Hostname: page-component-586b7cd67f-r5fsc Total loading time: 0 Render date: 2024-11-29T07:30:22.294Z Has data issue: false hasContentIssue false

Aluminum in Magnesium Silicate Perovskite: Synthesis and Energetics of Defect Solid Solutions

Published online by Cambridge University Press:  01 February 2011

Alexandra Navrotsky
Affiliation:
Thermochemistry Facility and Center For High Pressure Research, Department of Chemical Engineering and Materials Science, University of California at Davis, Davis, CA 95616, USA
Mirko Schoenitz
Affiliation:
Thermochemistry Facility and Center For High Pressure Research, Department of Chemical Engineering and Materials Science, University of California at Davis, Davis, CA 95616, USA
Hiroshi Kojitani
Affiliation:
Thermochemistry Facility and Center For High Pressure Research, Department of Chemical Engineering and Materials Science, University of California at Davis, Davis, CA 95616, USA Department of Chemistry, Gakushuin University, Tokyo, Japan
Hongwu Xu
Affiliation:
Thermochemistry Facility and Center For High Pressure Research, Department of Chemical Engineering and Materials Science, University of California at Davis, Davis, CA 95616, USA
Jianzhong Zhang
Affiliation:
Center for High Pressure Research and Department of Geosciences, State University of New York at Stony Brook, Stony Brook, NY 11794, USA
Donald J. Weidner
Affiliation:
Center for High Pressure Research and Department of Geosciences, State University of New York at Stony Brook, Stony Brook, NY 11794, USA
Masaki Akaogi
Affiliation:
Department of Chemistry, Gakushuin University, Tokyo, Japan
Raymond Jeanloz
Affiliation:
Department of Geology and Geophysics, University of California at Berkeley, Berkeley, CA 94720, USA
Get access

Abstract

MgSiO3 - rich perovskite is expected to dominate the Earth's lower mantle (pressures > 25 GPa), with iron and aluminum as significant substituents. The incorporation of trivalent ions, M3+, may occur by two competing mechanisms: MgA+ SiB = MA + MB and SiB = AlB + 0.5 VO. Phase synthesis studies show that both substitutions do occur, and the nonstoichiometric or defect substitution is prevalent along the MgSiO3 - MgAlO2.5 join. Oxide melt solution calorimetry has been used to compare the energetics of both substitutions. The stoichiometric substitution, represented by the reaction 0.95 MgSiO3 (perovskite) + 0.05 Al2O3 (corundum) = Mg0.95Al0.10Si0.95O3 (perovskite), has an enthalpy of -0.8±2.2 kJ/mol. The nonstoichiometric reaction, 0.90 MgSiO3 (perovskite) + 0.10 MgO (rocksalt) + 0.05 Al2O3 (corundum) = MgSi0.9Al0.1O2.95 (perovskite) has a small positive enthalpy of 8.5±4.6 kJ/mol. The defect substitution is not prohibitive in enthalpy, entropy, or volume, is favored in perovskite coexisting with magnesiowüstite, and may significantly affect the elasticity, rheology and water retention of silicate perovskite in the Earth.

Type
Research Article
Copyright
Copyright © Materials Research Society 2002

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

1. Horiuchi, A., Ito, E., and Weidner, D. J., Am. Mineral. 72, 357360 (1987).Google Scholar
2. Shim, S. H. and Duffy, T. S., Am. Mineral. 85, 354363 (2000).Google Scholar
3. Hama, J. and Suito, K., J. Geophys. Res. 103, 74437462 (1998).Google Scholar
4. Fiquet, G., Dewaele, A., Andrault, D., Kunz, M., and Bihan, T. Le, Geophys. Res. Lett. 27, 2124 (2000).Google Scholar
5. Ito, E., Akaogi, M., Topor, L., and Navrotsky, A., Science 249, 12751278 (1990).Google Scholar
6. Akaogi, M. and Ito, E., Geophys. Res. Lett. 20, 18391842 (1993).Google Scholar
7. Liu, L., EPSL 36, 237245 (1977).Google Scholar
8. Kanzaki, M., Phys. Earth. Planet. Inter. 49, 168175 (1987).Google Scholar
9. Irifune, T., Koizumi, T., and Ando, J., Phys. Earth. Planet. Inter. 96, 147157 (1996).Google Scholar
10. O'Neill, B. and Jeanloz, R., J. Geophys. Res. 99, 1990119915 (1994).Google Scholar
11. Wood, B. J. and Rubie, D. C., Science 273, 15221524 (1996).Google Scholar
12. Anderson, O. L. and Hama, J., Am. Mineral. 84, 221225 (1999).Google Scholar
13. Fei, Y., “Solid solutions and element partitioning at high pressures and temperatures,” Reviews in Mineralogy - Ultrahigh-Pressure Mineralogy: Physics and Chemistry of Earth's Deep Interior, ed. Hemley, R. J., (Mineralogical Society of America, 1998) pp. 343367.Google Scholar
14. Hirsch, L. M. and Shankland, T. J., Geophys. Res. Lett. 18, 1305–308 (1991).Google Scholar
15. Fitz Gerald, J. D. and Ringwood, A. E., Phys. Chem. Miner. 18, 4046 (1991).Google Scholar
16. Navrotsky, A., Science 284, 17881789 (1999).Google Scholar
17. Kreuer, K. D., Solid State Ionics 97, 115 (1997).Google Scholar
18. Nowick, A. S. and Du, Y., Solid State Ionics 77, 137146 (1995).Google Scholar
19. Takahashi, T. and Iwahara, H., Rev. Chim. Miner. 17, 243253 (1980).Google Scholar
20. Navrotsky, A., Chem. Mater. 10, 27872793 (1998).Google Scholar
21. Topor, L. and Navrotsky, A., “Advances in calorimetric techniques for high pressure phases,” High Pressure Research: Application to Earth and Planetary Sciences, ed. Syono, Y. and Manghnani, M. (Tena Publishing Company and American Geophysical Union, 1992) pp. 7176.Google Scholar
22. Akaogi, M. and Ito, E., Phys. Earth Planet. Inter. 114, 129140 (1999).Google Scholar