评估钢中 MgAl2O4-Ti2O3 复合夹杂物的吸附聚合机制

Yan Wang, Zhanlong Piao, Shuoming Wang, Liguang Zhu, Jinxia Huo
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引用次数: 0

摘要

对晶粒内针状铁素体包裹体的研究表明,由 Ti2O3 吸附析出的高熔点氧化物 MgAl2O4 内核和复合包裹体可用作氧化物冶金中的有效成核颗粒。然而,这种吸附行为的微观机制仍不清楚。因此,本研究采用基于密度泛函理论的第一性原理计算,研究了钢中 MgAl2O4(100)Mg- 和 MgAl2O4(111)O3(Mg)- 端面上 Ti2O3 的吸附和聚合机制。计算基于 DFT 第一性原理,由 CASTEP 代码在平面波基集下进行。交换相关能和相关效应通过使用 Perdew-Burke-Ernzerhof (PBE) 函数的广义梯度近似(GGA)来描述。所有计算都考虑了自旋极化。超软伪势(USPP)被用来描述电子-离子的相互作用。在目前的工作中,平面波基的能量截止点设定为 620 eV。对于布里渊区取样,我们采用 Monkhorst-Pack 方法对 MgAl2O4 体进行了 3 × 3 × 3 k 点网格划分。在 MgAl2O4 的顶面上方添加了一个 20.0 Å 的真空层,以消除表面法线周期性重复的相互作用。研究结果表明,当 Ti2O3 在 MgAl2O4(100)Mg- 和 MgAl2O4(111)O3(Mg)- 端面最稳定的吸附位置位于 TAl 和 FMg 时,吸附能最高且最稳定。最稳定的吸附构型位于垂直和平行(P1)表面。通过比较分析,发现吸附 Ti2O3 的最佳表面是 MgAl2O4(111)O3(Mg)- 端面,吸附行为主要发生在表面的第一层原子上。最佳吸附构型为 P1,当 Ti2O3 与表面形成成对连接的三个环并嵌入 MgAl2O4(111)O3(Mg) 端面表面时,吸附模式最佳。这项研究深入揭示了钢中 MgAl2O4-Ti2O3 复合物夹杂物的吸附聚合机制,有助于制造新型低熔点氧化物和硫化物。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Evaluations of the Adsorption Polymerization Mechanisms of MgAl2O4–Ti2O3 Complex Inclusions in Steel

Evaluations of the Adsorption Polymerization Mechanisms of MgAl2O4–Ti2O3 Complex Inclusions in Steel

Research on intragranular acicular ferrite inclusions has demonstrated that high-melting-point oxide MgAl2O4 cores and composite inclusions precipitated by Ti2O3 adhesion can be used as effective nucleation particles in oxide metallurgy. However, the microscopic mechanism underlying this adsorption behavior remains unclear. Hence, in this study, the adsorption and polymerization mechanisms of Ti2O3 on the MgAl2O4(100)Mg- and MgAl2O4(111)O3(Mg)-terminal surfaces in steel were studied using first-principles calculations based on density functional theory. The calculation based on the first principles of DFT and performed by the CASTEP code under plane wave basis set. The exchange correlation energy and correlation effects were described by generalized gradient approximation (GGA) using the Perdew–Burke–Ernzerhof (PBE) function. Spin polarization was considered in all calculation. Ultrasoft pseudopotentials (USPP) was employed to describe the electron-ion interactions. The energy cutoff for the plane wave basis was set at 620 eV in the current work. For the Brillouin zone sampling, we carried out 3 × 3 × 3 k-points mesh for MgAl2O4 bulk using the method of Monkhorst-Pack. A vacuum layer of 20.0 Å is added above the top surface of MgAl2O4 to eliminate the interaction of the normal periodic repetition of the surfaces. In all the surface calculations, the use of symmetry in bulk crystal was failed and k-point grids is set to 3 × 3 × 1. The results of this study revealed that when the most stable adsorption positions of Ti2O3 on the surface of MgAl2O4(100)Mg- and MgAl2O4(111)O3(Mg)-terminal are located at TAl and FMg, the adsorption energy is the highest and the most stable. The most stable adsorption configurations are located on vertical and parallel (P1) surfaces. Through comparative analysis, the best surface for Ti2O3 adsorption was found to be the MgAl2O4(111)O3(Mg)-terminal surface, and the adsorption behavior mainly occurred on the first layer of atoms on the surface. The best adsorption configuration was P1, and the best adsorption mode occurred when Ti2O3 formed three rings connected in pairs with the surface and embedded in the surface of the MgAl2O4(111)O3(Mg)-terminal. This study provides insights into the adsorption polymerization mechanisms of MgAl2O4–Ti2O3 complex inclusions in steel that could facilitate the fabrication of novel low-melting-point oxides and sulfides.

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