钢液中氢与镍相互作用的瓦格纳系数

L. A. Bolʼshov, S. K. Korneichuk, E. L. Bolʼshova
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引用次数: 0

摘要

最简单的结构和原子间相互作用模型应用于Fe - Ni体系液态合金中的氢溶液,该模型先前(2019 - 2021)被作者用于Fe - Cr、Fe - Mn、Fe - Ni、Ni - Co和Ni - Cr体系合金中的氮溶液。该理论基于铁-镍溶液的晶格模型。该模型假定为FCC晶格。在晶格的位置是铁和镍原子。氢原子位于八面体的间隙中。氢原子只与邻近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合金成分,也不取决于温度。为简单起见,我们假定Fe - Ni体系中的液体溶液是完美的。在提出的理论框架内,给出了钢液中氢与镍相互作用的瓦格纳系数的表达式。适当公式的右边部分是氢在液态铁和液态镍中溶解度的西弗茨定律常数之比的函数。温度为1873 K时,这些常数的值等于K 'H (Fe) = 0,0025,K 'H (Ni) = 0,0040 wt。%。同时,估计了钢液中氢与镍相互作用的瓦格纳系数 εHNi = - 0,54。这对应于Langenberg相互作用系数eHNi = - 0.002的值,这与实验估计值eHNi = - 0.0022非常接近。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Wagner coefficient of interaction between hydrogen and nickel in liquid steel
The simplest model of the structure and interatomic interaction is applied to hydrogen solutions in liquid alloys of Fe – Ni system, which earlier (2019 – 2021) was used by the authors for nitrogen solutions in alloys of Fe – Cr, Fe – Mn, Fe – Ni, Ni – Co and Ni – Cr systems. The theory is based on lattice model of the Fe – Ni solutions. The model assumes a FCC lattice. In the sites of this lattice are the atoms of Fe and Ni. Hydrogen atoms are located in octahedral interstices. The hydrogen 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 the alloy composition nor on the temperature. For simplicity it was assumed that liquid solutions in the Fe – Ni system are perfect. Within the framework of the proposed theory an expression is presented for the Wagner coefficient of interaction between hydrogen and nickel in liquid steel. The right-hand part of the appropriate formula is a function of the ratio of the Sieverts law constants for hydrogen solubility in liquid iron and in liquid nickel. The values of these constants for a temperature of 1873 K are taken equal to K′H(Fe) = 0,0025, K′H(Ni) = 0,0040 wt. %. At the same time, an estimate was obtained for the Wagner coefficient of interaction between hydrogen and nickel in liquid steel  εHNi = –0,54. This corresponds to the value of the Langenberg interaction coefficient eHNi = –0,002, wich is very close to the experimental estimate eHNi = –0,0022.
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