%0 Journal Article %1 Nover:September2005:0169-3298:593 %A Nover, Georg %D 2005 %J Surveys in Geophysics %K 2005 cru crustal electrical-conductivity explanation laboratory measurements properties review %P 593-651(59) %R doi:10.1007/s10712-005-1759-6 %T Electrical Properties of Crustal and Mantle Rocks A Review of Laboratory Measurements and their Explanation %U http://www.ingentaconnect.com/content/klu/geop/2005/00000026/00000005/00001759 %V 26 %X The electrical properties of rocks and minerals are controlled by thermodynamic parameters like pressure and temperature and by the chemistry of the medium in which the charge carriers move. Four different charge transport processes can be distinguished. Electrolytic conduction in fluid saturated porous rocks depends on petrophysical properties, such as porosity, permeability and connectivity of the pore system, and on chemical parameters of the pore fluid like ion species, its concentration in the pore fluid and temperature. Additionally, electrochemical interactions between water dipoles or ions and the negatively charged mineral surface must be considered. In special geological settings electronic conduction can increase rock conductivities by several orders of magnitude if the highly conducting phases (graphite or ores) form an interconnected network. Electronic and electrolytic conduction depend moderately on pressure and temperature changes, while semiconduction in mineral phases forming the Earth's mantle strongly depends on temperature and responds less significantly to pressure changes. Olivine exhibits thermally induced semiconduction under upper mantle conditions; if pressure and temperature exceed ~ 14GPa and 1400C, the phase transition olivine into spinel will further enhance the conductivity due to structural changes from orthorhombic into cubic symmetry. The thermodynamic parameters (temperature, pressure) and oxygen fugacity control the formation, number and mobility of charge carriers. The conductivity temperature relation follows an Arrhenius behaviour, while oxygen fugacity controls the oxidation state of iron and thus the number of electrons acting as additional charge carriers. In volcanic areas rock conductivities may be enhanced by the formation of partial melts under the restriction that the molten phase is interconnected. These four charge transport mechanisms must be considered for the interpretation of geophysical field and borehole data. Laboratory data provide a reproducible and reliable database of electrical properties of homogenous mineral phases and heterogenous rock samples. The outcome of geoelectric models can thus be enhanced significantly. This review focuses on a compilation of fairly new advances in experimental laboratory work together with their explanation.

@article{Nover:September2005:0169-3298:593, abstract = {The electrical properties of rocks and minerals are controlled by thermodynamic parameters like pressure and temperature and by the chemistry of the medium in which the charge carriers move. Four different charge transport processes can be distinguished. Electrolytic conduction in fluid saturated porous rocks depends on petrophysical properties, such as porosity, permeability and connectivity of the pore system, and on chemical parameters of the pore fluid like ion species, its concentration in the pore fluid and temperature. Additionally, electrochemical interactions between water dipoles or ions and the negatively charged mineral surface must be considered. In special geological settings electronic conduction can increase rock conductivities by several orders of magnitude if the highly conducting phases (graphite or ores) form an interconnected network. Electronic and electrolytic conduction depend moderately on pressure and temperature changes, while semiconduction in mineral phases forming the Earth's mantle strongly depends on temperature and responds less significantly to pressure changes. Olivine exhibits thermally induced semiconduction under upper mantle conditions; if pressure and temperature exceed ~ 14GPa and 1400C, the phase transition olivine into spinel will further enhance the conductivity due to structural changes from orthorhombic into cubic symmetry. The thermodynamic parameters (temperature, pressure) and oxygen fugacity control the formation, number and mobility of charge carriers. The conductivity temperature relation follows an Arrhenius behaviour, while oxygen fugacity controls the oxidation state of iron and thus the number of electrons acting as additional charge carriers. In volcanic areas rock conductivities may be enhanced by the formation of partial melts under the restriction that the molten phase is interconnected. These four charge transport mechanisms must be considered for the interpretation of geophysical field and borehole data. Laboratory data provide a reproducible and reliable database of electrical properties of homogenous mineral phases and heterogenous rock samples. The outcome of geoelectric models can thus be enhanced significantly. This review focuses on a compilation of fairly new advances in experimental laboratory work together with their explanation.}, added-at = {2009-10-01T14:25:03.000+0200}, author = {Nover, Georg}, biburl = {https://www.bibsonomy.org/bibtex/29680e43f70ff62bbf35c9082b5cdc7a4/aglinda}, description = {IngentaConnect Electrical Properties of Crustal and Mantle Rocks A Review of Lab...}, doi = {doi:10.1007/s10712-005-1759-6}, interhash = {68f63be9650b4364387491e71515af71}, intrahash = {9680e43f70ff62bbf35c9082b5cdc7a4}, journal = {Surveys in Geophysics}, keywords = {2005 cru crustal electrical-conductivity explanation laboratory measurements properties review}, pages = {593-651(59)}, timestamp = {2009-10-01T14:26:03.000+0200}, title = {Electrical Properties of Crustal and Mantle Rocks A Review of Laboratory Measurements and their Explanation}, url = {http://www.ingentaconnect.com/content/klu/geop/2005/00000026/00000005/00001759}, volume = 26, year = 2005 }