Formation of a metastable olivine wedge in a descending slab
Open Access
- 10 November 1997
- journal article
- research article
- Published by American Geophysical Union (AGU) in Journal of Geophysical Research
- Vol. 102 (B11) , 24627-24637
- https://doi.org/10.1029/97jb02334
Abstract
We present a thermal model of a descending slab in which the transformation of olivine to spinel is controlled by pressure‐ and temperature‐dependent reaction kinetics. Two different formulations of the kinetics are considered with the main discriminant being the temperature range over which olivine converts to spinel at pressures of about 15 GPa (about 500°–515°C and 560°–650°C). We use a finite element method to solve the coupled heat conduction (perpendicular and parallel to the dip of the slab) and kinetics equations, and we include the latent heat of the phase transformation. Latent heat release together with heat conduction parallel to the dip of the slab reduces significantly the length of the metastable olivine wedge and results in a very thin (≲5 km) two‐phase region. We employ the thermal parameter υτ sin δ (υ is the velocity of the descending slab, τ is the age of the slab, and δ is the dip of the slab to the horizontal) to interpret the results for the length of the metastable wedge. For values of the thermal parameter smaller than about 4000 and 7000 km, depending on the model of the kinetics, no metastable olivine wedge exists (the critical value of 7000 km for the thermal parameter corresponds to the kinetics model with the lowest transition temperature range). The length of the metastable olivine wedge is also found to be very sensitive to the model of the kinetics and to the effects of adiabatic heating. If the occurrence of deep earthquakes is related to the transformation of metastable olivine to spinel, then data on earthquake depth versus thermal parameter require that the onset of the reaction takes place at temperatures of about 550°–575°C. In this case the slab thermal parameter must be larger than 10,000 km for the metastable olivine wedge to extend down to 660 km depth. But deep earthquakes occur near 660 km depth in slabs with thermal parameter as small as about 5000 km (South America, for example). Either some deep earthquakes are unrelated to olivine metastability or our knowledge of olivine‐spinel reaction kinetics is incomplete.This publication has 19 references indexed in Scilit:
- Phase transition buoyancy contributions to stresses in subducting lithosphereGeophysical Research Letters, 1996
- The metastable olivine wedge in fast subducting slabs: Constraints from thermo-kinetic couplingEarth and Planetary Science Letters, 1996
- The Mechanics of Deep EarthquakesAnnual Review of Earth and Planetary Sciences, 1995
- Transformation mechanisms of San Carlos olivine to (MgFe)2SiO4 β-phase under subduction zone conditionsPhysics of the Earth and Planetary Interiors, 1994
- Phase transition Clapeyron slopes and transition zone seismic discontinuity topographyJournal of Geophysical Research, 1994
- The effects of phase transition kinetics on subducting slabsGeophysical Research Letters, 1993
- Olivine‐modified spinel‐spinel transitions in the system Mg2SiO4‐Fe2SiO4: Calorimetric measurements, thermochemical calculation, and geophysical applicationJournal of Geophysical Research, 1989
- Stress distribution due to olivine‐spinel phase transition in descending plate and deep focus earthquakesJournal of Geophysical Research, 1987
- Relations among subduction parametersReviews of Geophysics, 1986
- The kinetics of grain boundary nucleated reactionsActa Metallurgica, 1956