液态镍基合金中氮与铬、钼的瓦格纳相互作用系数

L. A. Bolʼshov, S. K. Korneichuk, E. L. Bolʼshova
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It is supposed that the liquid solutions in the Fe – Ni – Cr and Fe – Ni – Mo systems are perfect. Within the framework of the proposed theory, the relation is obtained that expresses the Wagner interaction coefficient between nitrogen and chromium in liquid nickel-based alloys \\(\\varepsilon _{\\rm{N}}^{{\\rm{Cr}}}\\)(Ni). The right-hand part of the appropriate formula is a function of the Wagner interaction coefficients between nitrogen and chromium \\(\\varepsilon _{\\rm{N}}^{{\\rm{Cr}}}\\)(Fe) and between nitrogen and nickel \\(\\varepsilon _{\\rm{N}}^{{\\rm{Ni}}}\\)(Fe) in liquid iron-based alloys. A similar relation is obtained for the Wagner interaction coefficient between nitrogen and molybdenum in liquid nickel-based alloys \\(\\varepsilon _{\\rm{N}}^{{\\rm{Mo}}}\\)(Ni). According to the first of these formulas, the value \\(\\varepsilon _{\\rm{N}}^{{\\rm{Cr}}}\\)(Ni) = –21,9 at a temperature of 1873 K is calculated. 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引用次数: 0

摘要

作者提出了Fe - Ni - Cr和Fe - Ni - Mo系合金中液氮溶液热力学性质的简单理论。该理论类似于作者之前在2019年和2021年提出的Fe - Cr和Fe - Ni体系二元合金中液氮溶液的理论。该理论建立在Fe - Ni - Cr体系和Fe - Ni - Mo体系三元液体溶液晶格模型的基础上。该模型假定为FCC晶格。Fe, Ni, Cr和Mo原子沉积在晶格的位置上。氮原子位于八面体间隙中。氮原子只与相邻晶格位上的金属原子相互作用。这种相互作用是两两的。假定这种相互作用的能量既不取决于成分,也不取决于温度。认为Fe - Ni - Cr体系和Fe - Ni - Mo体系的液相是完美的。在提出的理论框架内,得到了液态镍基合金\(\varepsilon _{\rm{N}}^{{\rm{Cr}}}\) (Ni)中氮和铬之间的瓦格纳相互作用系数的关系式。适当公式的右边部分是液态铁基合金中氮和铬\(\varepsilon _{\rm{N}}^{{\rm{Cr}}}\) (Fe)以及氮和镍\(\varepsilon _{\rm{N}}^{{\rm{Ni}}}\) (Fe)之间瓦格纳相互作用系数的函数。液态镍基合金\(\varepsilon _{\rm{N}}^{{\rm{Mo}}}\) (Ni)中氮与钼的瓦格纳相互作用系数也有类似的关系。根据第一个公式,计算出温度为1873 K时的值\(\varepsilon _{\rm{N}}^{{\rm{Cr}}}\) (Ni) = - 21,9。这对应于Langenberg相互作用系数\(e _{\rm{N}}^{{\rm{Cr}}}\) (Ni) = -0,108的值,与实验估计相符。根据第二个公式,在温度1873 K时计算出\(\varepsilon _{\rm{N}}^{{\rm{Mo}}}\) (Ni) = - 14,3。这对应于Langenberg相互作用系数\(e _{\rm{N}}^{{\rm{Cr}}}\) (Ni) = - 0.036,与实验估计\(\varepsilon _{\rm{N}}^{{\rm{Mo}}}\) (Ni) = - 15,1符合得很好;\(e _{\rm{N}}^{{\rm{Cr}}}\) (Ni) = - 0.038。
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Wagner interaction coefficients of nitrogen with chromium and molibdenum in liquid nickel-based alloys
The authors propose a simple theory of thermodynamic properties of liquid nitrogen solutions in alloys of the Fe – Ni – Cr and Fe – Ni – Mo systems. This theory is analogous to the theory for liquid nitrogen solutions in binary alloys of the Fe – Cr and Fe – Ni systems proposed previously by the authors in 2019 and 2021. The theory is based on lattice model of ternary liquid solutions of the Fe – Ni – Cr and Fe – Ni – Mo systems. The model assumes a FCC lattice. Atoms of Fe, Ni, Cr and Mo are deposed in the sites of the lattice. Nitrogen atoms are located in octahedral interstices. The nitrogen atom interacts only with the metal atoms located in the lattice sites neighboring to it. This interaction is pairwise. It is assumed that the energy of this interaction depends neither on composition nor on temperature. It is supposed that the liquid solutions in the Fe – Ni – Cr and Fe – Ni – Mo systems are perfect. Within the framework of the proposed theory, the relation is obtained that expresses the Wagner interaction coefficient between nitrogen and chromium in liquid nickel-based alloys \(\varepsilon _{\rm{N}}^{{\rm{Cr}}}\)(Ni). The right-hand part of the appropriate formula is a function of the Wagner interaction coefficients between nitrogen and chromium \(\varepsilon _{\rm{N}}^{{\rm{Cr}}}\)(Fe) and between nitrogen and nickel \(\varepsilon _{\rm{N}}^{{\rm{Ni}}}\)(Fe) in liquid iron-based alloys. A similar relation is obtained for the Wagner interaction coefficient between nitrogen and molybdenum in liquid nickel-based alloys \(\varepsilon _{\rm{N}}^{{\rm{Mo}}}\)(Ni). According to the first of these formulas, the value \(\varepsilon _{\rm{N}}^{{\rm{Cr}}}\)(Ni) = –21,9 at a temperature of 1873 K is calculated. This corresponds to the value of the Langenberg interaction coefficient \(e _{\rm{N}}^{{\rm{Cr}}}\)(Ni) = –0,108, which coincides with experimental estimate. According to the second formula, the value \(\varepsilon _{\rm{N}}^{{\rm{Mo}}}\)(Ni) = –14,3 is calculated at a temperature 1873 K. This corresponds to the value of the Langenberg interaction coefficient \(e _{\rm{N}}^{{\rm{Cr}}}\)(Ni) = –0,036, which is in satisfactory agreement with the experimental estimate \(\varepsilon _{\rm{N}}^{{\rm{Mo}}}\)(Ni) = –15,1; \(e _{\rm{N}}^{{\rm{Cr}}}\)(Ni) = –0,038.
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