる粒子体積分率と鉱石還元率と生産速度との関連を示
す。FIG. 4 shows the operation sequence of the fluidized-bed reduction reactor having the structure shown in FIG. 1, and shows the relationship between the circulation flow rate of ore particles and the gas flow rate, the particle volume fraction, the ore reduction rate, and the production rate. .
同図に示すように、ガス流速と粒子循環流量により流動
層内の粒子体積分率の制御が可能であり、ひいてはガス
流速と粒子循環流量により流動層の操業効率の制御が可
能であることが判る。As shown in the figure, it is possible to control the particle volume fraction in the fluidized bed by the gas flow velocity and the particle circulation flow rate, and it is possible to control the operation efficiency of the fluidized bed by the gas flow velocity and the particle circulation flow rate. I understand.
本発明の流動還元炉の操業法によって以下の効果を奏す
ることができる。The following effects can be achieved by the operation method of the fluidized-bed reduction reactor of the present invention.
(1) 還元ガスと鉱石の接触が良好な領域での反応が可
能となる。その結果、還元炉の効率を最大限に活かした
操業が可能となる。(1) The reaction can be performed in a region where the reducing gas and the ore are in good contact with each other. As a result, it is possible to operate the reduction furnace with the maximum efficiency.
(2) 効率の良い状態の操業が維持でき、還元炉の高効
率操業が可能となる。(2) The efficient operation can be maintained and the reduction furnace can be operated with high efficiency.
(3) 円滑に還元が進行し生産性が向上する。(3) Return will proceed smoothly and productivity will be improved.
第1図は本発明の操業形態を模図的に示す図である。第
2図は鉱石粒子の体積分率と還元ガス利用率との関連を
示し、第3図は鉱石粒子の体積分率とガス流速と粒子循
環流速との関係を示す図である。第4図は第1図に示す
流動還元炉の操業状態を示す図である。 1:上昇管、2:下降管 3:原料供給口、4:粉鉱石 5:還元ガス、6:サイクロン 7,8:成品取り出し口 9a,9b:圧力検出器、10:流動還元炉FIG. 1 is a diagram schematically showing an operating form of the present invention. FIG. 2 shows the relationship between the volume fraction of ore particles and the reducing gas utilization rate, and FIG. 3 is a diagram showing the relationship between the volume fraction of ore particles, the gas flow velocity, and the particle circulation flow velocity. FIG. 4 is a diagram showing an operating state of the fluidized-bed reduction reactor shown in FIG. 1: Upcomer pipe, 2: Downcomer pipe 3: Raw material supply port, 4: Fine ore 5: Reduction gas, 6: Cyclone 7,8: Product outlet 9a, 9b: Pressure detector, 10: Flow reduction furnace
フロントページの続き (72)発明者 江頭 達彦 福岡県北九州市戸畑区大字中原46番地の59 新日本製鐵株式會社機械・プラント事業 部内Front Page Continuation (72) Inventor Tatsuhiko Egashira 59, 46 Nakahara, Tobata-ku, Kitakyushu, Fukuoka Prefecture 59 Nippon Steel Co., Ltd. Machinery & Plant Division
Claims (1)
環流量あるいは両方を調整して流動還元炉内の粒子体積
分率を4〜15%の範囲内に維持する粉鉱石の流動還元炉
の操業方法。1. A fluidized reduction of fine ore in which a particle volume fraction in a fluidized-bed reduction reactor is maintained within a range of 4 to 15% by adjusting a gas flow rate in a fluidized-bed reduction fluidized bed and a circulation flow rate of ore or both. How to operate the furnace.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23963889A JPH0637653B2 (en) | 1989-09-14 | 1989-09-14 | Operation method of fluidized-ore reduction furnace for fine ore |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23963889A JPH0637653B2 (en) | 1989-09-14 | 1989-09-14 | Operation method of fluidized-ore reduction furnace for fine ore |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03100111A JPH03100111A (en) | 1991-04-25 |
| JPH0637653B2 true JPH0637653B2 (en) | 1994-05-18 |
Family
ID=17047692
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23963889A Expired - Lifetime JPH0637653B2 (en) | 1989-09-14 | 1989-09-14 | Operation method of fluidized-ore reduction furnace for fine ore |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0637653B2 (en) |
-
1989
- 1989-09-14 JP JP23963889A patent/JPH0637653B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03100111A (en) | 1991-04-25 |
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