The compressibility at room temperature and the thermal expansion at room pressure of two disordered crystals (space group C2/c) obtained by annealing a natural omphacite sample (space group P2/n) of composition close to Jd56Di44 and Jd55Di45, respectively, have been studied by single-crystal X-ray diffraction. Using a Birch–Murnaghan equation of state truncated at the third order [BM3-EoS], we have obtained the following coefficients: V0 = 421.04(7) Å^3, KT0 = 119(2) GPa, K’ = 5.7(6). A parameterized form of the BM3 EoS was used to determine the axial moduli of a, b and c. The anisotropy scheme is βc < βa < βb, with an anisotropy ratio 1.05:1.00:1.07. A fitting of the lattice variation as a function of temperature, allowing for linear dependency of the thermal expansion coefficient on the temperature, yielded αV(1bar,303K) = 2.64(2) x 10-5 K-1 and an axial thermal expansion anisotropy of αb ≫ αa>αc. Comparison of our results with available data on compressibility and thermal expansion shows that while a reasonable ideal behaviour can be proposed for the compressibility of clinopyroxenes in the jadeite–diopside binary join [KT0 as a function of Jd molar %: KT0 = 106(1) GPa + 0.28(2)x Jd(mol%)], the available data have not sufficient quality to extract the behaviour of thermal expansion for the same binary join in terms of composition.

New thermoelastic parameters of natural C2/c omphacite

CAMARA ARTIGAS, Fernando;
2012-01-01

Abstract

The compressibility at room temperature and the thermal expansion at room pressure of two disordered crystals (space group C2/c) obtained by annealing a natural omphacite sample (space group P2/n) of composition close to Jd56Di44 and Jd55Di45, respectively, have been studied by single-crystal X-ray diffraction. Using a Birch–Murnaghan equation of state truncated at the third order [BM3-EoS], we have obtained the following coefficients: V0 = 421.04(7) Å^3, KT0 = 119(2) GPa, K’ = 5.7(6). A parameterized form of the BM3 EoS was used to determine the axial moduli of a, b and c. The anisotropy scheme is βc < βa < βb, with an anisotropy ratio 1.05:1.00:1.07. A fitting of the lattice variation as a function of temperature, allowing for linear dependency of the thermal expansion coefficient on the temperature, yielded αV(1bar,303K) = 2.64(2) x 10-5 K-1 and an axial thermal expansion anisotropy of αb ≫ αa>αc. Comparison of our results with available data on compressibility and thermal expansion shows that while a reasonable ideal behaviour can be proposed for the compressibility of clinopyroxenes in the jadeite–diopside binary join [KT0 as a function of Jd molar %: KT0 = 106(1) GPa + 0.28(2)x Jd(mol%)], the available data have not sufficient quality to extract the behaviour of thermal expansion for the same binary join in terms of composition.
2012
39
295
304
http://www.springerlink.com/content/0342-1791/#BrowseSection
Omphacite; High pressure; High temperature; Single crystal; X-ray diffraction
Pandolfo F; Nestola F; Cámara F; Domeneghetti MC
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/91771
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