Japan Geoscience Union Meeting 2014

Presentation information

International Session (Oral)

Symbol S (Solid Earth Sciences) » S-IT Science of the Earth's Interior & Techtonophysics

[S-IT03_29AM2] Structure and dynamics of Earth and Planetary deep interiors

Tue. Apr 29, 2014 11:00 AM - 12:45 PM 418 (4F)

Convener:*Satoru Tanaka(Institute for Research on Earth Evolution Japan Agency for Marine-Earth Science and Technology), Takashi Yoshino(Institute for Study of the Earth's Interior, Okayama University), Masanori Kameyama(Geodynamics Research Center, Ehime University), Dapeng Zhao(Department of Geophysics, Tohoku University), John Hernlund(ELSI, Tokyo TECH), Chair:Masanori Kameyama(Geodynamics Research Center, Ehime University), Nozomu Takeuchi(Earthquake Research Institute, University of Tokyo)

11:30 AM - 11:45 AM

[SIT03-10] Phase transitions and mineral chemistry in pyrolite at 1600-2200C across 660-km seismic discontinuity

*Takayuki ISHII1, Hiroshi KOJITANI1, Masaki AKAOGI1 (1.Depertment of chemistry, Gakushuin University)

Keywords:post-spinel transition, 660-km seismic discontinuity, mantle plume, pyrolite, post-garnet transition

It is widely accepted that pyrolite is a model rock which represents the chemical composition of the Earth's upper mantle. Because the post-spinel transition in pyrolite occurs at about 23 GPa along mantle geotherm (e.g. Litasov et al. 2005), it has been accepted that the transition is responsible for the seismic 660-km discontinuity. Slow velocity anomalies by global seismic tomography which may indicate mantle upwelling have been found in the transition zone and the lower mantle, and these regions are higher in temperature than average mantle. To elucidate the origin and dynamics of the mantle plume, informations on phase relations in pyrolite are essential. However, few investigations on phase relations in pyrolite have been made at hot-plume temperatures (1800-2200C) (Hirose, 2002; Nishiyama and Yagi, 2003). In this study, we demonstrated detailed phase equilibrium experiments in pyrolite composition at hot plume conditions.The starting material was prepared as the oxide mixture in pyrolite composition after McDonugh and Sun (1995) excluding minor components (MnO, K2O and P2O5). Quench experiments were made at about 20-28 GPa and 1600-2200C for 2-10 hours using a Kawai-type 6-8 multianvil high-pressure apparatus at Gakushuin University. The starting material was packed with pressure calibrants (MgSiO3 and pyrope) in a Re multi-sample capsule. A LaCrO3 heater and a W5%Re-W26%Re thermocouple were inserted in a Cr2O3-doped MgO pressure medium. Phases of recovered samples were identified with microfocus-Xray diffractometer and SEM-EDS.The mineral assemblages of MgSiO3-rich perovskite (Mpv) + magnesiowustite (Mw) + garnet (Gt) + CaSiO3-perovskite (Cpv) and Mpv + Mw + Cpv at 1600-2200C are stable at pressure range of 22-24 GPa and above 24 GPa, respectively. The mineral assemblage of ringwoodite (Rw) + Gt + Cpv at 1600C changes to that of Rw + Mw + Gt + Cpv at 1800-2000C, and Rw disappears perfectly above 2200C. From mass balance calculation of analyzed compositions of the phases, we found that Gt content increases with increasing temperature before and after formation of Mpv. We also calculated the densities in pyrolite at each temperature. The density of average pyrolite mantle (1600C) is higher than pyrolite plume (1800-2200C) across 660-km discontinuity due to increase in Gt content with increasing temperature. Therefore, we conclude that hot-plume ascending nearby 660-km discontinuity has positive buoyancy by the phase transitions.