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铬的高压高温相图及状态方程的表征

Characterization of the high-pressure and high-temperature phase diagram and equation of state of chromium.

作者信息

Anzellini Simone, Errandonea Daniel, Burakovsky Leonid, Proctor John E, Turnbull Robin, Beavers Christine M

机构信息

Diamond Light Source Ltd., Harwell Science and Innovation Campus, Diamond House, Didcot, OX11 0DE, UK.

Departamento de Física Aplicada-Instituto de Ciencia de Materiales, Matter at High Pressure (MALTA) Consolider Team, Universidad de Valencia, Edificio de Investigación, C/Dr. Moliner 50, Burjassot, 46100, Valencia, Spain.

出版信息

Sci Rep. 2022 Apr 25;12(1):6727. doi: 10.1038/s41598-022-10523-2.

Abstract

The high-pressure and high-temperature phase diagram of chromium has been investigated both experimentally (in situ), using a laser-heated diamond-anvil cell technique coupled with synchrotron powder X-ray diffraction, and theoretically, using ab initio density-functional theory simulations. In the pressure-temperature range covered experimentally (up to 90 GPa and 4500 K, respectively) only the solid body-centred-cubic and liquid phases of chromium have been observed. Experiments and computer calculations give melting curves in agreement with each other that can both be described by the Simon-Glatzel equation [Formula: see text]. In addition, a quasi-hydrostatic equation of state at ambient temperature has been experimentally characterized up to 131 GPa and compared with the present simulations. Both methods give very similar third-order Birch-Murnaghan equations of state with bulk moduli of 182-185 GPa and respective pressure derivatives of 4.74-5.15. According to the present calculations, the obtained melting curve and equation of state are valid up to at least 815 GPa, at which pressure the melting temperature is 9310 K. Finally, from the obtained results, it was possible to determine a thermal equation of state of chromium valid up to 65 GPa and 2100 K.

摘要

铬的高压高温相图已通过实验(原位)和理论两种方法进行了研究。实验方面,采用激光加热金刚石对顶砧技术结合同步辐射粉末X射线衍射;理论方面,使用从头算密度泛函理论模拟。在实验覆盖的压力 - 温度范围内(分别高达90吉帕和4500开尔文),仅观察到铬的体心立方固态和液相。实验和计算机计算得出的熔化曲线相互吻合,均可用西蒙 - 格拉策尔方程[公式:见原文]描述。此外,在室温下对高达131吉帕的准静水压状态方程进行了实验表征,并与当前模拟结果进行了比较。两种方法得出的三阶Birch - Murnaghan状态方程非常相似,体积模量为182 - 185吉帕,压力导数分别为4.74 - 5.15。根据当前计算,所得熔化曲线和状态方程至少在815吉帕范围内有效,此时熔化温度为9310开尔文。最后,根据所得结果,有可能确定铬在高达65吉帕和2100开尔文范围内有效的热状态方程。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01c6/9038929/b3fddfd62a68/41598_2022_10523_Fig1_HTML.jpg

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