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Heat capacity and microstructure of ordered and disordered Pd3V

机译:有序和无序Pd3V的热容和微观结构

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Differences in the heat capacity and thermal expansion of cubic (fcc-disordered) and tetragonal (DO22-ordered) Pd3V were measured from 40 K to 315 K. Below 100 K the heat capacity difference was consistent with harmonic vibrations. At higher temperatures, however, the data show significant anharmonic effects. Measurements of elastic constants, densities and thermal expansion showed that the anharmonic volume expansion contribution (C-p - C-V) could account for only about one-third of this anharmonic heat capacity difference. The remainder may originate with elastic and plastic deformation of the polycrystalline microstructure. Strain energy from anisotropic thermal contractions of grains in the tetragonal ordered phase contributes to the heat capacity, but some of this strain energy is eliminated by plastic deformation. The vibrational entropy difference of disordered and ordered Pd3V was estimated to be S-dis - S-ord = (+0.035 +/- 0.001)k(B)/atom at 300 K, with 70% of this coming from anharmonic effects. [References: 23]
机译:立方(fcc无序)和四方(DO22序)Pd3V的热容量和热膨胀差异在40 K至315 K范围内测量。低于100 K时,热容量差异与谐波振动一致。然而,在较高温度下,数据显示出明显的非谐效应。弹性常数,密度和热膨胀的测量结果表明,非谐体积膨胀贡献(C-p-C-V)只能解决这一非谐热容差的三分之一。其余部分可能来自多晶微结构的弹性和塑性变形。晶粒在四方有序相中的各向异性热收缩产生的应变能有助于提高热容,但是这种应变能中的一部分通过塑性变形消除。在300 K时,无序和有序Pd3V的振动熵差估计为S-dis-S-ord =(+0.035 +/- 0.001)k(B)/原子,其中70%来自非谐效应。 [参考:23]

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