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The influence of porosity and crack morphology on seismic velocity and permeability in the upper oceanic crust
Author(s) -
Carlson R. L.
Publication year - 2014
Publication title -
geochemistry, geophysics, geosystems
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.928
H-Index - 136
ISSN - 1525-2027
DOI - 10.1002/2013gc004965
Subject(s) - geology , porosity , permeability (electromagnetism) , crust , asperity (geotechnical engineering) , lava , oceanic crust , dike , mineralogy , petrology , geophysics , seismology , geotechnical engineering , volcano , subduction , genetics , tectonics , membrane , biology
The purpose of this study is to explore the relationships between porosity, crack morphology, seismic velocity, and permeability in the upper oceanic crust. In a theoretical model, velocity is a quadratic function of porosity Φ, and the coefficients are functions of the fractional area of asperity contact A f across the cracks, a measure of crack morphology; thus, v  =  v ( A f , Φ). Fits to data sets from the lava and dike sections in Holes 504B and 1256D yield A f  = 0.096(8) and 0.045(3), with rms errors of 1.7 and 0.3%, respectively. Lower values of A f account for the high porosities and low velocities observed in Layer 2A. After 0.2 Ma, the porosities of both Layer 2A and the deeper part of the lava pile remain in the range 8 ± 4%. The observed increase of Layer 2A velocities after 0.2 Ma is caused largely by changing crack morphology as opposed to decreasing porosity; at 8% porosity, an increase of A f from ∼0.003 to 0.1 accounts for an increase of velocity from ∼3 to >5 km/s. An empirical log‐linear relationship between permeability κ and v suggests a relationship between κ and A f as well. This relationship between κ and v can be explained if the permeability coefficient κ o is a closely constrained quadratic function of the area of asperity contact A f . A f is thus the primary variable affecting both seismic velocities and the permeability of the uppermost oceanic crust.

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