2018 Volume 58 Issue 12 Pages 2253-2257
The behavior of tuyere coke obtained from a COREX-3000 process was investigated in the present study for an in-depth understanding for the condition of raceway. The coke samples was obtained in a dissection process of the furnace, and coke samples at P1 (200 mm from tuyere sleeve towards the furnace center), P2 (400 mm from tuyere sleeve towards the furnace center), P3 (600 mm from tuyere sleeve towards the furnace center), P4 (800 mm from tuyere sleeve to the furnace center), P5 (1000 mm from tuyere sleeve to the furnace center) and P6 (1200 mm from tuyere sleeve to the furnace center) were sieved, and the particles size distribution and average size of different position has been calculated. Microstructure of coke samples at P2, P4 and P6 was examined using scanning electron microscopy, and carbon structure and mineral phases of coke samples at P6 were identified using X-ray diffraction (XRD) analysis. The results showed that the percentage of small coke particles (<10 mm) was higher at P5 and P6, and the average particle size of coke samples at P5 and P6 were 12.04 mm and 7.71 mm, which is much smaller than that of other samples indicating a severe degradation of coke. The amount of pores of tuyere coke increased compared with charged coke, and more pores were found in coke sample at P6 than P2 and P4, indicating a violent reaction at this position. The graphitization degree of tuyere cokes at P6 were much higher than that of charged coke, and coke particle (10–16 mm) possess the highest graphitization degree, indicating the much higher temperature in the raceway zone. The main minerals in the tuyere coke were gehlenite and akermanite, and the slag was melt to be spherical particles confirming the higher temperature in raceway zone in COREX-3000 process.
The COREX process has obvious advantages in environment protection and CO2 reduction compared with conventional blast furnace process. It is independent on coking coal to meet the requirements of environment and source, and it has been successfully operated in India, South Africa and South Korea.1,2) Detailed information about the process and equipment of COREX can be found in the investigation by Wu et al.4,5)
However, the pig iron cost of COREX-3000 process is much higher than that of blast furnace because of raw materials including lump coal in China. Therefore, a series of COREX-3000 processes introduced by Baosteel in 2007 was entirely moved to XinJiang province to achieve operation with low cost, and the raw materials has changed compared with the primary process. A larger amount of coke are charged into the melter gasifier to obtain better permeability of the column. However, the coke charged into the COREX-3000 furnace is produced using low rank coke coal, which influences the properties of coke. The average Micum index6) M40 (cracking resistance index) and M10 (abrasive resistance index) of coke charged into the furnace were 86.3 and 6.8, respectively, however, the average CRI (coke reactivity index) and CSR (coke strength after reaction)7) were 51.34 and 35.40, respectively, which is absolutely different from that of coke charged into conventional blast furnace.
Coke is the most important material for the column permeability in COREX-3000 furnace as in blast furnace.8) Coke degradation occurs seriously in the furnace due to a series of complicated physical and chemical reaction and the poor CSR when it reaches tuyere zone. Tuyere drilling technique is usually used to extract samples from an operating blast furnace to provide useful information about inner phenomena in the tuyere level,9,10) and many studies9,10,11) have been done on the tuyere coke in blast furnace, however, the condition at tuyere level in COREX-3000 furnace is very different from that of blast furnace including the size of raceway and theoretical combustion temperature.12,13,14) Therefore, an in-depth understanding about coke reaction behavior in the high temperature zone of the COREX-3000 furnace is critical to optimize the process. Coke samples in the tuyere level in the present study were extracted when the COREX-3000 furnace is shun down.
In this paper, tuyere coke samples have been examined to characterize particle size distribution, microstructure and carbon structural order at different location from tuyere sleeve. The aim of this paper is to develop an understanding of the behavior and characteristic of the tuyere coke in the COREX-3000 furnace.
Tuyere coke samples are usually extracted from an operating blast furnace using tuyere drilling technique. In the present study, the tuyere coke samples were extracted from a COREX-3000 furnace when it was shut down for overhauling. The vertical position of the sample location was at the center line of tuyere, and the horizontal position of sample location was 200 mm (P1), 400 mm (P2), 600 mm (P3), 800 mm (P4), 1000 mm (P5) and 1200 mm (P6) from tuyere sleeve towards the furnace center as shown in Fig. 1. The coke samples were sieved using standard sieve with size of <1.6 mm (S1), 1.6–2.5 mm (S2), 2.5–10 mm (S3), 10–16 mm (S4), 16–20 mm (S5), 20–25 mm (S6), 25–40 mm (S7), >40 mm (S8) in turn.

The schematic of the tuyere coke sampling positions.
Then the mass of different coke samples was weighed, and the corresponding proportion was calculated, respectively. The average particle size was calculated according to Eq. (1)
| (1) |
Where D is average size of coke samples at some position, mm; Di is average size of sieve size range i, mm; Yi is mass percentage of coke samples with sieve size range i.
2.2. Microstructure AnalysisCoke samples at P2, P4 and P6 were selected, and pieces about 10 mm×10 mm×5 mm were cut from the selected samples. The coke pieces were mounted in the rounded plastic container with 15 mm diameter filled with the epoxy resin. The specimens were ground and polished, and then they were examined with a Quanta 250 Environmental scanning electron microscope (SEM) equipped with energy dispersive X-ray spectrometer (EDS) for microstructure analysis. Coke samples at P6 were crushed to select particles(less than 74 μm) for XRD examination. The analysis was conducted using a XRD diffractometer (Rigaku Corporation) with Cu Ka radiation. The scanning angles scope was 10 to 90 deg (2θ) at a rate of 10 deg/min.
Particle size distribution of tuyere coke at different position was shown in Fig. 2. The percentage of S8 (>40 mm) decreased sharply from P2 to P5, and there was no particle larger than 40 mm at P6. The percentage S7 (25–40 mm) increased from P2 to P4 and then decreased from P4 to P6. The percentage of S5 (16–20 mm) and S6 (20–25 mm) showed unclear size change tendency, and the percentage of S1 (<1.6 mm), S2 (1.6–2.5 mm) and S3 (2.5–10 mm) increased accordingly, especially for the percentage of S2 and S3. The percentage of small particles increased sharply from P5 to P6, indicating a serious degradation occurs at these positions.

Particle size distribution of tuyere coke at different position.
The average particle size of tuyere coke ranged from P1 to P6 were shown in Fig. 3. It shows that the average particle size of tuyere coke at P1, P2, P3 and P4 were 18.8 mm, 19.2 mm, 18.45 mm and 18.92 mm, respectively, however, the average particle size at P5 and P6 were 12.04 mm and 7.71 mm. The particle size distribution showed that the average particle size at P1, P2, P3 and P4 was almost the same, but it was much smaller at P5 and P6. It showed that more fines was product at P5 and P6 (1000 mm and 1200 mm from tuyere sleeve towards the furnace center), indicating serious degradation occurred at P5 and P6, and it was the beginning of the deadman zone.

The average particle size of tuyere coke at different positions.
The particle size distribution of the charged coke was shown in Fig. 4, and the percentage of particles with size of 40–60 mm is the largest, which was as high as 46.52%. That of particles larger than 40 mm is almost 76.75%, while there was no coke particles larger than 40 mm existing in tuyere coke samples. The average size of charged coke was 53.70 mm, which is much larger than that of tuyere coke at any position in the present study, indicating a severe degradation process of coke in the furnace.

Particle size distribution of charged coke.
Microstructure of charged coke and tuyere coke at P2, P4 and P6 was shown in Fig. 5. An amount of small open pores were observed in the charged coke, which was beneficial to diffusion of CO2. However, more pores were observed in tuyere coke samples at P2, P4 and P6 compared with the charged coke, and the size of the pores were enlarged. The pore wall of tuyere coke samples was thinner than that of charged coke due to gasification with CO2. A large amount of pores interconnected with each other were found in tuyere coke at P6 as shown in Fig. 4(d), indicating severe gasification reaction with CO2. Thinner pore wall resulted in poorer strength after reaction, and coke fine produced as well.

Microstructure of tuyere coke at P2, P4 and P6. (a) charged coke; (b) tuyere coke at P2; (c) tuyere coke at P4; (d) tuyere coke at P6.
Temperature has been proved to have a great effect on the degree of graphitization of tuyere coke, and coke fines (<74 μm) comes from the surface of lump coke due to high temperature. The temperature in tuyere zone of COREX-3000 furnace is much higher than that of blast furnace due to high oxygen enrichment rate, and the highest temperature in the raceway of COREX-3000 furnace is about 3500 K.13) Therefore, in-depth understanding of the effect of higher temperature on tuyere coke in this process needs to be investigated.
The XRD analysis of tuyere coke particles as well as charged coke confirmed the high degree of graphitization of tuyere coke as shown in Fig. 6. The sharp graphite (002) peak was observed in tuyere coke samples S1, S2, S3, S4 and S5, while the (002) peak of charged coke is much wider. Sharp (002) peak was not observed in tuyere coke samples S6 and S7, however, sharp (100) peak and quartz was observed in these cokes indicating larger crystal size and lower temperature compared with other tuyere coke.15)

XRD spectrum of tuyere coke samples with different size at P6.
As shown in Fig. 7, further magnification of graphite (002) peak area distinguished the different graphitization degree of tuyere coke samples with different size at P6. As the particle size of tuyere coke samples increased, the angles of graphite (002) peak increases except S2 and S4, indicating d002 decreased accordingly.

Magnification of graphite (002) peak.
The d002 value as well as Lc and La estimated with Scherrer equation of tuyere coke S1 to S7 and charged coke were shown in Table 1.10) The d002 value of tuyere coke samples and charged coke were calculated to be 3.40, 3.43, 3.47, 3.38, 3.44, 3.47, 3.46 and 3.52 nm, respectively, from the Bragg’s law. While the Lc values of tuyere coke samples and charged coke were estimated to be 1.79, 1.77, 1.40, 2.35, 1.71, 1.51, 1.38 and 0.16 nm, respectively, indicating that higher graphitization degree of tuyere coke than that of charged coke. The highest degree of graphitization of tuyere coke belongs to S4 (10–16 mm) showing that the highest temperature it underwent.
| Sample | d002/nm | Lc/nm | La/nm |
|---|---|---|---|
| Charged coke | 3.52 | 0.16 | 0.53 |
| S1 | 3.40 | 1.79 | 2.47 |
| S2 | 3.43 | 1.77 | 3.06 |
| S3 | 3.47 | 1.40 | 3.02 |
| S4 | 3.38 | 2.35 | 3.99 |
| S5 | 3.44 | 1.71 | 3.87 |
| S6 | 3.47 | 1.51 | 9.20 |
| S7 | 3.46 | 1.38 | 13.69 |
| Tuyere coke from blast furnace | 3.42 | 0.25 | 4.41 |
The Lc value of charged coke was only 0.16 nm indicating low graphitization degree resulting in high CRI and more pores were produced after gafication reaction. While the Lc values of all tuyere coke were higher due to the effect of high temperature in raceway zone, which is usually associate with hot metal and high theoretical combustion temperature due to high oxygen enrichment. The d002, Lc and La value of tuyere coke from a 2500 m3 blast furnace using the same charged coke was also calculated and listed in Table 1. It showed that, the Lc value of tuyere coke from the blast furnace is only 0.25 nm, which is much smaller than that of tuyere coke from COREX-3000 furnace indicating higher temperature in the tuyere zone of COREX-3000 furnace.
Li et al found that15) the graphitization degree of coke fines (<74 μm) in blast furnace hearth is higher than that of lump tuyere coke indicating that coke graphitization in the high temperature zone starts from the coke surface and leads to the formation of coke fines. Gupta9) et al. found the similar conclusion as well. However, the graphitization degree of tuyere coke S4 (10–16 mm) in the present study is the highest among all the tuyere coke samples, and the coke fines S1 (<1.6 mm) is smaller than that of S4 (10–16 mm) indicating that the coke fines was not formed by surface graphitization of lump coke in the present study. The degree of graphitization of small coke particles S1, S2 and S3 is almost equal to that of lump coke S5, S6 and S7, indicating that the small coke particles comes from degradation of lump coke due to the poor CSR of charged coke and severe condition in the raceway.
The microstructure of slag in tuyere coke S4 (10–16 mm) was shown in Fig. 8 to investigate slag behavior in the tuyere coke. Spherical particles were observed in the pores of tuyere coke S4 (10–16 mm) in Fig. 8(a), and molten agglomeration was found in the pore wall (Figs.7(b) and 7(c)). Macro pores and small pores interconnect with each other, and the pore wall has been destroyed.

Microstructure of ash of tuyere coke S4 (10–16 mm) at position P2.
The result of mapping analysis was shown in Fig. 9, and elements of Al, Si and Ca were found in the spherical ash particles from tuyere coke S4 (10–16 mm) at P2, which is in accordance with the XRD analysis. The minerals in tuyere coke were determined to be akermanite (Ca2MgSiO7) and gehlenite (Ca2Al2SiO7) in XRD analysis, which are the common minerals in the continuously cooled crystalline blast furnace slag.16)

Mapping analysis of the spherical ash particles.
Akermanite and gehlenite are belong to melilite, which is a solid solution. The melting temperature of melilite is higher than 1673 K, and the melting point of gehlenite is approximately 1873 K. Final slag has been found in the pores of tuyere coke and hearth coke,15) and it fills up the interconnected pores. However, spherical slag particle melted by high temperature has never been found in tuyere coke in blast furnace due to lower temperature in the raceway zone of the process, therefore, the temperature in raceway of COREX-3000 process must be much higher than that of blast furnace in accordance with the XRD analysis and Du’s calculating results.13)
Tuyere coke samples from a COREX-3000 process were examined to characterize the coke behavior, and following conclusions were made:
(1) The percentage of small coke particles (<10 mm) increased at P5 and P6, and the percentage of lump coke (>10 mm) changes little from P1 to P4. The average particle size of coke samples at P1, P2, P3 and P4 were 18.80 mm, 19.20 mm, 18.45 mm and 18.92 mm, respectively, and the average particle size at P5 and P6 were 12.04 mm and 7.71 mm, which is much smaller than that of the charged coke. The sharp decrement of coke particle size indicates a severe degradation of coke in the furnace.
(2) More pores were found in tuyere coke compared with charged coke due to gasification reaction with CO2, and more pores were determined in coke sample at P6 than P2 and P4, indicating a violent reaction at this position in accordance with the result of particles size distribution.
(3) The degree of graphitization of tuyere cokes were much higher than that of the charged coke due to the effect of high temperature. Tuyere coke with different particle size showed different graphitization degree. Coke particle (10–16 mm) possess the highest graphitization degree, and smaller coke fines (<10 mm) showed lower graphitization degree as well as lump coke (>16 mm), indicating that the coke fines come from degradation of lump coke due to poor strength after reaction.
(4) The higher graphitization degree of tuyere coke indicated high temperature in the raceway zone of COREX-3000 process. The main minerals in the tuyere coke were gehlenite and akermanite, and the slag was melt to be spherical particles confirming the higher temperature in raceway, which is in accordance with the XRD analysis.
The present work was supported of the National Science Foundation of China (51774032) & Yong Elite Scientists Sponsorship Program By CAST (2017QNRC001).