%0 Journal Article %1 revil1998 %A Revil, A. %A Glover, P. W. J. %D 1998 %I American Geophysical Union %J Geophysical Research Letters %K 1998 clays electrical-conductivity sands sandstone surface-conductivity %P 691-694 %T Nature of Surface Electrical Conductivity in Natural Sands, Sandstones, and Clays %U http://dx.doi.org/10.1029/98GL00296 %V 25 %X The electrical conductivity of rocks results from conduction through the bulk solution occupying the pores and from surface conduction occurring at the fluid/grain interface. The nature of the surface electrical conductivity of shaly and clean sands and sandstones is examined. Surface conduction is characterized by the specific surface conductance which is the sum of three contributions: (i) Conduction within the electrical diffuse layer, which makes a negligible contribution to the total specific surface conductance, (ii) Conduction in the Stern layer, which is shown to vary significantly with the salinity of the pore fluid at low salinities (10−6 to 10−3 mol 1−1), but becomes independent of salinity at higher salinities, (iii) A mechanism operating directly on the mineral surface, independent of salinity, and perhaps associated with proton transfer. At salinities higher than 10−3 mol 1−1 and at 25°C, the specific surface conductance of quartz and clays is equal to 8.9×10−9 S and 2.5×10−9 S respectively. Equations describing the influence of surface conductivity and microstructure upon the macroscopic electrical conductivity of sands, sandstones, and shales are also developed.

@article{revil1998, abstract = {The electrical conductivity of rocks results from conduction through the bulk solution occupying the pores and from surface conduction occurring at the fluid/grain interface. The nature of the surface electrical conductivity of shaly and clean sands and sandstones is examined. Surface conduction is characterized by the specific surface conductance which is the sum of three contributions: (i) Conduction within the electrical diffuse layer, which makes a negligible contribution to the total specific surface conductance, (ii) Conduction in the Stern layer, which is shown to vary significantly with the salinity of the pore fluid at low salinities (10−6 to 10−3 mol 1−1), but becomes independent of salinity at higher salinities, (iii) A mechanism operating directly on the mineral surface, independent of salinity, and perhaps associated with proton transfer. At salinities higher than 10−3 mol 1−1 and at 25°C, the specific surface conductance of quartz and clays is equal to 8.9×10−9 S and 2.5×10−9 S respectively. Equations describing the influence of surface conductivity and microstructure upon the macroscopic electrical conductivity of sands, sandstones, and shales are also developed.}, added-at = {2009-10-01T15:24:42.000+0200}, author = {Revil, A. and Glover, P. W. J.}, biburl = {https://www.bibsonomy.org/bibtex/2a25df846aecaa658c2debbd09ac5f8bc/schepers}, description = {Nature of surface electrical conductivity in natural sands, sandstones, and clays}, interhash = {c66df2c9d0520636124c486d67c37b18}, intrahash = {a25df846aecaa658c2debbd09ac5f8bc}, journal = {Geophysical Research Letters}, keywords = {1998 clays electrical-conductivity sands sandstone surface-conductivity}, pages = {691-694}, publisher = {American Geophysical Union}, timestamp = {2009-10-01T15:24:42.000+0200}, title = {Nature of Surface Electrical Conductivity in Natural Sands, Sandstones, and Clays}, url = {http://dx.doi.org/10.1029/98GL00296}, volume = 25, year = 1998 }