Jinglan Hu1, Yuelin Qin1,2, Xin Li1, Haowen Liu1, Yin Deng1, Hao Liu1,2. 1. School of Metallurgy and Materials Engineering, Chongqing University of Science and Technology, Chongqing401331, China. 2. Value-Added Process and Clean Extraction of Complex Metal Mineral Resources, Chongqing Municipal Key Laboratory of Institutions of Higher Education, Chongqing401331, China.
Abstract
Through thermodynamic calculation and high-temperature simulation experiments, the coupling behavior between gasification of high- and low-reactivity cokes and reduction of sintering ore in CO-N2-H2 mixed gas with 25% H2 volume fraction was studied, and the evolution of the coke carbon structure and the pore structure was analyzed. The results show that the reaction rate of the two cokes increases with the increase in temperature after the coupling reaction, and the strength after drumming decreases with the increase in temperature. The strength of low-reactivity coke after the reaction is higher than that of high-reactivity coke, and the reduction degree of sintering ore after the coupling reaction with low-reactivity coke is higher than that with high-reactivity coke. At high temperatures and high hydrogen-rich atmospheres with φ(H2) of 25%, the strength of high-reactivity coke after drum rotation is greater than 60.4%. The graphitization degree and carbon structure order of low-reactivity coke are higher than those of high-reactivity coke.
Through thermodynamic calculation and high-temperature simulation experiments, the coupling behavior between gasification of high- and low-reactivity cokes and reduction of sintering ore in CO-N2-H2 mixed gas with 25% H2 volume fraction was studied, and the evolution of the coke carbon structure and the pore structure was analyzed. The results show that the reaction rate of the two cokes increases with the increase in temperature after the coupling reaction, and the strength after drumming decreases with the increase in temperature. The strength of low-reactivity coke after the reaction is higher than that of high-reactivity coke, and the reduction degree of sintering ore after the coupling reaction with low-reactivity coke is higher than that with high-reactivity coke. At high temperatures and high hydrogen-rich atmospheres with φ(H2) of 25%, the strength of high-reactivity coke after drum rotation is greater than 60.4%. The graphitization degree and carbon structure order of low-reactivity coke are higher than those of high-reactivity coke.
In recent years, various
environmental problems caused by the greenhouse
effect have attracted worldwide attention. The iron and steel industry
is an important basic industry in the industrialized countries of
the world, and it is also an industry with high energy consumption
and high pollution. Blast furnace ironmaking is the main source of
molten iron in steel production and has not been replaced by other
processes. The consumption of fossil fuels such as coke in a blast
furnace is an important source of carbon dioxide emissions. It is
very difficult to excavate the energy-saving and emission reduction
potential of traditional production processes through advanced technology.
Hydrogen, as a reducing agent, causes no pollution and is an ideal
substitute for carbon. Therefore, some researchers have proposed a
hydrogen metallurgy process represented by blast furnace hydrogen-rich
smelting technology, including blast furnace injection of coke oven
gas,[1−4] coal manufacturing gas, and natural gas,[5,6] or
other hydrogen-containing substances.[7,8]After
the blast furnace is rich in hydrogen, the deterioration
of coke in the blast furnace is mainly caused by the dissolution reaction.
There are two different cases of coke dissolution reaction: one is
the carbon dissolution reaction between coke and CO2, and
the other is the water-gas reaction between coke and H2O. At present, researchers have mainly explored the effects of pure
H2O, pure CO2, or their mixture on the dissolution
behavior and performance of coke. Wang et al. found that the temperature
loss of coke caused by H2O was about 37 °C and 125
°C lower than that caused by CO2.[9−11] The gasification
rate of coke with H2O was about 1.27–3.16 times
higher than that of CO2, and the location of the gasification
reaction between coke and H2O was closer to the outside
of coke. Chang et al. studied the effects of CO2 and H2O on gasification dissolution and the deep reaction of coke.
The results show that the average reaction rate of coke with H2O is about 1.3–6.5 times that of CO2 at
950–1250 °C. With the increase of pressure, the gasification
dissolution reaction of coke transfers to a high-temperature zone.[12] Zhang studied the kinetics of the coke gasification
reaction in CO2–CO–N2 with or
without H2 by thermogravimetry. When the temperature is
low, the gasification rate with hydrogen is significantly higher than
that without hydrogen.[13] In addition, some
researchers also comparatively analyzed the effects of H2O and CO2 on the microstructure of coke and pointed out
that the damage of H2O on the coke structure was greater
than that of CO2, and the erosion of H2O on
the coke pore wall was more serious.[14−17] Whether the reactivity of coke
is an important factor that determines the performance of blast furnaces
has always been the subject of debate. Low-reactivity coke is widely
used as the main reducing agent for blast furnace ironmaking in the
steel industry. However, relevant theoretical research and production
practice have demonstrated that it is feasible to use high-reactivity
coke for hydrogen-rich blast furnaces.[18−22]The above literature shows that these studies
focus on the influence
of pure CO2 and pure H2O on the coke gasification
reaction and iron-bearing material reduction. In the actual production
process of a blast furnace, CO2 and H2O produced
by iron oxide reduction are the main sources of the coke gasification
reaction due to the special arrangement between an iron-bearing material
such as sintering ore and coke. Therefore, the dissolution loss behavior
of coke in a blast furnace is closely related to the reduction of
the iron-bearing material. However, there are few studies on this
aspect, and the analysis of the dissolution loss behavior of coke
during the coupling reaction of coke and an iron-bearing material
such as sintering ore is lacking. Especially, after the blast furnace
is rich in hydrogen, the H2 content of the bosh gas can
reach 14–20%, and its indirect reduction with iron ore produces
a large amount of H2O, which has a more obvious influence
on coke performance.[15] Therefore, based
on the hydrogen-rich smelting of the blast furnace, the coupling effects
of iron oxide reduction and coke gasification under different φ(H2) were analyzed by thermodynamic calculation. The coupling
behavior of high- and low-reactivity coke gasification and sintering
ore reduction under a high hydrogen-rich atmosphere (φ(H2) = 25%) was studied by a high-temperature reduction experiment.
It is expected that the research results can provide a reliable theoretical
basis for the application of blast furnace hydrogen-rich smelting
technology and high-reactivity coke.
Thermodynamic Analysis of Coupling Reaction
The main gas components in a hydrogen-rich BF include N2, H2, H2O, CO, and CO2. N2 is not involved in the reaction; CO and H2 are involved
in the reduction of iron oxides to produce CO2 and H2O, respectively. The gasification reaction of CO2 and H2O with coke is an important cause of coke deterioration.
Therefore, there is a coupling effect between coke gasification and
sintering ore reduction in a hydrogen-rich BF. As shown in Table , the reduction reaction
of iron oxide and the gasification reaction of coke in a BF are listed,
in which the reduction reaction of Fe2O3 is
ignored because the reaction is irreversible.
Table 1
Main Chemical Reaction Equations
chemical reaction equations
ΔrGmθ
–8287 + 9.993T
29 369 – 25.07T
–18 628 + 22.17T
16 826 – 10.30T
26 044 – 30.44T
61 473 – 62.88T
166 500 – 171T
133 100 – 141.63T
The thermodynamic equilibrium diagram of the coupling
reaction
between iron oxide reduction and coke gasification at different H2 volume fractions (φ(H2)) was calculated
and drawn using thermodynamic software (FactSage) under atmospheric
pressure, as shown in Figure . In the thermodynamic calculation process, the total amount
of the initial reducing gas was set to be 1 mol, and the initial atmosphere
of the reaction was CO–H2–N2,
where the volume fraction of CO was fixed at 42%. The reduction reactions
of iron oxide were investigated when the volume fractions of H2 were 0, 5, 15, and 25%. Then, according to the volume fractions
of CO and H2, the gasification reactions of CO2 and H2O generated after iron oxide reduction with coke
in Table were calculated
in equal proportion.
Figure 1
Thermodynamic equilibrium diagram of the coupling reaction
between
iron oxide reduction and coke gasification under different φ(H2).
Thermodynamic equilibrium diagram of the coupling reaction
between
iron oxide reduction and coke gasification under different φ(H2).In Figure , when
the temperature is less than 1100 K, the concentration of reducing
gas in the system increases when the iron oxide reduction reaction
reaches equilibrium with the increase of the H2 volume
fraction (φ(H2)) in the initial reaction gas. According
to the principle of minimum free energy, it is not conducive to the
further reduction of iron oxide, and the reduction reaction is mainly
controlled by CO. Additionally, CO2 and H2O
generated by the reduction of iron oxide also decreased, resulting
in the inhibition of coke gasification. However, when the temperature
is greater than 1100 K, the corresponding thermodynamic calculation
results are reversed. This is consistent with the thermodynamic results
calculated by Lan et al. under different φ(CO)/φ(H2).[23]The preceding results
demonstrate that the arrangement of iron
ore and coke layers in a blast furnace causes a coupling effect between
coke gasification and sintering ore reduction. In a hydrogen-rich
BF, when the contents of CO and H2 change, the contents
of CO2 and H2O generated in the reduction process
of iron ore are directly affected, thereby affecting the gasification
reaction of coke. The thermodynamic method can only determine the
energy relationship and the direction and limit of the change, but
it does not involve the steps, rate, and process mechanism. Consequently,
it is necessary to explore the coupling behavior of typical coke gasification
and sintering ore reduction by simulating the atmosphere of a hydrogen-rich
BF.
Experimental Section
Materials
The cokes used in the study
are of two kinds with obvious reactivity differences, which are low-reactivity
coke from Chongqing Iron and Steel Company (L-R coke) and high-reactivity
coke from Xinjiang Bayi Iron and Steel Company (H-R coke). The sintering
ore from Xinjiang Bayi Iron and Steel Company and its chemical composition
analysis are shown in Table . The coke reactivity index (CRI), strength after reaction
(CSR), and industrial analysis results are shown in Table . The meaning of the abbreviations
used in this paper is shown in Table .
Table 2
Chemical Composition of Sintering
Ore (%)
TFe
Al2O3
CaO
MgO
SiO2
FeO
S
P
54.7
1.01
11.1
1.7
5.97
9.52
0.046
0.093
Table 3
Industrial Analysis, CRI, and CSR
of Coke
industrial
analysis (%)
name
Mad
Vad
Ad
FCd
CRI (%)
CSR (%)
H-R coke
0.36
1.17
12.05
86.66
53.40
20.82
L-R coke
0.58
1.87
11.77
85.78
25.20
65.24
Table 4
Description of the Meaning of Abbreviations
abbreviation
implication
CRI
coke reactivity
index under the GB/T4000-2008 standard
test method
CSR
strength index
of coke after reaction under the GB/T4000-2008 standard test method
CRE
reaction rate of coke after the coupling reaction of coke gasification
and sintering ore reduction
CTS
strength of coke after drum rotation after the coupling reaction
of coke gasification and sintering ore reduction
RIt
reduction degree
of sinter after the coupling reaction of coke
gasification and sintering ore reduction
Experimental Apparatus
The schematic
diagram of the device for the coupling reaction experiment is shown
in Figure , which
is mainly composed of a reaction furnace, gas distribution system,
control system, and flue gas analysis system. The reaction tube is
a Φ80 × 5 × 800 mm3 fused corundum tube.
Figure 2
Schematic
diagram of the experimental apparatus for the coupling
reaction. 1, CO; 2, H2; 3, N2; 4, mass flowmeter;
5, gas outlet; 6, gas purification device; 7, gas analyzer; 8, water-cooled
cover; 9, coke; 10, sintering ore; 11, high-Al ball; 12, gas inlet;
13, thermocouple; 14, heater; and 15, furnace controller.
Schematic
diagram of the experimental apparatus for the coupling
reaction. 1, CO; 2, H2; 3, N2; 4, mass flowmeter;
5, gas outlet; 6, gas purification device; 7, gas analyzer; 8, water-cooled
cover; 9, coke; 10, sintering ore; 11, high-Al ball; 12, gas inlet;
13, thermocouple; 14, heater; and 15, furnace controller.
Experimental Methods
The sintering
ore and coke were ground to 23–25 mm diameter and dried at
378 ± 5 K for 2 h. The ratio of sintering ore to coke was 4:1,
that is, 200 ± 0.5 g coke and 800 ± 0.5 g sintering ore.
The sintering ore and coke were charged into the reaction tube with
the furnace heating up. Coke was in the upper layer, sintering ore
was in the lower layer, and the heating rate was 10 K/min. When the
temperature rose to 400 °C, the protective gas N2 (2
L/min) was introduced. N2 was stopped when the temperature
reached the experimental predetermined temperature (800–1100
°C). At the predetermined temperature, the reaction gas (CO/N2/H2 = 42%:33%:25%) was injected at a flow rate
of 5 L/min, and the purity of the gas was 99.99%. After a constant
temperature reaction for 4 h, the heating was stopped and N2 (2 L/min) was introduced into the cooling process. The content of
each component in the mixture was controlled by adjusting the gas
flow rate during the experiment. When the temperature of the reaction
tube was lower than room temperature (25 °C), the coke and sintering
ore were taken out and weighed, separately, and then, the thermal
strength of the coke was measured. All of the coke after the reaction
was charged into the I-type drum and rotated at a speed of 20 rpm/min
for 600 rpm. The coke was taken out for screening and weighed with
a 10 mm round hole. The CTS of coke and CRE of coke after the reaction
were calculated by formulas and 10, respectively. In addition, the
RI of sintering ore after the coupling reaction was calculated by formula as followswhere m0 is the
mass of coke before the reaction (g) and m1 is the mass of coke after the coupling reaction (g).where m2 is the
mass of gasified coke with a size larger than 10 mm after the drum
test (g).where M0 is the
mass of sintering ore before reduction (g), M is the mass of sintering ore after t min of experiment
(g), and W1 and W2 are the FeO and TFe content of sintering ore before experiment,
respectively (%).
Results and Discussion
Gasification of Typical Coke and Reduction
of Sintering Ore after Coupling Reaction
Figure shows the relationship between
CRE and temperature after the coupling reaction. As shown in Figure , when φ(H2) is 25% in a high hygrogen-rich atmosphere, the CRE of both
cokes increases with increasing temperature, especially when the temperature
is higher than 900 °C, which indicates that the higher the temperature
is, the more likely coke gasification occurs and the higher the reactivity
of coke is. This is because after H2 participates in the
indirect reduction of sintering ore, a large amount of H2O will be produced, and H2O reacts with coke by water-gas
reaction, which aggravates the deterioration of coke, which is consistent
with the results of the thermodynamic calculation. When the temperature
is lower than 900 °C, the change of CRE of the two cokes is not
particularly obvious, and it is speculated that this is mainly affected
by the thermodynamic conditions of the reaction.
Figure 3
Relationship between
CRE and temperature after the coupling reaction.
Relationship between
CRE and temperature after the coupling reaction.When the reaction temperature is less than 1000
°C, the CRE
of L-R coke is slightly higher than that of H-R coke. When the reaction
temperature is higher than 1000 °C, the CRE of L-R coke is lower
than that of H-R coke. The difference in CRE between L-R coke and
H-R coke under a simulated BF atmosphere is not substantial.Figure shows the
relationship between CTS and temperature after the coupling reaction.
As shown in Figure , with the increase in reaction temperature, the strength of H-R
coke and L-R coke after the coupling reaction decreased significantly,
and the dissolution loss was considerable, especially when the temperature
was higher than 900 °C. The analysis shows that with the increase
in reaction temperature, H2O produced by sintering ore
reduction in the lower part of the reaction tube increases, and the
water-gas reaction gets triggered at a high temperature. The dissolution
loss of coke is affected by H2O and CO2, which
leads to the decrease of coke strength after hydrogen enrichment.
The diagram of the coupling reaction between coke gasification and
sinter reduction is shown in Figure .
Figure 4
Relationship between CTS and temperature after the coupling
reaction.
Figure 5
Diagram of coupling reaction between coke gasification
and sintering
ore reduction.
Relationship between CTS and temperature after the coupling
reaction.Diagram of coupling reaction between coke gasification
and sintering
ore reduction.The difference in CRI and CSR between H-R coke
and L-R coke was
28.2 and 44.42%, respectively, under the national standard test conditions.
The CRE of H-R coke and L-R coke after the coupling reaction with
sintering ore was negatively correlated with CTS under the atmosphere
of φ(H2) = 25%. The difference between CRE and CTS
of H-R coke and L-R coke was not obvious, especially when the temperature
was lower than 1000 °C. Although the CTS of H-R coke is 60.4%
at 1100 °C, it still meets the requirements of a BF for metallurgical
coke strength.The results of the national standard experiment
are quite different
from the experimental results of this paper. The reason may be that
the dissolution reaction of coke is only carried out by pure CO2 under the national standard experimental conditions, and
the coupling reaction between iron-bearing raw materials such as sintering
ore and coke is ignored, which is inconsistent with the actual conditions
of BF production. CO2 and H2O produced by indirect
reduction of iron-bearing raw materials such as sintering ore with
CO and H2 are the main causes of coke dissolution loss.
It can be seen that the reactivity (CRI) obtained under the national
standard test conditions and the strength (CSR) after reaction may
mislead the evaluation of high-reactivity coke. When the temperature
and atmosphere are close to those of the BF, the test of coke reactivity
and strength is more reliable.Figure shows the
relationship between RI and temperature
after the coupling reaction. It can be seen from Figure that it does not change significantly
with temperature after the coupling reaction between sintering ore
and L-R coke, all above 98%. When the temperature is lower than 900
°C, the RI of the coupling reaction
between H-R coke and sintering ore is lower than that of L-R coke,
but when the temperature is higher than 900 °C, the difference
between them is not obvious. The reason is that the reaction rate
(CRE) of H-R coke gradually increases with the increase of temperature,
that is, the reduction gases CO and H2 produced by the
gasification reaction of H-R coke with CO2 and H2O increase, thus improving the reduction of sintering ore. Therefore,
the coupling effect of H-R coke and sintering ore promotes the reduction
of sinter. This is similar to the research results of Kashihara et
al.[24] Through experiments and mathematical
model analysis, they found that the reduction rate of ore and the
gasification rate of coke in the mixed layer of ore and coke were
accelerated due to the mutual utilization of the gases produced by
the reaction.
Figure 6
Relationship between RI and
temperature
after the coupling reaction.
Relationship between RI and
temperature
after the coupling reaction.
Effect of Temperature on the Carbon Structure
of Coke
The peak fitting method was used to distinguish the
peaks with the diffraction angle of 18–32° in the XRD
spectrum. After peak fitting, XRD spectra were deconvolved into the
peaks of graphite, SiO2, and amorphous carbon. The XRD
spectra of the 002 carbon peaks of L-R coke and H-R coke after reactions
at 800, 900, 1000, and 1100 °C are shown in Figures and 8, respectively. It can be seen from Figure that the graphitization degree of L-R coke
decreases first and then increases, and it is the lowest at 1000 °C.
The width of the 002 carbon peak of L-R coke first widened and then
narrowed with the increase of temperature, which was the widest at
1000 °C, indicating that the order of the carbon structure of
L-R coke first decreased and then increased with the increase of temperature.
Figure 7
XRD patterns
of L-R coke under the influence of temperature.
Figure 8
XRD patterns of H-R coke under the influence of temperature.
XRD patterns
of L-R coke under the influence of temperature.XRD patterns of H-R coke under the influence of temperature.Figure shows that
when the temperature is 800 and 1000 °C, the 002 carbon peak
of H-R coke is wide and diffuse, indicating that the order of the
carbon structure is poor. In addition, the width of the 002 carbon
peak of L-R coke is narrower than that of H-R coke, indicating that
the carbon structure of L-R coke is more orderly than that of H-R
coke. The relative content of SiO2 in H-R coke is higher
than that in L-R coke.The carbon structure and pore characteristics
of metallurgical
coke have a significant impact on coke behavior and reactivity in
a blast furnace. The basic unit of the carbon structure is a graphite
crystallite, and the size of the graphite crystallite can usually
be characterized by the stacking height Lc of the
carbon substrate.[25,26] In this study, the stacking height Lc was calculated using Origin. First, the XRD data was
drawn, and then the “multipeak fitting” was carried
out. The Lorentz function was used to obtain the corresponding peak
position 2θ and FWHM, and then the stacking height Lc was calculated by the Scherrer equation.where λ is the wavelength of the X-ray
radiation, nm; B is the full width at half-maximum
of the 002 peak, deg; and θ is the Bragg angle of the 002 peak,
deg.Figure shows the
relationship between the stacking height Lc of two
cokes with different reactivities and temperatures. It is found from Figure that in the range
of 800–1100 °C, the Lc value of L-R coke
decreases first and then increases with the increase in temperature.
The Lc value of H-R coke is higher at 900 and 1100
°C but lower at 800 and 1000 °C. In addition, the Lc value of H-R coke is lower than that of L-R coke, which
indicates that the graphitization degree and carbon structure order
of L-R coke are higher than those of H-R coke. According to the change
of CRE of the two kinds of coke after coupling reaction, it was found
that when the reaction temperature was 800–1000 °C, the
graphitization degree of coke was positively correlated with its reaction
activity. When the reaction temperature was higher than 1000 °C,
the graphitization degree of coke was negatively correlated with its
reaction activity.
Figure 9
Relationship between the stacking height Lc of
coke and temperature.
Relationship between the stacking height Lc of
coke and temperature.
Effect of Temperature on the Pore Structure
of Coke
The pore structure of coke is characterized by the
pore wall area, pore wall thickness, and pore size. It is an important
reaction interface in the gasification process of coke in a BF and
determines the kinetic conditions of the coke gasification process.
When φ(H2) is 25% in a high hydrogen-rich atmosphere,
the effects of temperature on the pore structure of H-R coke and L-R
coke are shown in Figures and 11, respectively. For H-R coke,
when compared with the pore structure at 800 and 900 °C, the
number of pores at 1000 and 1100 °C is greater, and even a large
number of perforations are produced. At the same time, the size of
pores becomes larger, and the thickness of the pore wall decreases
significantly, thereby increasing the reaction interface of CO2 and H2O with coke gasification reaction, resulting
in more serious damage to the carbon matrix of coke. This indicates
that the higher the temperature, the more serious the dissolution
loss of coke, thus affecting the thermal strength of metallurgical
coke.
Figure 10
SEM photographs of H-R coke after coupling reaction.
Figure 11
SEM photographs of L-R coke after coupling reaction.
SEM photographs of H-R coke after coupling reaction.SEM photographs of L-R coke after coupling reaction.The changing trend of the pore structure of L-R
coke with temperature
is basically consistent with that of H-R coke. However, comparing
the microstructure of different cokes under the same experimental
conditions, it can be seen that the pore structure formed by high-reactivity
coke is larger, and the pore size of low-reactivity coke is smaller.
Notably, although the microstructure of blast furnace coke may control
its reactivity and strength to some extent, it is not the only criterion.
The multiphase reaction in a BF, alkali metal, and the composition
of coke itself also directly affect the dissolution loss behavior
of metallurgical coke.
Conclusions
The coupling behavior between
gasification of typical coke and
reduction of sintering ore in a CO–N2–H2 gas mixture with φ(H2) of 25% at different
temperatures was studied using a conventional coke reactivity measuring
device. The following conclusions were reached:According to the thermodynamic calculation
results, when the temperature is lower than 1100 K, with the increase
of φ(H2) in the initial reaction gas, the concentration
of reducing gas in the system increases when the reduction reaction
of iron oxide reaches equilibrium, and the gasification of coke is
inhibited. When the temperature is higher than 1100 K, the results
are the opposite.The
CRE of both cokes increased with
the increase in temperature, and CTS decreased with the increase in
temperature. The CTS of L-R coke after the reaction is higher than
that of H-R coke, and the RI of sintering
ore after the coupling reaction with L-R coke is higher than that
with H-R coke.At a
high temperature and high hydrogen-rich
atmosphere with φ(H2) of 25%, the CTS of H-R coke
is greater than 60.4%, which meets the strength requirements of a
blast furnace for metallurgical coke. It can be seen that the reactivity
(CRI) obtained under the national standard test conditions and the
strength (CSR) after reaction may mislead the evaluation of high-reactivity
coke.The graphitization
degree and carbon
structure order of L-R coke are higher than those of H-R coke. When
the reaction temperature is 800–1000 °C, the graphitization
degree of coke is positively correlated with its reactivity, and when
the reaction temperature is greater than 1000 °C, it is negatively
correlated.