P. Schmoldt, PhD - MTNet - DIAS
P. Schmoldt, PhD - MTNet - DIAS P. Schmoldt, PhD - MTNet - DIAS
5. Earth’s properties observable with magnetotellurics Fig. 5.7.: Age of the oceanic plates, from 0 (red) to 280 Ma (violet); from Mueller et al. [2008]. exhibits a relatively small response in comparison with other factors, e.g. water content (cf. Sec. 5.1). The crust is commonly subdivided into continental and oceanic crust, accounting for the difference in composition (examined in the next paragraphs). Continental crust is usually thicker and older than oceanic crust, because oceanic crust is constantly recycled between mid-ocean-ridges (MOR) and subduction zones and rarely gets older than 280 million years (cf. Fig. 5.7). The composition of the crust The Earth’s continental crust contains a high amount of silica and aluminium and possesses a more felsic (or granitic) composition, in contrast to the more mafic (or basaltic) oceanic crust possessing a higher proportion of magnesium and calcium [Rudnick and Gao, 2003] (cf. Tab. 5.2). Close to the surface, both types of crust comprise a high amount of porous rocks, for which the measured electric conductivity is a combination of host matrix and contained fluid content (cf. Sec. 5.1.1). In situ EM investigation, barring marine experiments, that deal with structures at crustal depth are in most cases dominated by electrolytic conduction of fluids in a porous medium. Furthermore, fluids not only affect the bulk conductivity of a region through its inherent electrolytic conduction, but also by facilitating enhanced heat transport, e.g. through circulation of fluids along fault planes Pous et al. [1999]. Besides electrolytic conduction of fluids, electronic conduction in ore bodies and graphite or sulphide bearing oxides (Sec. 5.1.2) is of major importance for the conductivity at 90
Compound Formula 5.2. Variation of electric conductivity with depth Whole crust Oceanic Continental (A) (B) (C) (D) (E) (F) Silica SiO2 59.71 47.8 63.3 58.0 57.3 60.6 Alumina Al2O3 15.41 12.1 16.0 18.0 15.9 15.9 Lime CaO 4.90 11.2 4.1 7.5 7.4 6.4 Magnesia MgO 4.36 17.8 2.2 3.5 5.3 4.7 Sodium oxide Na20 3.55 1.31 3.5 3.7 3.1 3.1 Iron(II) oxide FeO 3.52 9.0 7.5 3.5 9.1 6.7 Potassium oxide K2O 2.80 0.03 1.5 2.9 1.1 1.8 Iron(III) oxide Fe2O3 2.63 - - 1.5 - - Water H2O 1.52 1.0 - 0.9 - - Titanium dioxide TiO2 0.60 0.59 0.8 0.6 0.9 0.7 Phosphorus pentoxide P2O5 0.22 - - - - 0.1 Manganese oxide MnO - - 0.14 - - - Tab. 5.2.: Models of the Earth’s crust bulk composition, in weight-percent (major elements >0.01%). A: [Clarke, 1889]; B: [Elthon, 1979], C: [Condie, 1982], D: [Taylor and McLennan, 1985] (Andesite model), E: [Taylor and McLennan, 1985] (Theoretical model) in Anderson [2004], F: Rudnick and Gao [2003]. crustal depth. Massive ore bodies and interconnected sulphide and graphite phases in shear zones can result in a vast increase of local conductivity at crustal depth, e.g. a conductivity of approximately 2 – 5 S/m is inferred for the North American Central Plains conductivity anomaly (NACP) [Jones and Craven, 1990] and conductivities of less then 1 Ωm are inferred by Korja et al. [1996] for the Lapland Granulite Belt. As for fluid phases in rock matrices, extension and connectivity of the conducting phase in an ore body is a fundamental factor (cf. Fig. 3.5). The effect of pressure on the conductivity of the Earth’s crust, in the absence of temperature changes, is mainly due to resulting changes in connectivity of a good conductor in its host medium, namely (i) closing fractures, (ii) changing the geometry of dry and fluid saturated porous media, or (iii) connecting areas with a high content of water or metal [e.g. Brace et al., 1965; Duba, 1976; Shankland et al., 1997; Wanamaker and Kohlstedt, 1991]. Such effects are highly dependent on the configuration of the composite structure and therefore extremely non-linear and localised. 5.2.2. The Earth’s mantle The Earth’s mantle describes the zone between the Moho and core–mantle boundary (CMB) at approximately 2890 km, which is further divided into upper mantle, mantle transition zone (MTZ), and lower mantle according to their chemical and rheological properties. Moreover, the upper mantle is commonly subdivided by the so-called lithosphere–asthenosphere boundary (LAB) into a lithospheric part (also referred to as uppermost mantle) and an asthenospheric part, referring to the rheological strong and weak layers, respectively. Except for extraordinary regions like MOR’s, the LAB is situated in 91
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Compound Formula<br />
5.2. Variation of electric conductivity with depth<br />
Whole crust Oceanic Continental<br />
(A) (B) (C) (D) (E) (F)<br />
Silica SiO2 59.71 47.8 63.3 58.0 57.3 60.6<br />
Alumina Al2O3 15.41 12.1 16.0 18.0 15.9 15.9<br />
Lime CaO 4.90 11.2 4.1 7.5 7.4 6.4<br />
Magnesia MgO 4.36 17.8 2.2 3.5 5.3 4.7<br />
Sodium oxide Na20 3.55 1.31 3.5 3.7 3.1 3.1<br />
Iron(II) oxide FeO 3.52 9.0 7.5 3.5 9.1 6.7<br />
Potassium oxide K2O 2.80 0.03 1.5 2.9 1.1 1.8<br />
Iron(III) oxide Fe2O3 2.63 - - 1.5 - -<br />
Water H2O 1.52 1.0 - 0.9 - -<br />
Titanium dioxide TiO2 0.60 0.59 0.8 0.6 0.9 0.7<br />
Phosphorus pentoxide P2O5 0.22 - - - - 0.1<br />
Manganese oxide MnO - - 0.14 - - -<br />
Tab. 5.2.: Models of the Earth’s crust bulk composition, in weight-percent (major elements >0.01%). A: [Clarke, 1889]; B: [Elthon,<br />
1979], C: [Condie, 1982], D: [Taylor and McLennan, 1985] (Andesite model), E: [Taylor and McLennan, 1985] (Theoretical model)<br />
in Anderson [2004], F: Rudnick and Gao [2003].<br />
crustal depth. Massive ore bodies and interconnected sulphide and graphite phases in<br />
shear zones can result in a vast increase of local conductivity at crustal depth, e.g. a conductivity<br />
of approximately 2 – 5 S/m is inferred for the North American Central Plains<br />
conductivity anomaly (NACP) [Jones and Craven, 1990] and conductivities of less then<br />
1 Ωm are inferred by Korja et al. [1996] for the Lapland Granulite Belt. As for fluid phases<br />
in rock matrices, extension and connectivity of the conducting phase in an ore body is a<br />
fundamental factor (cf. Fig. 3.5). The effect of pressure on the conductivity of the Earth’s<br />
crust, in the absence of temperature changes, is mainly due to resulting changes in connectivity<br />
of a good conductor in its host medium, namely (i) closing fractures, (ii) changing<br />
the geometry of dry and fluid saturated porous media, or (iii) connecting areas with a high<br />
content of water or metal [e.g. Brace et al., 1965; Duba, 1976; Shankland et al., 1997;<br />
Wanamaker and Kohlstedt, 1991]. Such effects are highly dependent on the configuration<br />
of the composite structure and therefore extremely non-linear and localised.<br />
5.2.2. The Earth’s mantle<br />
The Earth’s mantle describes the zone between the Moho and core–mantle boundary<br />
(CMB) at approximately 2890 km, which is further divided into upper mantle, mantle<br />
transition zone (MTZ), and lower mantle according to their chemical and rheological<br />
properties. Moreover, the upper mantle is commonly subdivided by the so-called<br />
lithosphere–asthenosphere boundary (LAB) into a lithospheric part (also referred to as uppermost<br />
mantle) and an asthenospheric part, referring to the rheological strong and weak<br />
layers, respectively. Except for extraordinary regions like MOR’s, the LAB is situated in<br />
91