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金的热膨胀:面心立方金属中的点缺陷浓度与预熔化

The thermal expansion of gold: point defect concentrations and pre-melting in a face-centred cubic metal.

作者信息

Pamato Martha G, Wood Ian G, Dobson David P, Hunt Simon A, Vočadlo Lidunka

机构信息

Department of Earth Sciences, University College London, Gower Street, London WC1E 6BT, UK.

出版信息

J Appl Crystallogr. 2018 Mar 26;51(Pt 2):470-480. doi: 10.1107/S1600576718002248. eCollection 2018 Apr 1.

Abstract

On the basis of computer simulations, pre-melting phenomena have been suggested to occur in the elastic properties of hexagonal close-packed iron under the conditions of the Earth's inner core just before melting. The extent to which these pre-melting effects might also occur in the physical properties of face-centred cubic metals has been investigated here under more experimentally accessible conditions for gold, allowing for comparison with future computer simulations of this material. The thermal expansion of gold has been determined by X-ray powder diffraction from 40 K up to the melting point (1337 K). For the entire temperature range investigated, the unit-cell volume can be represented in the following way: a second-order Grüneisen approximation to the zero-pressure volumetric equation of state, with the internal energy calculated a Debye model, is used to represent the thermal expansion of the 'perfect crystal'. Gold shows a nonlinear increase in thermal expansion that departs from this Grüneisen-Debye model prior to melting, which is probably a result of the generation of point defects over a large range of temperatures, beginning at / > 0.75 (a similar homologous to where softening has been observed in the elastic moduli of Au). Therefore, the thermodynamic theory of point defects was used to include the additional volume of the vacancies at high temperatures ('real crystal'), resulting in the following fitted parameters: = ()/γ = 4.04 (1) × 10 J, = 67.1671 (3) Å, = (' - 1)/2 = 3.84 (9), θ = 182 (2) K, (/Ω)exp(/) = 1.8 (23) and = 0.9 (2) eV, where is the unit-cell volume at 0 K, and ' are the isothermal incompressibility and its first derivative with respect to pressure (evaluated at zero pressure), γ is a Grüneisen parameter, is the Debye temperature, , and are the vacancy formation volume, enthalpy and entropy, respectively, Ω is the average volume per atom, and is Boltzmann's constant.

摘要

基于计算机模拟,有人提出在地球内核条件下,六方密堆积铁在熔化前的弹性性质中会出现预熔化现象。本文在更易于实验的金的条件下,研究了这些预熔化效应在面心立方金属物理性质中可能出现的程度,以便与该材料未来的计算机模拟结果进行比较。通过X射线粉末衍射测定了金从40 K到熔点(1337 K)的热膨胀。在所研究的整个温度范围内,晶胞体积可以用以下方式表示:采用零压体积状态方程的二阶格林爱森近似,并用德拜模型计算内能,来表示“完美晶体”的热膨胀。金的热膨胀呈现非线性增加,在熔化前偏离了这个格林爱森-德拜模型,这可能是由于在很宽的温度范围内产生了点缺陷,起始温度为/ > 0.75(这与在金的弹性模量中观察到软化的相似同源温度)。因此,使用点缺陷的热力学理论来考虑高温下空位的额外体积(“真实晶体”),得到以下拟合参数: = ()/γ = 4.04 (1) × 10 J, = 67.1671 (3) Å, = (' - 1)/2 = 3.84 (9),θ = 182 (2) K,(/Ω)exp(/) = 1.8 (23) 以及 = 0.9 (2) eV,其中 是0 K时的晶胞体积, 和 ' 分别是等温不可压缩性及其对压力的一阶导数(在零压力下求值),γ 是格林爱森参数, 是德拜温度, 、 和 分别是空位形成体积、焓和熵,Ω 是每个原子的平均体积, 是玻尔兹曼常数。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49d7/5884389/7104b0e6e66a/j-51-00470-fig1.jpg

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