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Thermal structure of the low velocity zone derived from laboratory and seismic investigations
Author(s) -
Sato Hiroki,
Sacks I. Selwyn,
Murase Tsutomu,
Scarfe Christopher M.
Publication year - 1988
Publication title -
geophysical research letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.007
H-Index - 273
eISSN - 1944-8007
pISSN - 0094-8276
DOI - 10.1029/gl015i011p01227
Subject(s) - asthenosphere , geology , low velocity zone , seismic velocity , peridotite , partial melting , mantle (geology) , plateau (mathematics) , lithosphere , geophysics , thermal , seismology , petrology , tectonics , meteorology , mathematical analysis , physics , mathematics
Laboratory measurements of seismic velocities in upper mantle peridotite can be used to constrain the thermal state in the low velocity zone. The measurements, carried out at high temperature and high confining pressure, can be extrapolated to upper mantle conditions. We compare laboratory velocities with seismic observations, and estimate temperatures and partial melt fractions in the low velocity zone. The comparison gives 1310°C and 7 vol.% partial melt at 45 km depth in 0‐5 my asthenosphere beneath the Iceland Plateau, and 1450°C and 3 vol.% partial melt at 85 km depth in 0‐20 my asthenosphere beneath the Pacific Ocean. The laboratory results show that up to a 6% velocity drop in the low velocity zone (relative to the lithospheric velocity) does not necessarily require the existence of partial melt. This implies that partial melt may not exist in the low velocity zone older than ∼5 my and ∼50 my in the Iceland Plateau and the Pacific Ocean, respectively.