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Detailed Reference Information |
Woodland, A.B., Angel, R.J., Koch, M., Kunz, M. and Miletich, R. (1999). Equations of state for Fe32+Fe23+Si3O12 “skiagite” garnet and Fe2SiO4-Fe3O4 spinel solid solutions. Journal of Geophysical Research 104: doi: 10.1029/1999JB900206. issn: 0148-0227. |
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The equations of state of Fe32+Fe23+Si3O12, or skiagite garnet, and two Fe2SiO4-Fe3O4 spinel solid solutions were determined from room temperature hydrostatic compression experiments up to 11 GPa performed at the European Synchrotron Radiation Facility. These data indicate that there are no first-order phase transitions or changes in compression mechanism in skiagite garnet or Fe3+-bearing silicate spinel solid solutions up to 11 GPa at room temperature. Skiagite garnet has an isothermal bulk modulus K0T=157.4(3.0) GPa and a pressure derivative of the isothermal bulk modulus K0T'=6.7(8), where numbers in parentheses represent 1 estimated standard deviation of these values. Combination of this result with those for other silicate garnets reveals an inverse linear relationship between the octahedral cation-oxygen (Y-O) bond length and the bulk modulus. The dominating effect of the octahedral site on the bulk compression of garnet can be understood by considering that the octahedral-tetrahedral network has no rigid unit modes and that no cation substitution occurs on the tetrahedral sites in these garnets. It is apparent that the incorporation of Fe3+ and Cr acts to lower the bulk modulus of aluminosilicate garnets. Consideration of the effect of compression on the molar volume results in nonsystematic changes in calculated oxygen fugacity for garnet-bearing mantle peridotites that equilibrated at high pressures. The pressure-volume data obtained from two Fe3+-bearing silicate spinel solid solutions with compositions Xfay=0.45 and Xfay=0.57 (fay, fayalite component) yielded similar enough values of K0T and K0T' to warrant a combined refinement with the data points scaled to the appropriate zero-pressure volumes. This gave K0T=168.9(1.2) GPa and K0T'=5.7(1.2) with &khgr;W2=4.6 (weighted &khgr;2) and K0T=175.5(1.4) GPa when K0T' is fixed equal to 4 (&khgr;W2=4.9). Our solid solutions have significantly lower bulk moduli than either magnetite or Fe2SiO4 spinel end-members or indeed many other spinels. ¿ 1999 American Geophysical Union |
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Abstract |
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Keywords
Mineral Physics, Equations of state, Mineral Physics, High-pressure behavior, Mineralogy and Petrology, Crystal chemistry |
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Publisher
American Geophysical Union 2000 Florida Avenue N.W. Washington, D.C. 20009-1277 USA 1-202-462-6900 1-202-328-0566 service@agu.org |
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