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Determination of Activity Coefficients of Elements and Related Thermodynamic Properties of Fe-Si Binary Melts Based on the Atom-Molecule Coexistence Theory

机译:基于原子-分子共存理论的Fe-Si二元熔体元素活度系数及相关热力学性质的确定

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摘要

The Raoultian activity coefficient γ_(Si)~0 of Si and γ_(Fe)~0 of Fe in the infinitely dilute solution of Fe-Si binary melts at temperatures of 1693, 1773, 1873, and 1973 K have been determined from the calculated mass action concentrations N_i of structural units in Fe-Si binary melts based on the atom and molecule coexistence theory (AMCT). The activity coefficients of elements γ_i relative to pure liquid matter as standard state or f_%, _i referred to 1 mass percentage as standard state or f_H, i based on the hypothetical pure liquid matter as standard state have been obtained. The values of first-order activity interaction coefficient ε_i~i or e_i~i or h_i~i of Si and Fe related with activity coefficients γ_i or f_%, _i or f_H, _i of Si and Fe are also determined. The standard molar Gibbs free energy change of dissolving liquid element i(l) for forming 1 mass percentage of element i in Fe-Si binary melts have been deduced in a temperature range from 1693 K to 1973 K. The molar mixing thermodynamic properties, such as molar mixing Gibbs energy change/enthalpy change/entropy change of Fe-Si binary melts have been reliably determined in a temperature range from 1693 K to 1973 K. The excess values and excess degrees of the above-mentioned molar mixing thermodynamic properties of Fe-Si binary melts have been also determined based on ideal solution or regular solution as a basis, respectively. The determined molar mixing Gibbs energy change of Fe-Si binary melts is equal to that based on regular solution as a basis in the full composition range of Fe-Si binary melts in a temperature range from 1693 K to 1973 K. The partial mixing thermodynamic properties of Si and Fe are not recommended to obtain from the calculated mass action concentration N_(Si) of Si and N_(Fe) of Fe as well as the measured activity a_R, _(Si) of Si and a_R, _(Fe) of Fe in Fe-Si binary melts.
机译:通过计算,求出了在1693、1773、1873和1973 K温度下无限稀释的Fe-Si二元熔体的Si的Raoultian活度系数γ_(Si)〜0和Fe的γ_(Fe)〜0。基于原子和分子共存理论(AMCT),Fe-Si二元熔体中结构单元的质量作用浓度N_i。基于假设的纯液体物质作为标准状态,已经获得了相对于作为标准状态的纯液体物质或f _%,_ i被称为1质量百分比的标准状态或f_H,i的元素γ_i的活度系数。还确定与活性系数γ_i或f _%,_ i或f_H,Si和Fe的_i有关的Si和Fe的一阶活性相互作用系数ε_i〜i或e_i〜i或h_i〜i的值。在1693 K至1973 K的温度范围内,推导了在Fe-Si二元熔体中形成1质量%的元素i的溶解液态元素i(l)的标准摩尔吉布斯自由能变化。作为摩尔混合法,已经可靠地确定了在1693 K至1973 K的温度范围内Fe-Si二元熔体的吉布斯能量变化/焓变化/熵变化。上述Fe摩尔混合热力学性质的过量值和过量度还分别基于理想溶液或常规溶液确定了-Si二元熔体。 Fe-Si二元熔体的确定的摩尔混合Gibbs能量变化等于在1693 K至1973 K的温度范围内Fe-Si二元熔体的整个组成范围内基于常规溶液的摩尔变化Gibbs能量变化。不建议从计算出的Si的质量作用浓度N_(Si)和Fe的N_(Fe)以及测得的Si和a_R的_(Si)和a_R的活性(_)中获得Si和Fe的性质Fe-Si二元熔融物中的Fe

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