Thermal equation of state of natural tourmaline at high pressure and temperature |
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Authors: | Jingui Xu Yunqian Kuang Bo Zhang Yonggang Liu Dawei Fan Xiaodong Li Hongsen Xie |
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Institution: | 1.Key Laboratory of High Temperature and High Pressure Study of the Earth’s Interior, Institute of Geochemistry,Chinese Academy of Sciences,Guiyang,China;2.University of Chinese Academy of Sciences,Beijing,China;3.Center for High Pressure Science and Technology Advanced Research,Changchun,China;4.Beijing Synchrotron Radiation Facility, Institute of High Energy Physics,Chinese Academy of Sciences,Beijing,China |
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Abstract: | Synchrotron-based in situ angle-dispersive X-ray diffraction experiments were conducted on a natural uvite-dominated tourmaline sample by using an external-heating diamond anvil cell at simultaneously high pressures and temperatures up to 18 GPa and 723 K, respectively. The angle-dispersive X-ray diffraction data reveal no indication of a structural phase transition over the P–T range of the current experiment in this study. The pressure–volume–temperature data were fitted by the high-temperature Birch–Murnaghan equation of state. Isothermal bulk modulus of K 0 = 96.6 (9) GPa, pressure derivative of the bulk modulus of \(K_{0}^{\prime } = 12.5 (4)\), thermal expansion coefficient of α 0 = 4.39 (27) × 10?5 K?1 and temperature derivative of the bulk modulus (?K/?T) P = ?0.009 (6) GPa K?1 were obtained. The axial thermoelastic properties were also obtained with K a0 = 139 (2) GPa, \(K_{a0}^{\prime }\) = 11.5 (7) and α a0 = 1.00 (11) × 10?5 K?1 for the a-axis, and K c0 = 59 (1) GPa, \(K_{c0}^{\prime }\) = 11.4 (5) and α c0 = 2.41 (24) × 10?5 K?1 for the c-axis. Both of axial compression and thermal expansion exhibit large anisotropic behavior. Thermoelastic parameters of tourmaline in this study were also compared with that of the other two ring silicates of beryl and cordierite. |
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