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

机译:金的热膨胀:点缺陷浓度和面心立方金属中的预熔

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摘要

On the basis of ab initio 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 via 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 T/T m > 0.75 (a similar homologous T 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: Q = (V 0 K 0)/γ = 4.04 (1) × 10−18 J, V 0 = 67.1671 (3) Å3, b = (K 0′ − 1)/2 = 3.84 (9), θD = 182 (2) K, (v f/Ω)exp(s f/k B) = 1.8 (23) and h f = 0.9 (2) eV, where V 0 is the unit-cell volume at 0 K, K 0 and K 0′ are the isothermal incompressibility and its first derivative with respect to pressure (evaluated at zero pressure), γ is a Grüneisen parameter, θ D is the Debye temperature, v f, h f and sf are the vacancy formation volume, enthalpy and entropy, respectively, Ω is the average volume per atom, and kB is Boltzmann’s constant.
机译:根据从头算的计算机模拟,已经暗示在熔融之前地球内芯的条件下,六方密堆积铁的弹性会发生预熔融现象。在这里,已经在实验上更容易接近的金的条件下研究了以面心为中心的立方金属的物理性能中也可能发生这些预熔作用的程度,从而可以与该材料的未来计算机模拟进行比较。金的热膨胀是通过X射线粉末衍射从40 K到熔点(1337 K)来确定的。对于所研究的整个温度范围,可以通过以下方式表示晶胞体积:零压力状态方程的二阶Grüneisen近似值,以及通过Debye模型计算的内部能量,用于表示“完美晶体”的热膨胀。金在熔化之前显示出不同于此Grüneisen-Debye模型的热膨胀的非线性增加,这可能是在T / T m> 0.75开始的较大温度范围内产生点缺陷的结果(相似的同源性在A的弹性模量中观察到软化的T。因此,使用点缺陷的热力学理论包括高温下额外的空位体积(“真实晶体”),得出以下拟合参数:Q =(V 0 K 0)/γ= 4.04(1) ×10 −18 J,V 0 = 67.1671(3)Å 3 ,b =(K 0′− 1)/ 2 = 3.84(9),θD= 182 (2)K,(v f /Ω)exp(s f / k B)= 1.8(23)和h f = 0.9 (2)eV,其中V 0是0 K时的晶胞体积, K 0和 K 0'是等温不可压缩性及其相对于压力的一阶导数(在零压力下评估),γ是Grüneisen参数,θ D是德拜温度, v f h f s f 分别是空位形成体积,焓和熵,Ω是每个原子的平均体积,而 k B是玻尔兹曼常数。

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