TY - JOUR
T1 - Mechanism and kinetics of the post-spinel transformation in Mg2SiO4
AU - Kubo, Tomoaki
AU - Otani, Eiji
AU - Kato, Takumi
AU - Urakawa, Satoru
AU - Suzuki, Akio
AU - Kanbe, Yuichi
AU - Funakoshi, Ken Ichi
AU - Utsumi, Wataru
AU - Kikegawa, Takumi
AU - Fujino, Kiyoshi
N1 - Funding Information:
We are grateful to T. Nagase and D. Yamazaki for useful discussions. N. Tomioka and T. Miyamoto helped the TEM and SEM observations, respectively. We also acknowledge T. Okada and H. Terasaki for their supports to the in situ X-ray diffraction experiments. Constructive reviews by D. Andrault and J. Mosenfelder were helpful to improve the manuscript. T. Kubo was supported by Research Fellowships of the Japan Society for the Promotion of Science for Young Scientists. This work was partially supported by the Grant-in-Aid for Scientific Research A (no. 09304051) to E. O. in situ X-ray diffraction experiments were carried out using the SPEED1500 system at BL04B1 of SPring-8 (proposal no. 1998A0130-ND-np) and the MAX90 system at BL14C of KEK-PF (proposal no. 98G264).
PY - 2002
Y1 - 2002
N2 - Mechanisms and kinetics of the post-spinel transformation in Mg2SiO4 were examined at 22.7-28.2 GPa and 860-1200°C by in situ X-ray diffraction experiments using synchrotron radiation combined with microstructural observations of the recovered samples. The post-spinel phases nucleated on spinel grain boundaries and grew with a lamellar texture. Under large overpressure conditions, reaction rims were formed along spinel grain boundaries at the initial stage of the transformation, whereas under small overpressure conditions, the transformation proceeded without formation of reaction rims. Mg2SiO4 spinel metastably dissociated into MgSiO3 ilmenite and periclase, and stishovite and periclase as intermediate steps in the transformation into the stable assemblage of MgSiO3 perovskite and periclase. Topotactic relationships were found in the transformation from spinel into ilmenite and periclase. Kinetic parameters in the Avrami rate equation, time taken to 10% completion, and the growth rate were estimated by analysis of the kinetic data obtained by in situ X-ray observations. The empirical activation energy for 10% transformation decreases with increasing pressure because the activation energy for nucleation becomes smaller at larger overpressure conditions. Extrapolations of the 10% transformation to ∼700°C, which is the lowest temperature expected for the cold slabs at ∼700 km depth, suggest that overpressure of more than ∼1 GPa is needed for the transformation. Because the growth rate is estimated to be large even at low-temperatures of ∼700°C and overpressures of 1 GPa, the depth of the post-spinel transformation in the cold slabs is possibly controlled by nucleation kinetics.
AB - Mechanisms and kinetics of the post-spinel transformation in Mg2SiO4 were examined at 22.7-28.2 GPa and 860-1200°C by in situ X-ray diffraction experiments using synchrotron radiation combined with microstructural observations of the recovered samples. The post-spinel phases nucleated on spinel grain boundaries and grew with a lamellar texture. Under large overpressure conditions, reaction rims were formed along spinel grain boundaries at the initial stage of the transformation, whereas under small overpressure conditions, the transformation proceeded without formation of reaction rims. Mg2SiO4 spinel metastably dissociated into MgSiO3 ilmenite and periclase, and stishovite and periclase as intermediate steps in the transformation into the stable assemblage of MgSiO3 perovskite and periclase. Topotactic relationships were found in the transformation from spinel into ilmenite and periclase. Kinetic parameters in the Avrami rate equation, time taken to 10% completion, and the growth rate were estimated by analysis of the kinetic data obtained by in situ X-ray observations. The empirical activation energy for 10% transformation decreases with increasing pressure because the activation energy for nucleation becomes smaller at larger overpressure conditions. Extrapolations of the 10% transformation to ∼700°C, which is the lowest temperature expected for the cold slabs at ∼700 km depth, suggest that overpressure of more than ∼1 GPa is needed for the transformation. Because the growth rate is estimated to be large even at low-temperatures of ∼700°C and overpressures of 1 GPa, the depth of the post-spinel transformation in the cold slabs is possibly controlled by nucleation kinetics.
KW - High-pressure and high-temperature
KW - Kinetics
KW - Pst-spinel transformation
KW - Subducting slab
KW - Synchrotron radiation
KW - Transmission electron microscopy
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U2 - 10.1016/S0031-9201(01)00270-9
DO - 10.1016/S0031-9201(01)00270-9
M3 - Article
AN - SCOPUS:0036170414
SN - 0031-9201
VL - 129
SP - 153
EP - 171
JO - Physics of the Earth and Planetary Interiors
JF - Physics of the Earth and Planetary Interiors
IS - 1-2
ER -