P-V-T equation of state of Ca3Cr2Si3O12 uvarovite garnet by using a diamond-anvil cell and in-situ synchrotron X-ray diffraction
P-V-T equation of state of Ca3Cr2Si3O12 uvarovite garnet by using a diamond-anvil cell and in-situ synchrotron X-ray diffraction
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使用金刚石砧池和原位同步加速器 X 射线衍射得到 Ca3Cr2Si3O12 钙铬榴石石榴石的 P-V-T 状态方程
DOI:
10.2138/am-2015-5002
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发表时间:
2015-02
影响因子:
3.1
通讯作者:
Hongsen Xie
中科院分区:
文献类型:
--
作者:
Dawei Fan;Jingui Xu;Maining Ma;Shuyi Wei;Bo Zhang;Jing Liu;Hongsen Xie
Abstract The pressure-volume-temperature (P-V-T) equation of state (EoS) of synthetic uvarovite has been measured at high temperatures up to 900 K and high pressures up to 16.20 GPa, by using in situ angle-dispersive X-ray diffraction and diamond-anvil cell. Analysis of room-temperature P-V data to a third-order Birch-Murnaghan EoS yielded: V0 = 1736.9 ± 0.5 Å3, K0 = 162 ± 2 GPa, and K′0 = 4.5 ± 0.3. With K′0 fixed to 4.0, we obtained: V0 = 1736.5 ± 0.3 Å3 and K0 = 164 ± 1 GPa. Fitting of our PV- T data by means of the high-temperature third-order Birch-Murnaghan equations of state, given the thermoelastic parameters: V0 = 1736.8 ± 0.8 Å3, K0 = 162 ± 3 GPa, K′0 = 4.3 ± 0.4, (∂K/∂T)P = -0.021 ± 0.004 GPa/K, and α0 = (2.72 ± 0.14)×10-5 K-1. We compared our elastic parameters to the results from the previous studies for uvarovite. From the comparison of these fittings, we propose to constrain the bulk modulus and its pressure derivative to K0 = 162 GPa and K′0 = 4.0-4.5 for uvarovite. Present results were also compared with previous studies for other ugrandite garnets, grossular and andradite, which indicated that the compression mechanism of uvarovite might be similar with grossular and andradite. Furthermore, a systematic relationship, K0 (GPa) = 398.1(7)-0.136(8) V0 (Å3) with a correlation coefficient R2 of 0.9999, has been established based on these isostructural analogs. Combining these results with previous studies for pyralspite garnets-pyrope, almandine, and spessartine-the compositional dependence of the thermoelastic parameters (bulk modulus, thermal expansion, and the temperature derivative of the bulk modulus) were discussed.
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影响因子:
3.2
作者:
K. Zhuravlev;A. Goncharov;S. Tkachev;P. Dera;V. Prakapenka
通讯作者:
K. Zhuravlev;A. Goncharov;S. Tkachev;P. Dera;V. Prakapenka
影响因子:
3.1
作者:
M. Wildner;M. Andrut
通讯作者:
M. Wildner;M. Andrut
影响因子:
1.4
作者:
Jianzhong Zhang
通讯作者:
Jianzhong Zhang
影响因子:
2.3
作者:
F. Guyot;Yanbin Wang;P. Gillet;Y. Ricard
通讯作者:
F. Guyot;Yanbin Wang;P. Gillet;Y. Ricard
影响因子:
1.4
作者:
Li Zhang;H. Ahsbahs;Ali Kutoglu;C. Geiger
通讯作者:
Li Zhang;H. Ahsbahs;Ali Kutoglu;C. Geiger