Abstract
According to the experimental results of hot metal dephosphorization by CaO-based slags at a commercial-scale hot metal pretreatment station, activity \( a_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \) of P2O5 in the CaO-based slags has been determined using the calculated comprehensive mass action concentration \( N_{{{\text{Fe}}_{t} {\text{O}}}}^{{}} \) of iron oxides by the ion and molecule coexistence theory (IMCT) for representing the reaction ability of Fe t O, i.e., activity of \( a_{{{\text{Fe}}_{t} {\text{O}}}}^{{}} \). The collected ten models from the literature for predicting activity coefficient \( \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \) of P2O5 in CaO-based slags have been evaluated based on the determined activity \( a_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \) of P2O5 by the IMCT as the criterion. The collected ten models of activity coefficient \( \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \) of P2O5 in CaO-based slags can be described in the form of a linear function as \( \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \equiv y = c_{0} + c_{1} x \), in which independent variable \( x \) represents the chemical composition of slags, intercept \( c_{0} \) including the constant term depicts temperature effect and other unmentioned or acquiescent thermodynamic factors, and slope \( c_{1} \) is regressed by the experimental results. Thus, a general approach for obtaining good prediction results of activity \( a_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \) of P2O5 in CaO-based slags is proposed by revising the constant term in intercept \( c_{0} \) for the collected ten models. The better models with an ideal revising possibility or flexibility in the collected ten models have been selected and recommended.
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Abbreviations
- a i :
-
Activity of component i in slags or element i in liquid iron, (–)
- \( a_{{{\text{R, }}i}} \) :
-
Activity of components i in slags or element i in liquid iron relative to pure solid or liquid component i or element i as standard state with mole fraction \( x_{i} \) as concentration unit and following Raoult’s law under the condition of taking ideal solution as reference state, i.e., \( a{_{{\rm R},i}} = x{_{i}} \gamma{_{i}} \), (–)
- \( a_{\%,{{i}}} \) :
-
Activity of element i in liquid iron referred to 1 mass percentage of element i as a standard state with mass percentage [pct i] as a concentration unit and obeying Henry’s law under the condition of taking the infinitely dilute ideal solution as a reference state, i.e., \( a_{\%,{{i}}} = [{\text{pct }}i]f_{\%,{{i}}} \), (–)
- \( c_{0} \) :
-
Coefficient of intercept in linear function of \( y = c_{0} + c_{1} x \), (–)
- \( c^{\prime}_{0} \) :
-
Coefficient of intercept in linear function of \( y_{{}}^{\prime} = c_{0}^{\prime} + c_{1}^{\prime} x \), (–)
- \( c_{1} \) :
-
Coefficient of slope in linear function of \( y = c_{0} + c_{1} x \), (–)
- \( c^{\prime}_{1} \) :
-
Coefficient of slope in linear function of \( y_{{}}^{\prime} = c_{0}^{\prime} + c_{1}^{\prime} x \), (–)
- \( d_{0}^{{}} \) :
-
Coefficient of intercept in linear function of \( \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} ,{\text{ predicted}}}}^{{}} = d_{0}^{{}} + d_{1}^{{}} \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} ,{\text{determined}}}}^{{}} \), (–)
- \( d_{1}^{{}} \) :
-
Coefficient of slope in linear function of \( \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} ,{\text{ predicted}}}}^{{}} = d_{0}^{{}} + d_{1}^{{}} \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} ,{\text{determined}}}}^{{}} \), (–)
- \( f_{\%,{{i}}} \) :
-
Activity coefficient of element i in liquid iron related with activity \( a_{\%,{{i}}}\), (–)
- \( \Delta_{\text{r}} G_{{{\text{m, }}i}}^{\Theta } \) :
-
Standard molar Gibbs free energy change of reaction for forming component i or structural unit i, (J/mol)
- \( K_{i}^{\Theta } \) :
-
Standard equilibrium constant of chemical reaction for forming component i or structural unit i, (–)
- M i :
-
Relative atomic mass of element i or relative molecular mass of component i, (–)
- m :
-
Number of experimental points, (–)
- \( p_{i} \) :
-
Partial pressure of species i in gaseous phase, (Pa)
- \( p^{\Theta } \) :
-
Standard pressure of gas at sea level and 273 K as 101,325 Pa, (Pa)
- R :
-
Gas constant, (8.314 J/(mol·K))
- \( R^{2} \) :
-
Adjusted parameter of the regressed function, (–)
- T :
-
Absolute temperature, (K)
- \( x \) :
-
Independent variable, (–)
- \( x_{i} \) :
-
Mole fraction of component i, (–)
- \( y \) :
-
Dependent variable, (–)
- \( y_{{}}^{\prime} \) :
-
Dependent variable, (–)
- \( \Delta y \) :
-
Disagreements between determined and predicted results of \( \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \), i.e., \( \Delta y = \Delta \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} = \left| {y - y^{\prime} } \right| = \left| {c_{0} - c_{0}^{\prime} } \right| \), (–)
- \( \overline{\Delta y} \) :
-
Mean disagreements between determined and predicted results of \( \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \) for m experimental points, i.e., \( \overline{\Delta y} = \frac{{\Delta \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} }}{m} = \frac{{\left| {y - y_{{}}^{\prime\prime} } \right|}}{m} = \frac{{\left| {\Delta y} \right|}}{m} \), (–)
- (pct i):
-
Mass percentage of component i in slags, (\( \times \)10−2, –)
- [pct i]:
-
Mass percentage of element i in liquid iron, (\( \times \)10−2, –)
- (i):
-
Species i in slag phase, (–)
- [i]:
-
Species i in liquid iron phase, (–)
- \( \varLambda \) :
-
Optical basicity of slags, (–)
- \( \varLambda_{i} \) :
-
Optical basicity of component i in slags, (–)
- \( \delta_{{{\text{slope, }}\gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} }} \) :
-
Deviation of slope \( c_{1}^{\prime} \) relative to measured slope \( c_{1}^{{}} \) as a basis, defined as \( \delta_{{{\text{slope, }}\gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} }} = \frac{{\left| {c_{1}^{{}} - c_{1}^{\prime} } \right|}}{{c_{1}^{{}} }} \times 100 \), (\( \times \)10−2, –)
- \( \delta_{\text{slope}}^{{}} \) :
-
Deviation of slope \( d_{1}^{{}} \) relative to 1.0 as a basis, defined as \( \delta_{\text{slope}}^{{}} = \sum {\left( {\frac{{\left| {1.0 - d_{1}^{{}} } \right|}}{1.0}} \right)} \times 100 \), (\( \times \)10−2, –)
- \( \delta_{{\gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} }} \) :
-
Mean deviation of \( \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} \) between determined and predicted ones by model for m points, defined as \( \delta_{{\gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} }} }} = \frac{1}{m}\sum {\left( {\frac{{\left| {\log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} ,{\text{determined}}}}^{{}} - \log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} ,{\text{ predicted}}}}^{i} } \right|}}{{\left| {\log \gamma_{{{\text{P}}_{ 2} {\text{O}}_{ 5} ,{\text{determined}}}}^{{}} } \right|}}} \right)} \times 100 \), (\( \times \)10−2, –)
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This work is supported by the National Natural Science Foundation of China (NSFC) under Grant No. 51174186.
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Manuscript submitted October 2, 2015.
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Yang, Xm., Li, Jy., Chai, GM. et al. Critical Assessment of P2O5 Activity Coefficients in CaO-based Slags during Dephosphorization Process of Iron-based Melts. Metall Mater Trans B 47, 2330–2346 (2016). https://doi.org/10.1007/s11663-016-0654-5
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DOI: https://doi.org/10.1007/s11663-016-0654-5