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Ab initio calculations of mechanical, thermodynamic and electronic structure properties of mullite, iota-alumina and boron carbide.

机译:莫来石,碘氧化铝和碳化硼的机械,热力学和电子结构性质的从头算。

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摘要

The alumino-silicate solid solution series (Al 4+2xSi2-2 xO10-x) is an important class of ceramics. Except for the end member (x=0), Al2 SiO5 the crystal structures of the other phases, called mullite, have partially occupied sites. Stoichiometric supercell models for the four mullite phases 3Al2O 3 · 2SiO2 · 2Al 2O3 · SiO2, 4 Al2O3· SiO 2, 9Al2O3 · SiO2, and iota-Al2 O3 (iota-alumina) are constructed starting from experimentally reported crystal structures. A large number of models were built for each phase and relaxed using the Vienna ab initio simulation package (VASP) program. The model with the lowest total energy for a given x was chosen as the representative structure for that phase. Electronic structure and mechanical properties of mullite phases were studied via first-principles calculations.;Of the various phases of transition alumina, iota-Al 2O3 is the least well known. In addition structural details have not, until now, been available. It is the end member of the aluminosilicate solid solution series with x=1. Based on a high alumina content mullite phase, a structural model for iota- Al2O3 is constructed. The simulated x-ray diffraction (XRD) pattern of this model agrees well with a measured XRD pattern. The iota-Al2 O3 is a highly disordered ultra-low-density phase of alumina with a theoretical density of 2854kg/m3. Using this theoretically constructed model, elastic, thermodynamic, electronic, and spectroscopic properties of iota-Al2 O3 have been calculated and compared it with those of alpha- Al2O3 and gamma- Al2O3.;Boron carbide (B4C) undergoes an amorphization under high velocity impacts. The mechanism of amorphization is not clear. Ab initio methods are used to carry out large-scale uniaxial compression simulations on two polytypes of stoichiometric boron carbide (B4C), B 11C-CBC, and B12- CCC where B11C or B12 is the 12-atom icosahedron and CBC or CCC is the three-atom chain. The simulations were performed on large supercells of 180 atoms. Simulated results indicate bending of the three-atom chain leads to the amorphization of the B 11C-CBC (B12-CCC ) at a uniaxial strain s=0.23 (0.22) and with a maximum stress of 168 (151) GPa. The mechanism of amorphization is analyzed with radial pair distribution function (RPDF), total density of states (TDOS), and the distribution of effective charges on atoms.
机译:铝硅酸盐固溶体系列(Al 4 + 2xSi2-2 xO10-x)是一类重要的陶瓷。除端部成员(x = 0)外,Al2 SiO5的其他相的晶体结构(称为莫来石)具有部分占据的位置。从实验报告的晶体结构开始,构建了四个莫来石相3Al2O 3·2SiO2·2Al 2O3·SiO2、4 Al2O3·SiO 2,9Al​​2O3·SiO2和iota-Al2 O3(iota-氧化铝)的化学计量超级电池模型。每个阶段都建立了大量模型,并使用Vienna从头算模拟程序包(VASP)程序进行放松。选择给定x的总能量最低的模型作为该阶段的代表结构。通过第一性原理计算研究了莫来石相的电子结构和力学性能。在过渡氧化铝的各种相中,最鲜为人知的是iota-Al 2O3。此外,到目前为止,尚无结构细节。它是x = 1的铝硅酸盐固溶体系列的末端成员。基于高铝含量的莫来石相,建立了碘铝-氧化铝的结构模型。该模型的模拟X射线衍射(XRD)图与测量的XRD图非常吻合。 iota-Al2 O3是一种高度无序的氧化铝超低密度相,理论密度为2854kg / m3。使用该理论构建的模型,已计算出iota-Al2 O3的弹性,热力学,电子和光谱性质,并将其与α-Al2O3和γ-Al2O3的性质进行了比较;碳化硼(B4C)在高速冲击下发生了非晶化。非晶化的机制尚不清楚。从头算方法用于对化学计量的碳化硼(B4C),B 11C-CBC和B12-CCC的两种多型体进行大规模单轴压缩模拟,其中B11C或B12是12原子的二十面体,而CBC或CCC是三原子链。模拟是在180个原子的大型超级电池上进行的。模拟结果表明,三原子链的弯曲导致B 11C-CBC(B12-CCC)在单轴应变s = 0.23(0.22)且最大应力为168(151)GPa时非晶化。通过径向对分布函数(RPDF),状态总密度(TDOS)以及原子上有效电荷的分布来分析非晶化的机理。

著录项

  • 作者

    Aryal, Sita Ram.;

  • 作者单位

    University of Missouri - Kansas City.;

  • 授予单位 University of Missouri - Kansas City.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2012
  • 页码 174 p.
  • 总页数 174
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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