Home Physical Sciences Kinetic Study on Phosphate Enrichment Behavior in CaO–SiO2–FeO–Fe2O3–P2O5 Steelmaking Slags
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Kinetic Study on Phosphate Enrichment Behavior in CaO–SiO2–FeO–Fe2O3–P2O5 Steelmaking Slags

  • Jin-yan Li EMAIL logo , Mei Zhang , Min Guo EMAIL logo and Xue-min Yang
Published/Copyright: June 1, 2017

Abstract

The iso-thermal crystallization behavior of phosphate-enriched phase has been experimentally investigated in the rapidly quenched CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags under different cooling schedules. The experimental results indicate that increasing endpoint temperature from 1453 to 1533 K and prolonging holding time from 2 to 60 min can result in an increasing tendency of the size of phosphate-enriched phase in the shape of one-dimensional rod. The crystallization kinetics of phosphate-enriched phase in steelmaking slags has been described by Avrami equation. The Avrami constant n was obtained to be 0.472, while the crystallization rate constant k was recommended as lnk=57.40+12,273.96/T8.25lnT5.5×103T. Thus, the apparent activation energy E of crystallization is recommended as E=537.60206.015T kJ/mol.

Introduction

Steelmaking slags essentially containing more or less content of phosphate cannot be effectively utilized in the traditional metallurgical refining routes. As one of prospective techniques, the crystallization and selective enrichment of phosphate from steelmaking slags has been attached more attention in recent decade. From the viewpoint of thermodynamics, the phosphate enrichment process can be described in sequence as follows: (1) component P2O5 can be easily bonded by CaO to form tricalcium phosphate 3CaO·P2O5 (C3P) [1, 23], and the formed complex component C3P can react with the produced dicalcium silicate 2CaO·SiO2 (C2S) to generate phosphate-enriched phase of solid solution n2CaO·SiO2–3CaO·P2O5 (nC2S–C3P) [4] under the fixed cooling conditions; (2) acidic or amphoteric oxides or components containing aluminum [5, 67], titanium [8,9], and fluorine [10] can indirectly affect phosphate enrichment behavior by combining with C2S in steelmaking slags, i. e., the generated free C2S content affects content of P2O5 of phosphate-enriched phase nC2S–C3P in steelmaking slags; (3) the maximum content of P2O5 in nC2S–C3P solid solution can reach to about 30.0 % [11]. On the other hand, the phosphate crystallization kinetics had also been investigated from the viewpoint of the influence of components in slags and crystallization temperature or endpoint temperature on viscosity [6, 9, 12], structure [6, 9, 12], and phosphorus distribution ratio [13, 14].

It is well known that the crystallization rate constant k related with apparent activation energy E of phosphate crystallization process is closely decided by cooling schedule including cooling rate, endpoint temperature, holding time and so on. The effect of cooling schedule on crystallization rate constant k of phosphate crystallization process in simple slags was studied through thermal analysis by single hot thermocouple technique (SHTT) [8, 15]. However, the crystallization kinetics of phosphate-enriched phase in complex steelmaking slags was usually studied by scanning electron microscopy (SEM) for detecting the mineralogical phases in quenched slag samples.

In this study, the mineralogical phases in the rapidly quenched slag samples of CaO–SiO2–FeO–Fe2O3–P2O5 slag systems [11] have been detected by the SEM observation. Meanwhile, the average crystal area fraction of phosphate-enriched phase in the SEM images has been counted through the image manipulation software Image-Pro-Plus (IPP). The influence of endpoint temperatures and holding time on the average crystal area fraction of phosphate-enriched phase has been described by Avrami equation coupled with the optimized expression of crystallization rate constant k through evaluating seven formulas of k from the literature. The kinetic behavior of phosphate-enriched phase in the steelmaking slags has been quantitatively described and predicted, meanwhile the optimal parameters of cooling schedule including endpoint temperatures, holding time, and cooling rate for obtaining larger size phosphate-enriched phase have been recommended.

Experimental

Experimental procedures

The CaO–SiO2–FeO–Fe2O3–P2O5 slag system was applied to model the complex steelmaking slags through melting the prepared powders of ferrous oxide FeO and reagent-grade powders of CaO, SiO2, Fe2O3, and P2O5, which reported in details by the present authors elsewhere [11]. The slag samples were synthesized in chemical composition of (% CaO)=34.18, (% SiO2)=26.29, (% FeO)=15.54, (% Fe2O3)=26.29, and (% P2O5)=5.00. The designed heating and cooling operations were conducted in a vertical tube-type heating furnace in ±3 K fluctuation with MoSi2 rods as heating elements. The high purity argon gas in 99.999 vol. % was used as carrier gas at a flow rate of 0.4 NL/min for avoiding re-oxidization of the prepared powders of ferrous oxide FeO during heating and cooling stages in all test-run experiments. In order to completely melt down the slag samples, 1773 K was applied to be the maximal heating temperature through heating the slag samples from ambient temperature at a rate of 3.0–5.0 K/min in Ar atmosphere.

From the standpoint of cooling schedule, two-group experiments were conducted in this study as listed in Table 1. In the first group of experiments, five test-run experiments corresponding to No. 1 to No. 5 in Table 1 were conduced to investigate the influence of endpoint temperature and holding time on kinetics of phosphate enrichment in the quenched slag samples at a fixed cooling rate of 5 K/min. Five endpoint temperatures at 1453, 1473, 1493, 1513, and 1533 K and four holding times in 2, 10, 30, and 60 min were applied as shown in Figure 1. In the second group of experiments, three test-run experiments corresponding to No. 6 to No. 8 in Table 1 were carried out at the endpoint temperature of 1453 K with holding time in 60 min at three cooling rates of 1, 3, and 5 K/min.

Figure 1: Applied heating schedule from ambient temperature to 1773 K and cooling schedule for slag samples of No. 1 to No. 5 test-run experiments.
Figure 1:

Applied heating schedule from ambient temperature to 1773 K and cooling schedule for slag samples of No. 1 to No. 5 test-run experiments.

Table 1:

Determined crystallization area fraction of phosphate-enriched phase of eight test-run experiments and average grain diameters of No. 6–No. 8 test-run experiments under various cooling conditions.

Test No.Endpoint temperature (K)Crystallization area fraction of phosphate-enriched phase at various holding times (%)Cooling rate (K/min)Average grain diameter (μm)
t=2 mint=10 mint=30 mint=60 min
1145314.5522.1224.1925.575
2147313.0719.5023.7225.415
3149311.7417.5222.2924.835
415138.7513.5320.0224.795
515336.2010.2717.2524.945
6145326.17164.7
7145324.73343.2
8145325.57537.8

Two methods were adopted to take the slag samples in terms of holding time. The slag samples in Pt crucible in holding time less than 30 min were taken by quickly dipping a steel rod, while the slag samples in holding time longer than 30 min were taken by rapidly removing the Pt crucible from the furnace. The slag samples taken by dipping a steel rod or by removing Pt crucible were quenched by water. The water quenched slag samples were dried in an oven at 403 K for at least 4 hours.

In order to observe the micromorphology of quenched slag samples, the dried slag samples were mounted in epoxy resin, ground with SiC sandpapers, polished, and coated with carbon for the SEM (MLA250) observation. The phosphate enrichment area in crystalline phase was counted by the image manipulation software IPP. Thus, the crystalline area fraction of phosphate-enriched phase was experimentally determined for kinetic study.

Determination of endpoint temperature range

The possibly formed components in the steelmaking slags were calculated by FactSage 6.3 software over a temperature range from 1300 to 2000 K as shown in Figure 2. It can be observed in Figure 2 that the melting point of the slags is about 1560 K. The possibly formed components in the slags change in six temperature ranges: (1) In the case of T>1591 K, the main components of the molten slags exist as simple oxides CaO, SiO2, FeO, and Fe2O3, whereas P2O5 exist as solid solution C3P. (2) In the case of T<1591 K, iron oxides of both FeO and Fe2O3 tend to decrease and form Fe3O4. (3) In the case of T<1560 K, simple oxides of CaO, SiO2, FeO, and Fe2O3 show a decreasing tendency and solid solution CaO·SiO2 (CS) will be precipitated, while solid solution 3CaO·2SiO2 (C3S2) will be also precipitated at T<1540 K. (4) The simple oxides CaO, SiO2, FeO, Fe2O3 will disappear at melting point as T=1560 K. (5) In the case of T<1469 K, the precipitations of Fe3O4, CS and C3S2 reach to their peaks, and solid solution CaFeSiO4 is formed. (6) In the case of T<1439 K, the solid solution C3S2 phase will decrease and CS phase can disappear.

Figure 2: Variation of possibly formed components in CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags over a temperature from 1300 to 2000 K by FactSage software.
Figure 2:

Variation of possibly formed components in CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags over a temperature from 1300 to 2000 K by FactSage software.

Thus, the lowest crystallization temperature or endpoint temperature for the steelmaking slags was recommended over a temperature range from 1439 to 1540 K for the purpose of precipitating enough amount of C2S phase.

Kinetic considerations of crystallization

It has been widely accepted that the iso-thermal crystallization kinetics of crystals can be quantitatively described by Avrami equation [16, 17, 1819] as

(1)x=1exp(ktn)

where x is the average mass fraction of formed crystals (–), k is the crystallization rate constant related with temperature (s–1), t is the crystallization time (s), n is Avrami constant coupled with crystallization mechanism. Avrami equation [16, 17, 1819] in eq. (1) can be rewritten through double-logarithmic transformation as

(2)ln[ln(1x)]=nlnt+lnk

Evidently, Avrami constant n can be obtained from slope of the linear relationship between ln[ln(1x)] and lnt, while the crystallization rate constant lnk corresponds to the intercept. The relationship between Avrami constant n in eq. (1) and eq. (2) and crystallization mechanism can be correlated by [20, 21]

(3)n=a+bc

where a means the crystal nucleation parameter (–), b stands for the crystal growth dimension parameter (–), and c is the crystal growth parameter (–). Three cases were defined [20, 21] to set the value of a as: (1) a=0 was applied for the case with the crystallization rate as zero; (2) 0<a<1 was used for the case with the crystallization rate decreasing over prolonging crystallization time; and (3) a>1 was applied for the case with the crystallization rate increasing over prolonging crystallization time. Similarly, three cases were also defined [20, 21] to set the value of b as b=1,2,3 for the cases with one-dimension, two-dimension and three-dimension growth of crystalline phase, respectively. Meanwhile, there were two cases for setting the value of c as [20, 21]: (1) c=1 was for the case of crystallization process controlled by the interface reaction; and (2) c=0.5 was for the case of crystallization process controlled by phase diffusion.

The involved crystallization rate constant k in eq. (1) or eq. (2) of Avrami equation can be described by the famous Arrhenius formula as [22]

(4)k=Aexp(E/ERTRT)(s1)

where A is the pre-exponential factor (–), E is the apparent activation energy of crystallization (J/mol), R is the gas constant (8.314 J/(mol·K)), and T is the endpoint temperature in this study (K). Obviously, Arrhenius formula in eq. (4) can be rewritten through logarithmic transformation as

(5)lnk=lnAE/ERTRT(s1)

According to the linear relationship between lnk and 1/T, the apparent activation energy E of crystallization can be obtained from the slope.

Beside the famous Arrhenius formula in eq. (4) or eq. (5), some formulas claimed as non-Arrhenius formulas were also proposed as listed in the second column of Table 2. Clearly, six collected formulas of non-Arrhenius formulas are named as M2–M7, while Arrhenius formula in eq. (4) or eq. (5) is labeled as M1.

Table 2:

Summary of seven collected formulas of crystallization rate constant k from the literature.

Formula No.Formula of k (s–1)Expression of lnk (s–1)dlnk/dT (s–1⋅K–1)Expression of E (J/mol)Author(s)Ref.
M1k=Aexp(E/RT)lnk=lnAE/RT1/RT2EArrhennius[22]
M2k=ATj2lnk=lnA+j2lnTj2/TRj2THarecourt and Esson[23]
M3k=Aexp(j3T)lnk=lnA+j3Tj3Rj3T2Berthelot and Hood[25, 26]
M4k=ATj2exp(j1/T)lnk=lnAj1/T+j2lnTj1/T2+j2/TRj1+j2TKooij[28]
M5k=Aexp(j3T)exp(j1/T)lnk=lnAj1/T+j3Tj1/T2+j3Rj1+j3T2van’t Hoff[29]
M6k=ATj2exp(j3T)lnk=lnA+j2lnT+j3Tj2/T+j3Rj2T+j3T2Flynn[30]
M7k=ATj2exp(j3T)exp(j1/T)lnk=lnAj1/T+j2lnT+j3Tj1/T2+j2/T+j3Rj1+j2T+j3T2van’t Hoff[29]

The formula M2 by Harcourt–Esson [23] was applied by Dollimore et al. [24] to interpret the decomposition kinetics of calcium carbonate (CaCO3). The formula M3 by Berthelot–Hood [25, 26] was used by Simon [27]. Beside formula M4 by Kooij [28] as well as formulas M5 and M7 by van’t Hoff [29] originally developed in the nineteenth century, formula M6 was proposed by Flynn [30] in 1997. It is interesting to find that all seven collected formulas from M1 to M7 can be expressed in a general form as lnk=lnAj1/T+j2lnT+j3T.

The apparent activation energy E of crystallization for seven formulas in Table 2 can be derived as

(6)E=Rdlnkd(1/1TT)=RT2dlnkdT(J/mol)

Thus, seven formulas in the second column of Table 2 can be also expressed in natural logarithmic forms as listed in the third column. The derived formulas of the apparent activation energy E of crystallization from eq. (6) are summarized in the fifth column of Table 2 combining with the formulas of dlnk/dT in the fourth column.

Results and discussion

Determination of crystallization area fraction

The SEM images for slag samples of No. 1, No. 3, and No. 5 test-run experiments at three endpoint temperatures in four holding times are displayed in Figure 3. Taking slag sample of No. 1 test-run experiment as an example, the SEM images of No. 1 slag samples in four holding times of 2, 10, 30, and 60 min are shown in Figures 3(a1)–3(a4). The similar labels are also used to No. 3 and No. 5 slag samples in Figures 3(b1)–3(b4) and 3(c1)–3(c4), respectively. Three zones in white, gray, and dark color can be observed in Figure 3, whereas the white zone is iron oxides-enriched phase, the gray zone is matrix phase and the dark zone is phosphate-enriched phase, which is the same as those reported in the previous study [5].

Figure 3: SEM images of No. 1, No. 3 and No. 5 test-run slag samples at three endpoint temperatures of 1453 K (a), 1493 K (b), and 1533 K (c) with four holding times in 2, 10, 30, 60 min, respectively.
Figure 3:

SEM images of No. 1, No. 3 and No. 5 test-run slag samples at three endpoint temperatures of 1453 K (a), 1493 K (b), and 1533 K (c) with four holding times in 2, 10, 30, 60 min, respectively.

It can be confirmed from Figure 3 that increasing the endpoint temperature and prolonging the holding time can result in an increasing tendency of the size of phosphate-enriched phase in dark zones. In comparison with the SEM images in Figures 3(a1)–3(a4), it can be deduced that increasing the holding time at the fixed endpoint temperature of 1453 K can promote the size of phosphate-enriched phase in dark zones. Thus, prolonging the holding time is an effective measure to expand the size of phosphate-enriched phase.

In comparison with the SEM images in Figures 3(a1), 3(b1), and 3(c1), it can be deduced that increasing the endpoint temperature from 1453 to 1513 K can promote the formation of phosphate-enriched phase in dark zones in the same holding time of 2 min. It is due to that improving the endpoint temperature can decrease the instantaneous nucleation numbers, thus increase the size of phosphate-enriched phase in dark zones. It is further verified through comparing with Figures 3(a4), 3(b4), and 3(c4) that the phosphate-enriched phase in dark zones can be increased with improving the endpoint temperature in the fixed holding time of 60 min because of enhancing diffusion of phosphate-enriched phase.

The measured results of crystallization area fraction of phosphate-enriched phase in dark zones for all 20 quenched slag samples from the SEM images by software IPP are summarized in Table 1. The crystallization mass fraction x is proportional to the measured area ratio of phosphate-enriched phase in dark zones to the total slag samples. Thus, it can be replaced by the measured area ratio of formed phosphate-enriched phase in the SEM images as suggested by Ito et al. [31]

The influence of holding time on the average crystallization area fraction as well as the normalized area fraction of phosphate-enriched phase at five endpoint temperatures is illustrated in Figures 4(a) and 4(b), respectively. It can be observed in Figure 4 that prolonging the holding time can result in an increasing tendency of the average crystal area fraction as well as the normalized area fraction of phosphate-enriched phase. The average crystal area fraction of phosphate-enriched phase can reach to the maximum value as 25.57 % at five endpoint temperatures through prolonging the holding time to 60 min.

Figure 4: Influence of holding time on crystallization area fraction (a) and normalized area fraction (b) of phosphate-enriched phase in CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags over a temperature range from 1453 to 1533 K, respectively.
Figure 4:

Influence of holding time on crystallization area fraction (a) and normalized area fraction (b) of phosphate-enriched phase in CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags over a temperature range from 1453 to 1533 K, respectively.

Kinetic description of phosphate-enriched phase in steelmaking slags

In order to describe the iso-thermal crystallization kinetics of phosphate-enriched phase by Avrami equation in eq. (1) or eq. (2), the involved parameters such as Avrami constant n and crystallization rate constant k should be in first determined.

Determination of Avrami constant n

The relationship between lnt and ln[ln(1x)] at five endpoint temperatures is shown in Figure 5, respectively. The obtained Avrami constant n and crystallization rate constant lnk from the regressed slopes and intercepts of linear plots in Figure 5 are tabulated in Table 3. It should be emphasized that the unit of holding time in Figure 5 must be in second, rather than in minute. Otherwise, wrong results of slopes and intercepts will be produced. The obtained Avrami constant n changes from 0.442 to 0.506 with an average in 0.472.

Figure 5: Relationship between holding time in natural logarithmic form lnt$$\ln t$$ and ln[−ln(1−x)]$${\rm{ln[}} - {\rm{ln(1}} - x{\rm{)]}}$$ for phosphate-enriched phase in CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags at temperatures of 1453, 1473, 1493, 1513 and 1533 K, respectively.
Figure 5:

Relationship between holding time in natural logarithmic form lnt and ln[ln(1x)] for phosphate-enriched phase in CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags at temperatures of 1453, 1473, 1493, 1513 and 1533 K, respectively.

Table 3:

Obtained results of Avrami constant n and crystallization rate constant lnk of phosphate-enriched phase in steelmaking slags at five endpoint temperatures.

Test No.Endpoint temperature (K)Avrami constant n (–)lnk (s–1)
114530.465–2.365
214730.477–2.637
314930.442–2.624
415130.469–3.166
515330.506–3.761

It was reported [32, 33] that the phosphate-enriched phase crystallization was controlled by phase diffusion. Thus, the crystallization growth parameter c should be set as c=0.5. Furthermore, the observed phosphate-enriched phase is in the shape of one-dimensional rod as shown in Figure 3, the crystallization growth dimension parameter b is set as b=1. According to the relationship of n=a+bc in eq. (3), the crystallization nucleation parameter a should be set as a<1 under conditions of b=1, c=0.5, and n=0.472. This result conforms to the definition of crystallization nucleation parameter 0<a<1 introduced in section “Kinetic considerations of crystallization” as that the crystallizing rate of phosphate-enriched phase decreases with an increase of holding time.

Optimization of formula of crystallization rate constant k and determination of apparent activation energy E

Seven formulas of crystallization rate constant k as listed in Table 2 were used to determine the apparent activation energy E of crystallization. Based on the results of E with less errors, the optimal formula of crystallization rate constant k is recommended.

The relationship between lnk and 1/T by formula M1 in Table 2 is illustrated in Figure 6(a). The apparent activation energy E of crystallization for phosphate-enriched phase can be determined as E=−306.137 kJ/mol from the slope, i. e., E/R, as 36.821 in Figure 6(a). Meanwhile, the relationship of lnk against T by formula M2 or against lnT by formula M3 is displayed in Figures 6(b) and 6(c), respectively. Obviously, the slopes of the regressed linear plots give adjustable parameters j2 and j3. Thus, the apparent activation energy E by formulas M2 and M3 can be calculated by the formulas in the fifth column in Table 2. The calculated results of E by formulas M2 and M3 at five endpoint temperatures are listed in Table 4.

Figure 6: Relationship of crystallization rate constant in natural logarithmic form lnk$$\ln k$$ by three formulas of k$$k$$ against 1/T$$1/T$$ (a) or lnT$$\ln T$$ (b) or endpoint temperature T (c) over a temperature range from 1453 to 1533 K, respectively.
Figure 6:

Relationship of crystallization rate constant in natural logarithmic form lnk by three formulas of k against 1/T (a) or lnT (b) or endpoint temperature T (c) over a temperature range from 1453 to 1533 K, respectively.

Table 4:

Regressed results of pre-exponential factor lnA, adjustable parameters j1, j2, and j3, apparent activation energy E of crystallization, and mean deviation δE based on seven collected formulas of k.

Formula No.Regressed results of parameters in expression of k in form of lnk=lnAj1/T+j2lnT+j3TApparent activation energy E at five endpoint temperatures(J/mol)Mean deviation δE (×10−2, –)
Pre-exponential factor In A (–)Adjustable parameters
j1 (–)j2 (–)j3 (–)T=1453 KT= 1473 KT=1493 KT=1513 KT=1533 K
M1–27.58–36,821.87–306,137–306,137–306,137–306,137–306,137–1.66
M2177.88–24.74–298,834–302,947–307,060–311,174–315,287–0.01
M321.89–0.017–291,548–299,629–307,821–316,124–324,536–1.66
M475.150–18,410.94–12.37–302,485–304,542–306,598–308,655–310,712–0.83
M5–2.84–18,410.94–0.0083–298,842–302,883–306,979–311,130–315,336–0.01
M699.89–12.37–0.0083–295,191–301,288–307,441–313,649–319,912–0.83
M757.40–12,273.96–8.25–0.0055–298,839–302,904–307,006–311,145–315,3200.00
Average*NDNDNDND–298,840–302,905–307,007–311,145–315,320ND
  1. *Note: ND means no data.

To formulas M4−M7, the pre-exponential factor lnA and adjustable parameters j1 of 1/T, j2 of lnT, and j3 of T can be also obtained through the multiple linear regression method based on the results of lnk at various endpoint temperatures T in different holding times. Thus, the apparent activation energy E of crystallization by four formulas of M4 to M7 can be determined by the expressions of E in the fifth column of Table 2 as listed in Table 4.

The effect of endpoint temperatures from 1453 to 1533 K on the obtained apparent activation energy E of crystallization by seven formulas of k in Table 4 is shown in Figure 7(a), respectively. Large discrepancies of the obtained apparent activation energy E of crystallization can be observed in Figure 7(a) by seven formulas of k. In order to find the best formula among seven formulas of k, the mean deviation of apparent activation energy δE is calculated based on the mean activation energy EAvg. as a basis through

(5)δE=1mEEAvg.EAvg.×100
Figure 7: Comparison of calculated apparent activation energy E$$E$$ (a) and mean deviation δE$${\delta _E}$$ (b) by seven collected formulas of k$$k$$ over a temperature range from 1453 to 1533 K, respectively.
Figure 7:

Comparison of calculated apparent activation energy E (a) and mean deviation δE (b) by seven collected formulas of k over a temperature range from 1453 to 1533 K, respectively.

where m is the number of slag samples as 5 (–). The means deviation of apparent activation energy δE by seven formulas is illustrated in Figure 7(b). It can be observed in Figures 7(a) and 7(b) that three formulas M2, M5 and M7 of k can produce smaller mean deviation δE comparing with the largest ones by formula M1. Thus, the crystallization rate constant lnk can be described as lnk=57.40+12,273.96/T8.25lnT5.5×103T in the form of formula M7 of k. Meanwhile, the determined apparent activation energy E of crystallization can be expressed by E=537.60206.015T kJ/mol based on formula M7 of k.

Effect of cooling rate on grain size of phosphate-enriched phase

The SEM images of the slag samples in the second group of experiments, i. e., No. 6–No. 8 test-run experiments, is displayed in Figure 8, respectively. The measured average crystal area fraction and grain size of phosphate-enriched phase in the slag samples of No. 6–No. 8 test-run experiments are also summarized in Table 1. It can be obtained from Table 1 that increasing cooling rate from 1 to 5 K/min can result in a decreasing tendency of the grain size of phosphate–enriched phase. Lower cooling rate can promote the formation of phosphate-enriched phase in larger size. Larger than 40 μm as a criterion size [32, 33] is beneficial to separating the formed phosphate-enriched phase in steelmaking slags. Thus, the cooling rate smaller than 3 K/min is recommended for easily separation phosphate-enriched phase from the quenched slag samples in terms of viewpoint of the crystallization and selective enrichment of phosphate.

Figure 8: SEM images of No. 6 to No. 8 test-run slag samples under the condition of keeping endpoint temperature at 1453 K with holding time in 60 min at three cooling rates of 1, 3, and 5 K/min, respectively.
Figure 8:

SEM images of No. 6 to No. 8 test-run slag samples under the condition of keeping endpoint temperature at 1453 K with holding time in 60 min at three cooling rates of 1, 3, and 5 K/min, respectively.

Conclusions

The iso-thermal crystallization behavior of phosphate-enriched phase has been experimentally investigated in the rapidly quenched CaO–SiO2–FeO–Fe2O3–P2O5 steelmaking slags under different cooling schedules. The crystallization kinetics has been described by Avrami equation including Avrami constant n and crystallization rate constant k. Furthermore, the apparent activation energy E of crystallization has also been determined based on evaluation of seven collected formulas of crystallization rate constant k. The main summary remarks can be summarized as follows:

  1. The obtained Avrami constant n from experimental results is 0.472 during crystallization of phosphate-enriched phase in steelmaking slags. The involved two parameters in Avrami constant n as the crystallization growth parameter c and the crystallization growth dimension parameter b can be set as 0.5 and 1.0, respectively. Thus, the crystallization nucleation parameter a is derived to be less than 1.0 according to the definition of Avrami constant n=a+bc. This means that the crystallizing rate of phosphate-enriched phase in steelmaking slags shows a decreasing trend with an increase of holding time.

  2. The apparent activation energy E of crystallization has been obtained by seven formulas of the crystallization rate constant k. The accurate results of apparent activation energy E of crystallization can be obtained by formulas M7 of k. The crystallization rate constant k is recommended as lnk=57.40+12,273.96/T8.25lnT5.5×103T, while the apparent activation energy E of crystallization is recommended as E=537.60206.015T kJ/mol based on formula M7 of k.

  3. The phosphate-enriched phase greater than 40 μm in the shape of one-dimensional rod can be formed in the quenched slag samples at cooling rate smaller than 3 K/min from 1773 to 1453 K in holding time of 60 min.

Funding statement: National Natural Science Foundation of China, (Grant / Award Number: ‘Nos. 51372019, 51174186, and 51072022’.).

Acknowledgments

The work was financially supported by the National Basic Research Program of China (No. 2014CB643401), the National Natural Science Foundation of China (Nos. 51372019, 51174186, and 51072022).

References

[1] R. Inoue and H. Suito, ISIJ Int., 46 (2006) 174–179.10.2355/isijinternational.46.174Search in Google Scholar

[2] H. Suito and R. Inoue, ISIJ Int., 46 (2006) 180–187.10.2355/isijinternational.46.180Search in Google Scholar

[3] R. Inoue and H. Suito, ISIJ Int., 46 (2006) 188–194.10.2355/isijinternational.46.188Search in Google Scholar

[4] W. Fix, H. Heyman and R. Heinke, J. Am. Ceram. Soc., 52 (1969) 346–347.10.1111/j.1151-2916.1969.tb11948.xSearch in Google Scholar

[5] L. Lin, Y.P. Bao, M. Wang and H.M. Zhou, Ironmaking Steelmaking, 41 (2014) 193–198.10.1179/1743281213Y.0000000117Search in Google Scholar

[6] Z.J. Wang, Y.Q. Sun, S. Sridhar, M. Zhang, M. Guo and Z.T. Zhang, Metall. Mater. Trans. B, 46B (2015) 537–541.10.1007/s11663-015-0303-4Search in Google Scholar

[7] Z.J. Wang, Y.Q. Sun, S. Sridhar, M. Zhang, M. Guo and Z.T. Zhang, Metall. Mater. Trans. B, 46B (2015) 2246–2254.10.1007/s11663-015-0391-1Search in Google Scholar

[8] J. Li, X.D. Wang and Z.T. Zhang, ISIJ Int., 51 (2011) 1396–1402.10.2355/isijinternational.51.1396Search in Google Scholar

[9] Y.Q. Sun, K. Zheng, J.L. Liao, X.D. Wang and Z.T. Zhang, ISIJ Int., 54 (2014) 1491–1497.10.2355/isijinternational.54.1491Search in Google Scholar

[10] Z.J. Wang, Y.Q. Sun, S. Sridhar, M. Zhang, M. Guo and Z.T. Zhang, ISIJ Int., 56 (2016) 546–553.10.2355/isijinternational.ISIJINT-2015-538Search in Google Scholar

[11] J.Y. Li, M. Zhang, M. Guo and X.M. Yang, Int. J. Min. Met. Mater., 23 (2016) 520–533.10.1007/s12613-016-1263-7Search in Google Scholar

[12] Z.J. Wang, Q.F. Shu, S. Sridhar, M. Zhang, M. Guo and Z.T. Zhang, Metall. Mater. Trans. B, 46B (2015) 758–765.10.1007/s11663-014-0270-1Search in Google Scholar

[13] X. Gao, H. Matsuura, M. Miyata and F. Tsukihashi, ISIJ Int., 53 (2013) 1381–1385.10.2355/isijinternational.53.1381Search in Google Scholar

[14] S.L. Xie, W.L. Wang, Y.Z. Liu and H. Matsuura, ISIJ Int., 54 (2014) 766–773.10.2355/isijinternational.54.766Search in Google Scholar

[15] K. Yoshiaki, C.E. Cicutti and A.W. Cramb, ISIJ Int., 38 (1998) 357–365.10.2355/isijinternational.38.357Search in Google Scholar

[16] M.C. Weinberg, D.P. Birnie III and V.A. Shneidman, J. Non-Cryst. Solids, 219 (1997) 89–99.10.1016/S0022-3093(97)00261-5Search in Google Scholar

[17] P.N. Kalu and D.R. Waryoba, Mat. Sci. Eng. A-Struct., 464 (2007) 68–75.10.1016/j.msea.2007.01.124Search in Google Scholar

[18] J.J. Li, J.C. Wang, Q. Xu and G.C. Yang, Acta Materialia, 55 (2007) 825–832.10.1016/j.actamat.2006.07.044Search in Google Scholar

[19] A.T. Lorenzo, M.L. Arnal, J. Albuerne and A.J. Muller, Polym. Test., 26 (2007) 222–231.10.1016/j.polymertesting.2006.10.005Search in Google Scholar

[20] S. Ranganathan and M.V. Heimendahl, J. Mater. Sci., 16 (1981) 2401–2404.10.1007/BF01113575Search in Google Scholar

[21] K. Matusita, T. Komatsu and R. Yokota, J. Mater. Sci., 19 (1984) 291–296.10.1007/BF02403137Search in Google Scholar

[22] S. Arrhenius, Z. Physik Chem., 226 (1889) 23–26.Search in Google Scholar

[23] A.V. Harecourt and W. Esson, Proc. Roy. Soc., 58 (1895) 112.Search in Google Scholar

[24] D. Dollimore, P. Tong and K.S. Alexander, Thermochim. Acta, 282/283 (1996) 13–27.10.1016/0040-6031(95)02810-2Search in Google Scholar

[25] M. Berthelot, Ann. De Chim. Et De Phys., 366 (1862) 110–117.Search in Google Scholar

[26] J.J. Hood, Phil. Mag., 20 (1885) 323.10.1080/14786448508627764Search in Google Scholar

[27] P. Simon, J. Therm. Anal. Calorim., 79 (2005) 703–708.10.1007/s10973-005-0599-4Search in Google Scholar

[28] D.M. Kooij, Int. J. Res. Phys. Chem. Chem. Phys., 12 (1893) 155–161.Search in Google Scholar

[29] J.H. van’t Hoff, Lectures on Theoretical and Physical Chemistry, Trans. R.A. Lechfeldt, Edward Arnold Publisher: Oxford, London, Part 1, Chemical Dynamics (1899) 230–235.Search in Google Scholar

[30] J.H. Flynn, Thermochim. Acta, 300 (1997) 83–92.10.1016/S0040-6031(97)00046-4Search in Google Scholar

[31] K. Ito, M. Yanagisawa and N. Sano, Tetsu–to–Hagané, 68 (1982) 342–344.10.2355/tetsutohagane1955.68.2_342Search in Google Scholar

[32] N. Wang, Z.G. Liang, M. Chen and Z.S. Zou, J. Iron Steel Res. Int., 18 (2011) 17–19, 39.Search in Google Scholar

[33] N. Wang, Z.G. Liang, M. Chen and Z.S. Zou, J. Iron Steel Res. Int., 18 (2011) 22–26.Search in Google Scholar

Received: 2016-11-27
Accepted: 2017-3-11
Published Online: 2017-6-1
Published in Print: 2018-4-25

© 2018 Walter de Gruyter GmbH, Berlin/Boston

This article is distributed under the terms of the Creative Commons Attribution Non-Commercial License, which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.

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