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首页> 外文期刊>Journal of Materials Science >Approximated equations for molar volumes of pure solid fcc metals and their liquids from zero Kelvin to above their melting points at standard pressure
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Approximated equations for molar volumes of pure solid fcc metals and their liquids from zero Kelvin to above their melting points at standard pressure

机译:纯固体fcc金属及其液体在标准压力下从零开尔文到其熔点以上的摩尔体积的近似方程式

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摘要

Approximated equations have been constructed to describe the temperature (T) dependence of the molar volumes (V) of fcc solid metals (Ag, Al, Au, Cu, Ir, Ni, Pb, Pd, Pt, and Rh) and their liquids below and above their melting points at standard pressure of 1 bar from zero Kelvin. Below the melting point, the following new approximated equation is suggested for both the solid and liquid metals: V = a + b * T (to the power of n), where a, b, and n are semi-empirical parameters (at n larger than 1; this equation obeys the boundary condition that the thermal expansion coefficient becomes zero at T = 0 K). This approximated equation reproduces the measured molar volume of solids from zero Kelvin to melting point with an accuracy of 0.2 % or better. As a compromise, the derivative of this equation reproduces the measured thermal expansion coefficient of solids only with an accuracy 10 % or better and only above 100 K. Above the melting point, the following well-known equation is used for both liquid and solid phases: V = c + d * T, where c and d are semi-empirical parameters. This equation implies that the thermal expansion coefficient above the melting point has an approximately constant value. It is found that the volume change upon melting extrapolated to zero K is about 58 % of that at the melting point for all the 10 fcc metals. The tabulated 4 equations (below and above the melting point/for fcc and liquid states) are provided for each of the 10 fcc metals. These equations will be useful for estimating phase equilibria of nano-materials.
机译:已构建近似方程式来描述以下fcc固态金属(Ag,Al,Au,Cu,Ir,Ni,Pb,Pd,Pt和Rh)及其液体的摩尔体积(V)的温度(T)依赖性在高于零开尔文的1巴标准压力下高于熔点。在熔点以下,对于固体和液体金属,建议使用以下新的近似方程式:V = a + b * T(以n的幂为单位),其中a,b和n是半经验参数(在n大于1;此等式服从边界条件,即热膨胀系数在T = 0 K时变为零。该近似方程式再现了从零开尔文到熔点的测得的固体摩尔体积,精确度为0.2%或更高。作为折衷方案,该方程式的导数仅以10%或更高的精度且仅在100 K以上的温度下才能再现所测得的固体热膨胀系数。在熔点以上,液相和固相均使用以下众所周知的方程式:V = c + d * T,其中c和d是半经验参数。该方程式意味着高于熔点的热膨胀系数具有近似恒定的值。发现对于所有10fcc金属,在外推到零K时熔化时的体积变化为在熔点时的体积变化的约58%。为10种fcc金属中的每一种提供了列表的4个方程式(熔点以下和以上/ fcc和液态)。这些方程对于估计纳米材料的相平衡将是有用的。

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