US20220403477A1 - Blast furnace operation method - Google Patents

Blast furnace operation method Download PDF

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US20220403477A1
US20220403477A1 US17/779,384 US202017779384A US2022403477A1 US 20220403477 A1 US20220403477 A1 US 20220403477A1 US 202017779384 A US202017779384 A US 202017779384A US 2022403477 A1 US2022403477 A1 US 2022403477A1
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gas
hydrogen
containing gas
concentration hydrogen
temperature
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Hiroshi Sakai
Kaoru Nakano
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JFE Steel Corp
Kobe Steel Ltd
Nippon Steel Corp
Nippon Steel Engineering Co Ltd
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JFE Steel Corp
Kobe Steel Ltd
Nippon Steel Corp
Nippon Steel Engineering Co Ltd
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Assigned to NIPPON STEEL ENGINEERING CO., LTD., KABUSHIKI KAISHA KOBE SEIKO SHO (KOBE STEEL, LTD.), NIPPON STEEL CORPORATION, JFE STEEL CORPORATION reassignment NIPPON STEEL ENGINEERING CO., LTD. ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: NAKANO, KAORU, SAKAI, HIROSHI
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    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21BMANUFACTURE OF IRON OR STEEL
    • C21B5/00Making pig-iron in the blast furnace
    • C21B5/06Making pig-iron in the blast furnace using top gas in the blast furnace process
    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21BMANUFACTURE OF IRON OR STEEL
    • C21B7/00Blast furnaces
    • C21B7/16Tuyéres
    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21BMANUFACTURE OF IRON OR STEEL
    • C21B7/00Blast furnaces
    • C21B7/007Controlling or regulating of the top pressure
    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21BMANUFACTURE OF IRON OR STEEL
    • C21B5/00Making pig-iron in the blast furnace
    • C21B5/001Injecting additional fuel or reducing agents
    • C21B2005/005Selection or treatment of the reducing gases

Definitions

  • the present invention relates to a blast furnace operation method.
  • a blast furnace method is a mainstream steelmaking process.
  • iron-bearing materials for a blast furnace raw materials including iron oxide; mainly sintered ores; hereinafter simply referred to as “iron-bearing materials”
  • coke are alternately charged in layers in the blast furnace from the top of the blast furnace, and hot blast is blown into the blast furnace from a tuyere of a lower part of the blast furnace.
  • the hot blast reacts with pulverized coal blown together with the hot blast and the coke in the blast furnace such that a high-temperature reducing gas (here, mainly CO gas) is produced in the blast furnace. That is, the hot blast gasifies the coke and the pulverized coal in the blast furnace.
  • a high-temperature reducing gas here, mainly CO gas
  • the reducing gas rises in the blast furnace and reduces the iron-bearing materials while heating the iron-bearing materials.
  • the iron-bearing materials are heated and reduced by the reducing gas while falling in the blast furnace.
  • the iron-bearing materials are melted and are dropped into the blast furnace while being further reduced by the coke.
  • the iron-bearing materials are accumulated in a hearth as molten iron (pig iron) including about 5 mass % of carbon.
  • the molten iron in the hearth is extracted from a tap hole and is provided for the next steelmaking process. Accordingly, in the blast furnace method, a carbon material such as coke or pulverized coal is used as a reducing material.
  • the reducing material has a function of heating charges inside the furnace as a heat source and a function of reducing the iron-bearing material in the furnace, and the reduction efficiency in the furnace needs to be increased in order to reduce the reducing material ratio.
  • Reduction reactions in the furnace can be represented by various reaction formulae.
  • a direct reduction reaction reaction formula: FeO+C ⁇ Fe+Co
  • coke is an endothermic reaction accompanied by high endothermic heat. Accordingly, in order to reduce the reducing material ratio, it is important to suppress the occurrence of this reaction as much as possible.
  • the direct reduction reaction occurs in a lower part of the blast furnace. Therefore, as long as the iron-bearing materials can be sufficiently reduced by a reducing gas such as CO or H 2 before the iron-bearing materials reach the furnace lower part, the iron-bearing materials that are a target of the direct reduction reaction can be reduced.
  • Patent Documents 1 to 6 a technique of blowing a reducing gas (H 2 gas, coke oven gas (COG), natural gas, city gas, or the like) together with hot blast from a tuyere to improve the reducing gas potential in the furnace is known.
  • the reducing gas is a carbon-containing reducing gas (a reducing gas in which carbon atoms are contained in a molecular structure of the gas, for example, a hydrocarbon gas)
  • the carbon atoms in the carbon-containing gas become CO gas in the blast furnace, which reduces the iron-bearing materials.
  • the hydrogen gas reduces the iron-bearing materials. Accordingly, the amount of the iron-bearing materials that are a target for the direct reduction reaction can be reduced.
  • carbon and “hydrogen” mean “carbon atom” and “hydrogen atom”, respectively.
  • an object of the present invention is to provide a new and improved blast furnace operation method capable of increasing the gas volume of a high-concentration hydrogen-containing gas blown from a tuyere as a reducing gas while maintaining a stable blast furnace operation, and further reducing the CO 2 emissions.
  • a blast furnace operation method comprising blowing a high-concentration hydrogen-containing gas containing 80 mol % or more of hydrogen gas from a tuyere under: a condition in which a blowing temperature of the high-concentration hydrogen-containing gas is room temperature or higher and 300° C. or lower and a gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is 200 Nm 3 /t or more and 500 Nm 3 /t or less; a condition in which the blowing temperature of the high-concentration hydrogen-containing gas is higher than 300° C. and 600° C.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is 145 Nm 3 /t or more; a condition in which the blowing temperature of the high-concentration hydrogen-containing gas is higher than 600° C. and 900° C. or lower and the gas volume of the high-concentration hydrogen-containing gas is 125 Nm 3 /t or more; a condition in which the blowing temperature of the high-concentration hydrogen-containing gas is higher than 900° C. and 1200° C. or lower and the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is 110 Nm 3 /t or more; or a condition in which the blowing temperature of the high-concentration hydrogen-containing gas is higher than 1200° C. and the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is 100 Nm 3 /t or more.
  • the blowing temperature of the high-concentration hydrogen-containing gas may be room temperature or higher and 300° C. or lower and the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas may be 200 Nm 3 /t or more and 300 Nm 3 /t or less.
  • the blowing temperature of the high-concentration hydrogen-containing gas may be higher than 300° C. and 600° C. or lower and the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas may be 145 Nm 3 /t or more and 600 Nm 3 /t or less.
  • the flame temperature may be 2050° C. or lower.
  • the flame temperature may be set to higher than 2050° C. and 2150° C. or lower.
  • the flame temperature may be set to higher than 2150° C. and 2250° C. or lower.
  • blowing temperature of the high-concentration hydrogen-containing gas may be higher than 600° C. and 1400° C. or lower.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas may be 1000 Nm 3 /t or less.
  • a flame temperature may be set to 2050° C. or lower.
  • a blast furnace operation method comprising obtaining a gas volume-carbon consumption parameter correlation, which is a correlation between a gas volume of hydrogen gas in a high-concentration hydrogen-containing gas and a carbon consumption parameter related to a carbon consumption amount when a blowing temperature of the high-concentration hydrogen-containing gas containing 80 mol % or more of the hydrogen gas is a predetermined value, in advance for each flame temperature; determining the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas at which the carbon consumption amount is reduced compared to that of a current operation, on the basis of the gas volume-carbon consumption parameter correlation; and blowing the high-concentration hydrogen-containing gas from the tuyere at the determined gas volume.
  • a gas volume-carbon consumption parameter correlation which is a correlation between a gas volume of hydrogen gas in a high-concentration hydrogen-containing gas and a carbon consumption parameter related to a carbon consumption amount when a blowing temperature of the high-concentration hydrogen-containing gas containing 80 mol % or more of the hydrogen gas is
  • the correlation between the hydrogen gas volume into the high-concentration hydrogen-containing gas and the carbon consumption parameter may be obtained for each blowing temperature of the high-concentration hydrogen-containing gas.
  • a gas volume-pressure drop change correlation which is a correlation between the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas and a change amount of a pressure loss with respect to a base operation when the blowing temperature of the high-concentration hydrogen-containing gas is a predetermined value, may be obtained in advance for each flame temperature, and the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas at which the carbon consumption amount is reduced compared to that of the current operation and the change amount of the pressure loss is a value within a predetermined range may be determined on the basis of the gas volume-carbon consumption parameter correlation and the gas volume-pressure drop change correlation.
  • a gas volume-top gas temperature change amount correlation which is a correlation between the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas and a change amount of a top gas temperature with respect to a base operation when the blowing temperature of the high-concentration hydrogen-containing gas is a predetermined value, may be obtained in advance for each flame temperature, and the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas at which the carbon consumption amount is reduced compared to that of the current operation and the change amount of the top gas temperature is a value within a predetermined range may be determined on the basis of the gas volume-carbon consumption parameter correlation and the gas volume-top gas temperature change amount correlation.
  • FIG. 1 is a diagram for explaining a blowing temperature of a high-concentration hydrogen-containing gas.
  • FIG. 2 is a graph showing the correlation between the gas volume of pure hydrogen gas at room temperature and the reduction percentage Input ⁇ C of specific carbon consumption for each flame temperature Tf.
  • FIG. 3 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 300° C. and the reduction percentage Input ⁇ C of the specific carbon consumption for each flame temperature Tf.
  • FIG. 4 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 350° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 5 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 600° C. and the reduction percentage Input ⁇ C of the specific carbon consumption for each flame temperature Tf.
  • FIG. 6 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 650° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 7 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 900° C. and the reduction percentage Input ⁇ C of the specific carbon consumption for each flame temperature Tf.
  • FIG. 8 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 950° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 9 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 1200° C. and the reduction percentage Input ⁇ C of the specific carbon consumption for each flame temperature Tf.
  • FIG. 10 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 1250° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 11 is a graph showing the correlation between the gas volume of the pure hydrogen gas at room temperature or the gas volume of the hydrogen gas in an 80 mol % H 2 -20 mol % N 2 high-concentration hydrogen-containing gas at room temperature and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 12 is a graph showing the correlation between the gas volume of the pure hydrogen gas at room temperature and the change amount of pressure loss for each flame temperature Tf.
  • FIG. 13 is a graph showing the correlation between the gas volume of the pure hydrogen gas at room temperature and the change amount of a top gas temperature for each flame temperature Tf.
  • FIG. 14 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 1200° C. and the change amount of pressure loss when the flame temperature Tf reaches 2100° C.
  • FIG. 15 is a graph showing the correlation between the blowing temperature of the pure hydrogen gas and the gas volume of pure hydrogen gas required to set the reduction percentage Input ⁇ C of specific carbon consumption to 10%.
  • FIG. 16 is a graph showing the correlation between the blowing temperature of the pure hydrogen gas and the gas volume of pure hydrogen gas required to set the reduction percentage Input ⁇ C of the specific carbon consumption to 20%.
  • a numerical range represented using “to” is a range including numerical values described before and after “to” as a lower limit and an upper limit.
  • the “reducing material ratio” is the total mass of a reducing material required to produce 1 ton of molten iron. Therefore, the reducing material ratio is basically the total mass of the coke and the pulverized coal required to produce 1 ton of molten iron, and the mass of a carbon-containing reducing gas in a high-concentration hydrogen-containing gas is treated as not included in the reducing material ratio.
  • the “specific carbon consumption (Input C)” is the carbon required to produce 1 ton of molten iron (that is, the carbon consumption amount per ton of molten iron).
  • the “reduction percentage Input ⁇ C of specific carbon consumption” is the reduction percentage of specific carbon consumption to the base operation that is an operation in which the high-concentration hydrogen-containing gas is not blown. Assuming that the Input C of the base operation in units of kg/t is A and the Input C at the time of the operation in units of kg/t is B, the Input ⁇ C is expressed by the following formula.
  • the present inventor has focused on the high-concentration hydrogen-containing gas as a reducing gas.
  • the high-concentration hydrogen-containing gas in the present embodiment is a gas containing 80 mol % or more of hydrogen gas (mol % of hydrogen gas with respect to the total amount of substances of all the gases constituting the high-concentration hydrogen-containing gas).
  • the high-concentration hydrogen-containing gas may be pure hydrogen gas (gas having a hydrogen gas concentration of 100 mol %).
  • the present inventors have focused on the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas (hereinafter, also simply referred to as the gas volume of hydrogen) and the blowing temperature of the high-concentration hydrogen-containing gas.
  • the reduction reaction of an iron-bearing material by the hydrogen gas in the high-concentration hydrogen-containing gas is an endothermic reaction.
  • raising the blowing temperature of the hydrogen gas can be considered.
  • the present inventors first performed a detailed study on the above matters. Specifically, finding the composition of various gases such as hydrogen gas and CO gas in the high-concentration hydrogen-containing gas and the reduction reaction rate of the high-concentration hydrogen-containing gas at various blowing temperatures, finding the effect of the temperature inside the furnace, which changes due to the reduction reaction heat of these gases, on the reduction reaction rate and the effect of the gas composition, which changes due to the reduction reaction, on the reduction reaction rate, and then finding the amounts of heat such that the reduction reaction rate does not decrease were performed for the entire furnace.
  • various gases such as hydrogen gas and CO gas in the high-concentration hydrogen-containing gas and the reduction reaction rate of the high-concentration hydrogen-containing gas at various blowing temperatures
  • the reduction percentage Input ⁇ C of the specific carbon consumption does not simply increase with an increase in the gas volume of hydrogen gas in the high-concentration hydrogen-containing gas, but is relaxed and starts to decrease when the gas volume increases to some extent. Also, the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas when the reduction percentage Input ⁇ C of the specific carbon consumption is relaxed and starts to decrease varies depending on the blowing temperature of the high-concentration hydrogen-containing gas.
  • the reduction percentage Input ⁇ C of the specific carbon consumption tends to increase with an increase in the gas volume.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas increases to some extent, the reduction percentage Input ⁇ C of the specific carbon consumption becomes, for example, 7% or more. Therefore, the CO 2 emissions can be significantly reduced by blowing the gas volume of the high-concentration hydrogen-containing gas in the blast furnace, which is determined according to the gas volume of hydrogen gas in this appropriate range.
  • the reduction percentage Input ⁇ C of specific carbon consumption during the operation of the blast furnace can be set to 7% or more, and the CO 2 emissions can be significantly reduced.
  • the present inventors came up with a blast furnace operation method according to the present embodiment on the basis of such knowledge. Hereinafter, the present embodiment will be described in detail.
  • the high-concentration hydrogen-containing gas is blown from a tuyere.
  • the high-concentration hydrogen-containing gas is a gas containing 80 mol % or more of hydrogen gas as described above.
  • the high-concentration hydrogen-containing gas includes pure hydrogen gas.
  • the high-concentration hydrogen-containing gas includes gas components other than the hydrogen gas, for example, the above-described carbon-containing reducing gas (for example, a hydrocarbon gas), CO gas, CO 2 gas, H 2 O gas, N 2 gas, or the like.
  • the total concentration of the other gases is less than 20 mol %.
  • Gases of which the total concentration of the other gas components is 20 mol % or more are not included in the high-concentration hydrogen-containing gas in the present embodiment. This is because the reduced amount of CO 2 gas decreases significantly in a case where the concentration of the other gases is 20 mol % or more.
  • the reduction efficiency in the blast furnace decreases. For this reason, the amount of iron-bearing materials that reach a lower part of the blast furnace without being reduced increases. Therefore, the amount of direct reduction reaction by coke increases.
  • the reducing material is required to maintain the temperature in the blast furnace, and the amount of CO 2 gas reduction decreases significantly.
  • COG coke furnace gas
  • the hydrogen gas is blown into the blast furnace with a gas volume of 300 Nm 3 /t.
  • the effect of reducing the CO 2 emissions in this case is significantly inferior to that when the pure hydrogen gas is blown into the blast furnace with a gas volume of 300 Nm 3 /t, and does not lead to a drastic reduction of the CO 2 emissions (for example, reduction percentage Input ⁇ C of specific carbon consumption ⁇ 7%).
  • the effect of reducing the CO 2 emissions is maximized when the gas volume is about 300 Nm 3 /t.
  • the blast furnace operation method according to the present embodiment will be described.
  • the blowing temperature of the high-concentration hydrogen-containing gas is determined within a range of room temperature or higher.
  • FIG. 1 is a diagram for explaining the blowing temperature.
  • the temperature of the high-concentration hydrogen-containing gas is regulated, for example, in a gas tank 3 including a heater 5 . That is, the high-concentration hydrogen-containing gas is sent to the tuyere 2 for blowing hot blast provided at the lower part of the blast furnace 1 after being heated by the heater 5 in the gas tank 3 or while remaining unheated at room temperature.
  • the high-concentration hydrogen-containing gas sent to the tuyere 2 can be blown into the blast furnace 1 from the tuyere 2 .
  • the high-concentration hydrogen-containing gas sent to the tuyere 2 is mixed (merged) with the hot blast generated in a hot blast furnace 4 and then blown into the blast furnace 1 from the tuyere 2 .
  • the blowing temperature is the temperature of the high-concentration hydrogen-containing gas immediately before being mixed with the hot blast when the hot blast is blown into the blast furnace 1 from the tuyere 2 .
  • the set temperature of the heater 5 can be set as the blowing temperature.
  • the temperature in this case is not the blowing temperature in the present embodiment. Additionally, although the blast temperature is described in Patent Document 1, the blast temperature in Patent Document 1 is different from the blowing temperature in the present embodiment.
  • FIG. 2 is a graph showing the correlation between the gas volume of the pure hydrogen gas at room temperature and the reduction percentage Input ⁇ C of the specific carbon consumption for each flame temperature Tf.
  • This graph is obtained by blast furnace operation simulation. Details of the blast furnace operation simulation are described in the examples. However, here, a so-called “Blast Furnace Mathematical Model” Kouji TAKATANI, Takanobu INADA, Yutaka UJISAWA, “Three-dimensional Dynamic Simulator for Blast Furnace”, ISIJ International, Vol.
  • FIG. 3 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 300° C. and the reduction percentage Input ⁇ C of the specific carbon consumption for each flame temperature Tf.
  • FIG. 4 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 350° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 5 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 600° C.
  • FIG. 6 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 650° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 7 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 900° C. and the reduction percentage Input ⁇ C of the specific carbon consumption for each flame temperature Tf.
  • FIG. 8 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 950° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • FIG. 9 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 1200° C. and the reduction percentage Input ⁇ C of specific carbon consumption for each flame temperature Tf.
  • FIG. 10 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 1250° C. and the reduction percentage Input ⁇ C of the specific carbon consumption.
  • the blowing temperature of the high-concentration hydrogen-containing gas it is preferable to raise the blowing temperature of the high-concentration hydrogen-containing gas. Specifically, it is preferable to determine the blowing temperature in a range of higher than 300° C., more preferably in a range of higher than 600° C., and more preferably in a range of higher than 900° C.
  • the blowing temperature of the high-concentration hydrogen-containing gas may be determined within a range of room temperature to 600° C.
  • the blowing temperature of the high-concentration hydrogen-containing gas may be determined within a range of higher than 600° C.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is determined.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is the flow rate per ton of molten iron of hydrogen gas in the high-concentration hydrogen-containing gas blown into the blast furnace from the tuyere, and the unit is Nm 3 /t.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is equal to the gas volume of the high-concentration hydrogen-containing gas.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is the amount obtained by multiplying the gas volume of the high-concentration hydrogen-containing gas in units of mol % by the ratio of the hydrogen gas.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is calculated from the value indicated by a flow meter provided at a discharge port of a high-concentration hydrogen-containing gas supply source (for example, a gas tank) and the ratio of the hydrogen gas in the high-concentration hydrogen-containing gas in units of mol %.
  • the gas volume is determined by classifying cases at the blowing temperature of the high-concentration hydrogen-containing gas. Specifically, in a case where the blowing temperature is room temperature to 300° C., the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is determined within a range of 200 to 500 Nm 3 /t. On the other hand, in a case where the blowing temperature is higher than 300° C. and 600° C. or lower, the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is determined within a range of 145 Nm 3 /t or more. In a case where the blowing temperature of the high-concentration hydrogen-containing gas is higher than 600° C. and 900° C.
  • the gas volume of the high-concentration hydrogen-containing gas is determined within a range of 125 Nm 3 /t or more.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is determined within a range of 110 Nm 3 /t or more.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is determined within a range of 100 Nm 3 /t or more.
  • the reduction percentage Input ⁇ C of the specific carbon consumption increases when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is increased from 0 in the base operation. Then, when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas reaches about 300 Nm 3 /t, the reduction percentage Input ⁇ C of the specific carbon consumption reaches a peak, and when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas further increases, the reduction percentage Input ⁇ C of the specific carbon consumption starts to decrease.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is in a range of 200 to 500 Nm 3 /t, it is possible to set the reduction percentage Input ⁇ C of the specific carbon consumption to 7% or more.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is the gas volume of the high-concentration hydrogen-containing gas.
  • this value is the amount obtained by multiplying the gas volume of the high-concentration hydrogen-containing gas by the ratio of the hydrogen gas (mol %).
  • the reduction reaction of the iron-bearing materials with the hydrogen gas (that is, the hydrogen reduction reaction) is an endothermic reaction.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas exceeds 300 Nm 3 /t, it is considered that such an endothermic reaction occurs frequently in the furnace and the temperature inside the furnace drops.
  • such a decrease in the temperature inside the furnace is considered to reduce the reduction efficiency of the reducing gas containing hydrogen gas. In order to prevent such a decrease in reduction efficiency, it is necessary to increase the reducing material ratio to perform the operation.
  • the reduction percentage Input ⁇ C of the specific carbon consumption starts to decrease. Therefore, in a case where the blowing temperature is room temperature to 300° C., it is preferable to determine the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas within a range of 200 to 400 Nm 3 /t, and it is more preferable to determine the gas volume within a range of 200 to 300 Nm 3 /t. In this case, it is possible to set the reduction percentage Input ⁇ C of the specific carbon consumption to 8% or more.
  • the reduction percentage Input ⁇ C of the specific carbon consumption increases when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is increased from 0 Nm 3 /t Nm in the base operation. Then, when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is 145 Nm 3 /t or more, the reduction percentage Input ⁇ C of the specific carbon consumption becomes 7% or more. In a case where the blowing temperature of the high-concentration hydrogen-containing gas is 600° C., as shown in FIG.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is about 600 Nm 3 /t, and the reduction percentage Input ⁇ C of the specific carbon consumption reaches saturation. Then, in a case where the blowing temperature of the high-concentration hydrogen-containing gas is 350° C., as shown in FIG. 4 , when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas reaches about 300 Nm 3 /t, the reduction percentage Input ⁇ C of the specific carbon consumption reaches a peak, and when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas further increases, the reduction percentage Input ⁇ C of the specific carbon consumption starts to decrease.
  • the blowing temperature of the high-concentration hydrogen-containing gas is 350° C.
  • the flame temperature Tf is often set to about 2200° C., and in a case where it is difficult to maintain the flame temperature Tf at 2200° C., the operation conditions of the related-art blast furnace operation will be changed.
  • the reason why the reduction percentage Input ⁇ C of the specific carbon consumption starts to decrease in a case where the blowing temperature of the high-concentration hydrogen-containing gas is 350° C. is the same as above.
  • the blowing temperature of the high-concentration hydrogen-containing gas is 600° C.
  • the reduction percentage Input ⁇ C of the specific carbon consumption does not start to decrease in a range of the gas volume up to 700 Nm 3 /t.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is about 600 Nm 3 /t, the effect of reducing the specific carbon consumption reaches saturation.
  • the blowing temperature is higher than 350° C. and 600° C. or lower, the sensible heat of the Bosch gas is larger.
  • the temperature inside the furnace is considered unlikely to drop even if more hydrogen gas is blown than in the above case. Therefore, it is considered that even when a large amount of hydrogen gas is blown into the blast furnace, the temperature inside the furnace does not easily decrease and the reduction efficiency is unlikely to decrease. For this reason, the reduction percentage Input ⁇ C of the specific carbon consumption is considered to have reached saturation. Moreover, in a case where the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is 300 to 600 Nm 3 /t, the reduction percentage Input ⁇ C of the specific carbon consumption is 10% or more.
  • the reduction percentage Input ⁇ C of the specific carbon consumption increases when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is increased from 0 Nm 3 /t in the base operation. Then, in a case where the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is within a range of 125 Nm 3 /t or more, the reduction percentage Input ⁇ C of the specific carbon consumption is 7% or more.
  • the reduction percentage Input ⁇ C of the specific carbon consumption is 10% or more.
  • the increase rate of the reduction percentage Input ⁇ C of the specific carbon consumption decreases.
  • the reduction percentage Input ⁇ C of the specific carbon consumption does not start to decrease. This behavior is clearly different from the case where the blowing temperature of the high-concentration hydrogen-containing gas is 600° C. or lower.
  • FIG. 7 is a graph showing the correlation between the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas and the reduction percentage Input ⁇ C of the specific carbon consumption in a case where the blowing temperature of the high-concentration hydrogen-containing gas (here, the pure hydrogen gas) is 900° C.
  • the blowing temperature of the high-concentration hydrogen-containing gas here, the pure hydrogen gas
  • FIG. 7 was observed even in a case where the blowing temperature of the high-concentration hydrogen-containing gas was 650° C.
  • the reduction percentage Input ⁇ C the specific carbon consumption is 7.0% or more.
  • the reduction reaction caused by the hydrogen gas is an endothermic reaction
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas increases to some extent
  • the reduction percentage Input ⁇ C of the specific carbon consumption starts to decrease.
  • the blowing temperature of the high-concentration hydrogen-containing gas is higher than 600° C.
  • the sensible heat of the Bosch gas generated in the blast furnace becomes extremely high.
  • the reaction heat required for the reduction reaction can be covered. For this reason, it is considered that even when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas increases, the reduction percentage Input ⁇ C of the specific carbon consumption does not start to decrease but continues to increase.
  • the reduction percentage Input ⁇ C of the specific carbon consumption increases when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is increased from 0 Nm 3 /t Nm in the base operation. Then, in a case where the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is within a range of 110 Nm 3 /t or more, the reduction percentage Input ⁇ C of the specific carbon consumption is 7% or more.
  • the reduction percentage Input ⁇ C of the specific carbon consumption is 10% or more.
  • the increase rate of the reduction percentage Input ⁇ C of the specific carbon consumption decreases.
  • the reduction percentage Input ⁇ C of the specific carbon consumption does not start to decrease.
  • FIG. 9 is a graph showing the correlation between the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas and the reduction percentage Input ⁇ C of the specific carbon consumption in a case where the blowing temperature of the high-concentration hydrogen-containing gas (here, pure hydrogen gas) is 1200° C. The same tendency as in FIG. 9 was observed even in a case where the blowing temperature of the high-concentration hydrogen-containing gas was 950° C.
  • the specific carbon consumption reduction percentage Input ⁇ C is 7.0% or more.
  • the upper limit of the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is not separately set.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas may be 1000 Nm 3 /t or less.
  • the blast furnace operation simulation in a case where the blowing temperature of the high-concentration hydrogen-containing gas is 1200° C. and the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is 800 Nm 3 /t or more, the gas volume of the pulverized coal becomes 0, and it is possible to further reduce the specific carbon consumption by reducing a coke ratio.
  • a decrease in the coke ratio causes an increase in the pressure loss, resulting in unstable operation.
  • the pressure loss is a difference between the pressure at the tuyere tip (the outlet of the tuyere), in other words, the pressure inside the furnace at an outlet of the tuyere and the pressure at the top of the furnace, and a value excluding the pipe pressure loss from a blower to the tuyere tip.
  • the pressure loss is measured by a pressure gauge installed on a furnace wall portion.
  • the gas viscosity and the gas density in the furnace decrease significantly. Therefore, the concern about an increase in the pressure loss when the coke ratio is reduced is resolved, and the pressure loss is such that there is no problem with stable operation in the actual operation.
  • FIG. 14 is a graph showing the correlation between the gas volume of the pure hydrogen gas at 1200° C. and the change amount of the pressure loss inside the furnace when the flame temperature reaches 2100° C., which is obtained by the blast furnace operation simulation.
  • the pressure loss in normal operation is about 85 kPa as a standard. According to FIG. 14 , it can be seen that the pressure loss is less than 85 kPa under the operation conditions of the present embodiment.
  • the reduction percentage Input ⁇ C of the specific carbon consumption increases when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is increased from 0 Nm 3 /t Nm in the base operation. Then, in a case where the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is within a range of 100 Nm 3 /t or more, the reduction percentage Input ⁇ C of the specific carbon consumption is 7% or more. Moreover, similar to the case where the blowing temperature of the high-concentration hydrogen-containing gas becomes higher than 600° C. and 900° C.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas may be 1000 Nm 3 /t or less.
  • the upper limit of the blowing temperature is not particularly limited as long as the environment allows the blowing temperature of the high-concentration hydrogen-containing gas to exceed 600° C.
  • the effect of reducing the specific carbon consumption is almost unchanged in a range where the blowing temperature of the high-concentration hydrogen-containing gas is in a range of higher than 1200° C. to about 1400° C.
  • FIGS. 15 and 16 are graphs showing the correlation between the blowing temperature of the pure hydrogen gas and the gas volume of the pure hydrogen gas required to set the reduction percentage Input ⁇ C of the specific carbon consumption to 10% or 20%.
  • the flame temperature Tf was set to 2100° C.
  • the blowing temperature of the high-concentration hydrogen-containing gas may be 1400° C. or lower. That is, the blowing temperature of the high-concentration hydrogen-containing gas may be, for example, higher than 600° C. and 1400° C. or lower.
  • the high-concentration hydrogen-containing gas is blown from the tuyere at the determined blowing temperature and gas volume. Accordingly, the reduction percentage Input ⁇ C of the specific carbon consumption can be set to, for example, 7% or more, and the CO 2 emissions can be significantly reduced.
  • the tuyere for blowing the high-concentration hydrogen-containing gas is, for example, a tuyere for blowing hot blast provided at the lower part of the furnace. The present embodiment is described based on the premise that the high-concentration hydrogen-containing gas is blown from the tuyere for blowing hot blast. However, the tuyere for blowing the high-concentration hydrogen-containing gas is not limited to this.
  • the tuyere is so-called shaft tuyeres provided on a shaft portion.
  • the high-concentration hydrogen-containing gas may be blown into the blast furnace from any of these tuyeres or may be blown into the blast furnace from both tuyeres.
  • the total gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas blown from each tuyere matches the above-determined gas volume.
  • the operation of appropriately maintaining the top gas temperature is possible. For this reason, it is unnecessary to blow in the preheated gas or preheat the charges inside the furnace, which is performed to maintain the top gas temperature, but these may be separately performed.
  • the flame temperature Tf is maintained at 2050° C. or lower.
  • the flame temperature is an in-furnace temperature in a tip end portion of the tuyere on the inside of the furnace, and will also be referred to as “tuyere tip temperature Tf”.
  • the flame temperature Tf is calculated as a tuyere tip theoretical combustion temperature according to a Lamm equation described in “Ironmaking Handbook” (Chijinshokan Co., Ltd.), Akitoshi SHIGEMI.
  • the reduction percentage Input ⁇ C of the specific carbon consumption in a case where the flame temperature Tf is 2050° C. or lower (2000° C. in FIGS. 2 , 3 , 5 , 7 , and 9 ) is larger than the reduction percentage Input ⁇ C of the specific carbon consumption in a case where the flame temperature Tf is higher than 2050° C. (2100° C. and 2200° C. in FIGS. 2 , 3 , 5 , 7 , and 9 ).
  • the flame temperature Tf is maintained at 2050° C. or lower. Accordingly, the reduction percentage Input ⁇ C of the specific carbon consumption can be further increased.
  • the flame temperature Tf may be set to 2050° C. or lower.
  • the flame temperature Tf is lowered by blowing the high-concentration hydrogen-containing gas in the blast furnace.
  • the hot blast blown into the blast furnace is a gas including air.
  • the hot blast may include hygroscopic moisture and enriched oxygen in addition to air.
  • the oxygen enrichment ratio is adjusted by changing the flow rate of enriched oxygen in units of Nm 3 /t and the flow rate of air without changing the flow rate of oxygen, which is the total flow rate of the enriched oxygen in units of Nm 3 /t and oxygen in the hot blast.
  • the reduction percentage Input ⁇ C of the specific carbon consumption in a case where the flame temperature Tf is 2050° C. or lower is larger than the reduction percentage Input ⁇ C of the specific carbon consumption in a case where the flame temperature Tf is larger than 2050° C.
  • the flame temperature Tf is preferably 2000° C. or higher.
  • the flame temperature Tf may be lower than 2000° C.
  • the flame temperature Tf may be set to lower than 2000° C.
  • the gas volume of the pulverized coal is 0 (that is, the pulverized coal ratio is 0).
  • the flame temperature Tf can be set to lower than 2000° C. That is, if the gas volume of the pulverized coal can be set to 0 as a result of raising the blowing temperature of the high-concentration hydrogen-containing gas and increasing the gas volume, the flame temperature Tf may be set to lower than 2000° C.
  • the flame temperature Tf is maintained higher than 2050° C. and lower than 2150° C.
  • the reduction percentage Input ⁇ C of the specific carbon consumption can be increased by setting the flame temperature Tf to 2050° C. or lower.
  • the flame temperature Tf decreases, there is a possibility of the combustion rate of the pulverized coal decreasing. That is, when the flame temperature Tf decreases, the pulverized coal is unlikely to combust. In a case where the pulverized coal is flame-retardant or in a case where the operation is performed by increasing the pulverized coal ratio, the possibility of the combustion rate of the pulverized coal decreasing is further increased.
  • the flame temperature Tf is maintained higher than 2150° C.
  • the flame temperature Tf is often set to about 2200° C. Therefore, by setting the flame temperature Tf to higher than 2150° C., the operation can be performed without significantly changing the operation conditions from the related-art blast furnace operation.
  • the flame temperature Tf is preferably 2250° C. or lower.
  • the reduction percentage Input ⁇ C of the specific carbon consumption for each of several gas volumes is obtained by the blast furnace operation simulation in which the current blast furnace operation including the blowing temperature of the high-concentration hydrogen-containing gas is reflected.
  • the specific method may be the same as that of the examples described below.
  • the values obtained by the above method are plotted on a plane where the horizontal axis is the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas in units of Nm 3 /t and the vertical axis is the reduction percentage Input ⁇ C (%) of the specific carbon consumption.
  • the approximation curve from these plots may be obtained by, for example, the least squares method, and the approximation curve, more specifically, a relational expression showing the approximation curve, may be used as the above-described gas volume-specific carbon consumption reduction percentage correlation. It is preferable to obtain the gas volume and the specific carbon consumption reduction percentage correlation for each flame temperature Tf.
  • the gas volume at which the reduction percentage Input ⁇ C of the specific carbon consumption is larger than that of the current operation is determined on the basis of the gas volume-specific carbon consumption reduction percentage correlation obtained above.
  • the high-concentration hydrogen-containing gas is blown from the tuyere at the determined gas volume. Accordingly, the reduction percentage Input ⁇ C of the specific carbon consumption can be more reliably increased.
  • the gas volume-specific carbon consumption reduction percentage correlation in advance for each blowing temperature of the high-concentration hydrogen-containing gas. Accordingly, even in a case where the blowing temperature fluctuates, the desired gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas can be easily determined. That is, even in a case where the blowing temperature fluctuates, it is possible to easily determine the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas in which the reduction percentage Input ⁇ C of the specific carbon consumption becomes large.
  • FIG. 12 is a graph showing, for each flame temperature Tf, the correlation between the gas volume of the pure hydrogen gas at room temperature in units of Nm 3 /t and the change amount of the pressure loss in units of kPa with respect to the base operation, which is an operation in which the high-concentration hydrogen-containing gas is not blown.
  • This graph is obtained from a blast furnace operation simulation. The details will be described in the examples.
  • the pressure loss is a difference between the pressure at the tuyere tip (the outlet of the tuyere), in other words, the pressure inside the furnace at an outlet of the tuyere and the pressure at the top of the furnace, and a value excluding the pipe pressure loss from a blower to the tuyere tip.
  • the pressure loss is measured by a pressure gauge installed on a furnace wall portion.
  • the change amount of the pressure loss with respect to the base operation is a value obtained by subtracting the pressure loss during the base operation from the pressure loss during a certain operation. It is preferable that the pressure loss be almost the same as that of the base operation or a value lower than that of the base operation from the viewpoint of the restriction of the blast pressure, the prevention of blow-by, and the like.
  • FIG. 12 shows the above correlation in a case where the pure hydrogen gas at room temperature is used. The above correlation can also be obtained in a case where the high-concentration hydrogen-containing gas other than the pure hydrogen gas is used. Additionally, even when the blowing temperature of the high-concentration hydrogen-containing gas is higher than room temperature, the above correlation can be obtained.
  • the oxygen enrichment ratio is adjusted while the tapped iron amount is kept at a predetermined amount by changing the flow rate of enriched oxygen in units of Nm 3 /t and the flow rate of air without changing the flow rate of oxygen, which is the total flow rate of the enriched oxygen and oxygen in the hot blast in units of Nm 3 /t. Therefore, when the oxygen enrichment ratio increases, the flow rate of hot blast decreases. As a result, the amount of the Bosch gas decreases. In other words, in a case where the flame temperature Tf is low, the amount of the Bosch gas increases. As a result, there is a possibility of the pressure loss being larger than that of the base operation.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is further increased, the gas viscosity and gas density of the gas in the furnace are lowered, and the pressure loss is reduced. Then, the decrease in pressure loss caused by the decrease in gas viscosity and gas density offsets the increase in the pressure loss caused by the increase in the amount of the Bosch gas, and as a result, the pressure loss decreases.
  • the gas volume-specific carbon consumption reduction percentage correlation is obtained in advance similar to Modification Example 4. Moreover, a gas volume-pressure drop change correlation, which is the correlation between the gas volume and the change amount of the pressure loss with respect to the base operation, is obtained.
  • the change amount of the pressure loss for each of several gas volumes is obtained by the blast furnace operation simulation in which the current blast furnace operation including the blowing temperature of the high-concentration hydrogen-containing gas is reflected.
  • the specific method may be the same as that of the examples described below.
  • the values obtained by the above method are plotted on a plane where the horizontal axis is the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas in units of Nm 3 /t and the vertical axis is A pressure loss that is the change amount of the pressure loss in units of kPa.
  • the approximation curve from these plots may be obtained by, for example, the least squares method, and the approximation curve (more specifically, a relational expression showing the approximation curve) may be used as the above-described gas volume-pressure drop change correlation.
  • the gas volume-pressure drop change correlation is preferably obtained for each flame temperature Tf.
  • the reduction percentage Input ⁇ C of the specific carbon consumption is larger than that of the current operation, that is, the carbon consumption amount is reduced and the gas volume in which the change amount of the pressure loss is a value within a predetermined range is determined on the basis of the gas volume-specific carbon consumption reduction percentage correlation and the gas volume-pressure drop change correlation.
  • the predetermined range is, for example, about ⁇ 50 to +5 kPa, but is not limited to this.
  • the high-concentration hydrogen-containing gas is blown from the tuyere at the determined gas volume. Accordingly, the reduction percentage Input ⁇ C of the specific carbon consumption can be more reliably increased while the change amount of the pressure loss is set to a value within a predetermined range.
  • FIG. 13 is a graph showing the correlation between the gas volume of the pure hydrogen gas in units of Nm 3 /t at room temperature and the change amount of the top gas temperature with respect to the base operation in units of ° C. for each flame temperature Tf.
  • This graph is obtained from a blast furnace operation simulation.
  • the top gas temperature is the temperature of the furnace top gas (mainly CO 2 , N 2 , unreacted CO, or the like) discharged from the top of the blast furnace, and in the actual operation, is measured by a thermometer installed on a riser tube or the like.
  • the change amount of the top gas temperature with respect to the base operation is a value obtained by subtracting the top gas temperature during the base operation from the top gas temperature during a certain operation.
  • the top gas temperature is preferably almost the same as that of the base operation from the viewpoint of restrictions on furnace top equipment and efficient operation, and as an example, is preferably within a range of about ⁇ 20° C. from the top gas temperature of the base operation.
  • FIG. 13 shows the above correlation in a case where the pure hydrogen gas at room temperature is used The above correlation can also be obtained in a case where the high-concentration hydrogen-containing gas other than the pure hydrogen gas is used. Additionally, even when the blowing temperature of the high-concentration hydrogen-containing gas is higher than room temperature, the above correlation can be obtained.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas decreases as described above.
  • the flame temperature Tf decreases as described above.
  • the oxygen enrichment ratio is adjusted by changing the flow rate of air in units of Nm 3 /t without changing the flow rate of oxygen in units of Nm 3 /t. Therefore, when the oxygen enrichment ratio increases, the flow rate of hot blast decreases. As a result, the amount of the Bosch gas decreases.
  • the operation is performed by increasing the reducing material ratio.
  • the reducing material ratio is increased, the amount of heat input into the furnace increases and the top gas temperature tends to rise. Therefore, the top gas temperature starts to increase.
  • the gas volume-specific carbon consumption reduction percentage correlation is obtained in advance similar to Modification Example 4. Moreover, a gas volume-top gas temperature change amount correlation, which is the correlation between the gas volume and the change amount of the top gas temperature with respect to the base operation, is obtained.
  • the change amount of the top gas temperature for each of several gas volumes is obtained from the blast furnace operation simulation in which the current blast furnace operation including the blowing temperature of the high-concentration hydrogen-containing gas is reflected.
  • the specific method may be the same as that of the examples described below.
  • the values obtained by the above method are plotted on a plane where the horizontal axis is the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas in units of Nm 3 /t and the vertical axis in the unit kPa is A top gas temperature that is the change amount of the top gas temperature in units of ° C.
  • the approximation curve from these plots may be obtained by, for example, the least squares method, and the approximation curve, more specifically, a relational expression showing the approximation curve, may be used as the above-described gas volume-top gas temperature change amount correlation.
  • the gas volume-top gas temperature change amount correlation is preferably obtained for each flame temperature Tf.
  • the gas volume in which the reduction percentage Input ⁇ C of the specific carbon consumption is larger than that of the current operation, that is, the carbon consumption amount is reduced and in which the change amount of the top gas temperature is a value within a predetermined range is determined on the basis of the gas volume-specific carbon consumption reduction percentage correlation and the gas volume-top gas temperature change amount correlation.
  • the predetermined range is, for example, about ⁇ 20 to +20° C., but is not limited thereto.
  • the high-concentration hydrogen-containing gas is blown from the tuyere at the determined gas volume. Accordingly, the reduction percentage Input ⁇ C of the specific carbon consumption can be more reliably increased while the change amount of the top gas temperature is set to a value within a predetermined range.
  • the parameter paired with the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is not necessarily limited to the reduction percentage Input ⁇ C of the specific carbon consumption. That is, the parameter paired with the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas may be any parameter related to the carbon consumption amount, that is, any carbon consumption parameter. This is because if the carbon consumption amount is reduced, the CO 2 emissions can be reduced.
  • Examples of such a carbon consumption parameter include the specific carbon consumption, the reducing material ratio, the reduction percentage of the reducing material ratio, and the like in addition to the reduction percentage Input ⁇ C of the specific carbon consumption.
  • the reduction percentage of the reducing material ratio is the reduction percentage of the reducing material ratio with respect to the base operation, and the calculation method is the same as the calculation method of the reduction percentage Input ⁇ C of the specific carbon consumption.
  • Modification Example 5 and Modification Example 6 may be combined with each other. Accordingly, the reduction percentage Input ⁇ C of the specific carbon consumption can be more reliably increased while the change amount of the pressure loss and the change amount of the top gas temperature are set to values within a predetermined ranges.
  • Example 1 Verification in a Case where Blowing Temperature of High-Concentration Hydrogen-Containing Gas is Room Temperature to 600° C.
  • Example 1 As described above, the correlation between the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas and the reduction percentage Input ⁇ C of the specific carbon consumption shows a different behavior with the blowing temperature of 600° C. as a boundary. Thus, in Example 1, verification was performed in a case where the blowing temperature of the high-concentration hydrogen-containing gas was 600° C. or lower.
  • blast furnace operation simulation As the blast furnace operation simulation, a so-called “Blast Furnace Mathematical Model” Kouji TAKATANI, Takanobu INADA, Yutaka UJISAWA, “Three-dimensional Dynamic Simulator for Blast Furnace”, ISIJ International, Vol. 39 (1999), No. 1, pp. 15 to 22 was used.
  • this blast furnace mathematical model an internal region of the blast furnace is divided in a height direction, a radial direction, and a circumferential direction to define a plurality of meshes (small regions), and the behavior of each of the meshes is simulated.
  • the gas volume of the high-concentration hydrogen-containing gas is set as the amount of the high-concentration hydrogen-containing gas blown from the tuyere.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is set as the amount obtained by multiplying the gas volume of the high-concentration hydrogen-containing gas by the ratio of the hydrogen gas in units of mol %.
  • the blowing temperature of the high-concentration hydrogen-containing gas is set as the temperature of the high-concentration hydrogen-containing gas when the high-concentration hydrogen-containing gas is blown from the tuyere.
  • the flame temperature Tf is calculated as a result of considering the combustion heat of various gases, the sensible heat of blast, the temperature of the coke flowing into the tuyere tip (the outlet of the tuyere), various reaction heats, and the like.
  • the pressure loss is calculated using the Ergun equation as the pressure loss of a packed bed inside the furnace.
  • the top gas temperature is calculated as the gas temperature in the outermost layer (uppermost layer) of the charges inside the furnace.
  • the calculation conditions are shown in Table 1.
  • the coke ratio in Table 1 is the amount of coke used per ton of molten iron.
  • Table 2 shows the specifications of the base operation in which high-concentration hydrogen-containing gas is not blown in.
  • the flame temperature Tf was set to any of 2000° C., 2100° C., or 2200° C.
  • the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas was set to 0 to 600 Nm 3 /t.
  • the blast volume, the oxygen enrichment ratio, and the gas volume of PC were adjusted such that the tapped iron ratio and the molten iron temperature were constant in all operations.
  • the iron-bearing materials were all sintered ores. Additionally, the composition of the sintered ores was T-Fe: 58.5%, FeO: 7.5%, C/S: 1.9, and Al 2 O 3 : 1.7%. Additionally, regarding coke, a case where C: 87.2% and ash: 12.6% was used was assumed. In addition, all of the above “%” represent “mass %”.
  • Example 1-1 Case where Blowing Temperature of High-Concentration Hydrogen-Containing Gas is Room Temperature to 600° C. and High-Concentration Hydrogen-Containing Gas is Pure Hydrogen Gas
  • Example 1-1 the correlation between the gas volume of the pure hydrogen gas and the reduction percentage Input ⁇ C of the specific carbon consumption was calculated using the high-concentration hydrogen-containing gas as the pure hydrogen gas, under the condition that the blowing temperature of the high-concentration hydrogen-containing gas was 600° C. or lower. The results are shown in FIGS. 2 to 5 .
  • the reduction percentage Input ⁇ C of the specific carbon consumption does not simply increase with an increase in the gas volume but reaches saturation and starts to decrease when the gas volume of air increases to some extent. Then, it was found that the gas volume when the reduction percentage Input ⁇ C of the specific carbon consumption reaches saturation and starts to decrease is slightly different depending on the blowing temperature. That is, it was found that an appropriate range of the gas volume is present for each blowing temperature. The appropriate range was 200 to 500 Nm 3 /t in a case where the blowing temperature was room temperature to 300° C.
  • the reduction percentage Input ⁇ C of the specific carbon consumption does not simply increase with an increase in the gas volume but reaches saturation at a gas volume of about 600 Nm 3 /t when the blowing temperature is 600° C. and starts to decrease with an increase in the gas volume at a gas volume peak of about 300 Nm 3 /t when the blowing temperature is 350° C. Also, in a case where the blowing temperature is higher than 300° C. and 600° C.
  • the reduction percentage Input ⁇ C of the specific carbon consumption can be increased, and the CO 2 emissions can be significantly reduced.
  • Example 1-2 it was confirmed that even if the high-concentration hydrogen-containing gas contains a gas component other than the hydrogen gas, the same operation as in the case of the pure hydrogen gas is possible. Specifically, 80 mol % H 2 -20 mol % N 2 gas composed of 80 mol % hydrogen gas and 20 mol % nitrogen gas was assumed as the high-concentration hydrogen-containing gas. Then, the blast furnace operation simulation was performed in the same manner as in Example 1 with the blowing temperature set to 25° C. and the flame temperature Tf set to 2100° C. The results are shown in FIG. 11 . FIG.
  • FIG. 11 shows a comparison between the calculation result of the pure hydrogen gas (100 mol % H 2 gas) and the calculation result of 80 mol % H 2 -20 mol % N 2 gas.
  • the horizontal axis in FIG. 11 represents a value obtained by converting the flow rate of a mixed gas in the pure hydrogen gas, that is, a value obtained by multiplying the flow rate of 80 mol % H 2 -20 mol % N 2 gas by 80 mol %.
  • Example 1-3 the pure hydrogen gas at room temperature was used as the high-concentration hydrogen-containing gas, and the change amount of the pressure loss with respect to each of several gas volumes (the change amount of the pressure loss with respect to the base operation) was obtained.
  • FIG. 12 shows the results. As is clear from FIG. 12 , it was found that there is a certain correlation between the gas volume of the pure hydrogen gas and the change amount of the pressure loss. For example, it was found that there is a possibility of the pressure loss being large with respect to the base operation in a case where the flame temperature Tf is low. However, the pressure loss decreases when the gas volume of the pure hydrogen gas increases. More specifically, in a case where the flame temperature Tf is 2000° C.
  • the pressure loss increases by about 10 to 20 kPa as compared to the base operation. This is a value outside the predetermined range described above. However, when the gas volume increases to 200 Nm 3 /t or more, the pressure loss is almost the same as or less than the value of the base operation. The reason why such a phenomenon occurs is as described above.
  • the gas volume-pressure drop change correlation which is the correlation between the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas and the change amount of the pressure loss with respect to the base operation when the blowing temperature is a predetermined value, in advance for each flame temperature Tf and by determining the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas at which the carbon consumption amount is reduced compared to that of the current operation, and the change amount of the pressure loss is a value within a predetermined range on the basis of the gas volume-carbon consumption parameter correlation and the gas volume-pressure drop change correlation.
  • Example 1-4 the pure hydrogen gas at room temperature was used as the high-concentration hydrogen-containing gas, and the change amount of the top gas temperature with respect to each of several gas volumes (the change amount of the top gas temperature with respect to the base operation) was obtained.
  • FIG. 13 shows the results.
  • the change amount of the top gas temperature is a value outside the above-described predetermined range.
  • the gas volume may be adjusted in consideration of the correlation between the gas volume of the pure hydrogen gas and the change amount of the top gas temperature.
  • the gas volume-top gas temperature change amount correlation which is the correlation between the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas and the change amount of the top gas temperature with respect to the base operation when the blowing temperature is a predetermined value, in advance for each flame temperature Tf and by determining the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas at which the carbon consumption amount is reduced compared to that of the current operation, and the change amount of the top gas temperature is a value within a predetermined range on the basis of the gas volume-carbon consumption parameter correlation and the gas volume-top gas temperature change amount correlation.
  • Example 2 Verification in Case where Blowing Temperature of High-Concentration Hydrogen-Containing Gas is Higher than 600° C.
  • Example 2 a case where the blowing temperature of the high-concentration hydrogen-containing gas is higher than 600° C. was verified.
  • Example 3 In the blast furnace operation simulation, the same “blast furnace mathematical model” as in Example 1 was used. Calculation conditions are shown in Table 3. As shown in Table 3, the calculation conditions were almost the same as those in Example 1, but the coke ratio was different from that in Example 1. That is, in Example 2, the coke ratio was constant at 300 kg/t in a case where the pulverized coal gas volume was larger than 0 tons/h, and the coke ratio fluctuated in a case where the pulverized coal gas volume was 0 tons/h (that is, in a case where the pulverized coal ratio was 0). That is, in a case where the gas volume of the pulverized coal was 0 tons/h, the furnace temperature was adjusted according to the coke ratio.
  • the gas volume of the pulverized coal may be 0 tons/h. In this case, by reducing the coke ratio, it is possible to further reduce the specific carbon consumption. Additionally, the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas was set to 0 to 1000 Nm 3 /t. Additionally, the blowing temperature of the high-concentration hydrogen-containing gas was set to higher than 600° C. and 1400° C. or less. In addition, the specifications of the base operation in which the high-concentration hydrogen-containing gas was not blown were the same as in Example 1. Other conditions were the same as those of Example 1. For example, the blast volume, the oxygen enrichment ratio, and the gas volume of PC (pulverized coal) were adjusted such that the tapped iron ratio and the molten iron temperature were constant in all operations. The iron-bearing materials were sintered ore used in Example 1.
  • Example 2-1 Case where Blowing Temperature of High-Concentration Hydrogen-Containing Gas is Higher than 600° C. and High-Concentration Hydrogen-Containing Gas is Pure Hydrogen Gas
  • Example 2-1 the correlation between the gas volume of the pure hydrogen gas and the reduction percentage Input ⁇ C of the specific carbon consumption was calculated using the high-concentration hydrogen-containing gas as the pure hydrogen gas. The results are shown in FIGS. 6 to 10 .
  • the reduction percentage Input ⁇ C of the specific carbon consumption increases when the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas is increased from 0 Nm 3 /t in the base operation. Moreover, as the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas increases, the increase rate of the reduction percentage Input ⁇ C of the specific carbon consumption (increase amount of the reduction percentage Input ⁇ C of the specific carbon consumption to the unit increase amount of the gas volume) decreases. However, the reduction percentage Input ⁇ C of the specific carbon consumption did not start to decrease. This behavior was clearly different from the case where the blowing temperature of the high-concentration hydrogen-containing gas was 600° C. or lower.
  • a range where the reduction percentage Input ⁇ C of the specific carbon consumption was 7% or more was different depending on the blowing temperature of the high-concentration hydrogen-containing gas. Specifically, in a case where the blowing temperature was higher than 600° C. and 900° C. or lower and in a case where the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas was within a range of 125 Nm 3 /t or more, the reduction percentage Input ⁇ C of the specific carbon consumption was 7% or more. Additionally, in a case where the blowing temperature was higher than 900° C. and 1200° C.
  • the reduction percentage Input ⁇ C of the specific carbon consumption was 7% or more.
  • the blowing temperature was higher than 1200° C. and in a case where the gas volume of the hydrogen gas in the high-concentration hydrogen-containing gas was within a range of 100 Nm 3 /t or more, the reduction percentage Input ⁇ C of the specific carbon consumption was 7% or more.

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US20240218472A1 (en) * 2021-06-28 2024-07-04 Jfe Steel Corporation Supplied heat quantity estimation method, supplied heat quantity estimation device, supplied heat quantity estimation program, and blast furnace operation method
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JPS5315732B2 (zh) 1973-09-27 1978-05-26
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IT1212372B (it) 1979-09-26 1989-11-22 Abc Ist Biolog Chem Spa Composizioni farmaceutiche ad atti vita' antiulcera contenenti un derivato dell'acido acetoidrossamico
JPS5887210A (ja) * 1981-11-18 1983-05-25 Kawasaki Steel Corp 高炉操業方法
JP2668486B2 (ja) * 1992-08-11 1997-10-27 新日本製鐵株式会社 水素ガス利用率を用いた高炉操業方法
JP3183226B2 (ja) * 1996-09-20 2001-07-09 住友金属工業株式会社 廃棄物のガス化溶融炉およびガス化溶融方法
JP4984396B2 (ja) * 2005-01-31 2012-07-25 Jfeスチール株式会社 高炉操業方法
JP5050706B2 (ja) 2007-07-25 2012-10-17 住友化学株式会社 タンクのベントガスの処理方法
JP5315732B2 (ja) 2008-03-17 2013-10-16 Jfeスチール株式会社 高炉操業方法
JP4661890B2 (ja) * 2008-03-17 2011-03-30 Jfeスチール株式会社 高炉操業方法
BRPI1011905B1 (pt) * 2009-04-30 2018-02-06 Jfe Steel Corporation Método de operação de alto-forno, usina de alto- forno e método de combustão de gás de valor calorífico baixo com uso de um queimador de combustão
JP5708029B2 (ja) * 2011-02-25 2015-04-30 Jfeスチール株式会社 高炉操業方法
EP2796566B1 (en) * 2011-12-21 2018-08-29 JFE Steel Corporation Blast furnace operation method
JP5851828B2 (ja) 2011-12-22 2016-02-03 Jfeスチール株式会社 燃焼性ガスの製造方法
JP5770124B2 (ja) 2012-03-06 2015-08-26 新日鐵住金株式会社 高炉操業方法
JP6019893B2 (ja) 2012-07-31 2016-11-02 Jfeスチール株式会社 高炉の操業方法
JP5987773B2 (ja) 2013-04-19 2016-09-07 Jfeスチール株式会社 高炉操業方法
KR20160120334A (ko) * 2014-03-26 2016-10-17 제이에프이 스틸 가부시키가이샤 산소 고로의 조업 방법
CN107408985B (zh) 2015-03-18 2020-02-21 日本电气株式会社 光传送系统及其分析方法、终端站设备和管理设备
US10961596B2 (en) * 2016-02-05 2021-03-30 Nippon Steel Corporation Method for supplying hydrogen-containing reducing gas to shaft part of blast furnace
CN106282455B (zh) * 2016-03-01 2018-06-15 华北理工大学 一种高效利用冶金废气的高炉富氢冶炼工艺
JP6717629B2 (ja) * 2016-03-25 2020-07-01 日本製鉄株式会社 高炉シャフト部への水素含有還元ガス供給方法
HUE057873T2 (hu) * 2017-07-03 2022-06-28 Air Liquide Eljárás vas- vagy acélmû mûködtetésére
JP7043352B2 (ja) 2018-06-14 2022-03-29 キヤノン電子管デバイス株式会社 電源装置及び回転陽極x線管装置

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