Schmucker, 1970 (Scripps) - MTNet
Schmucker, 1970 (Scripps) - MTNet
Schmucker, 1970 (Scripps) - MTNet
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2 Bulletin, <strong>Scripps</strong> Institution of Oceanography<br />
At first sight the electrical conductivity 0" of subterranean matter may not<br />
seem to be a very noteworthy parameter. There is, however, its close relation<br />
to temperature, following the general theory of semiconduction, and<br />
even a relatively small rise in ambient temperature may cause a substantial<br />
increase of the conductivity (sec. 1.4). We have to bear in mind, however,<br />
that semiconduction in nonmetallic solids is primarily an impurity effect.<br />
Thus, minute changes of composition can have an equally strong effect upon<br />
0", not counting the largely unknown influence of pressure.<br />
This limits the effective use of the conductivity as an absolute thermometer<br />
for the earth's interior. There remains, however, the important aspect<br />
to use 0" as relative thermometer, namely, to infer deep-seated lateral gradients<br />
of conductivity and possibly temperature from their distorting effect<br />
upon the internal part of geomagnetic variations. Such thermal imbalances in<br />
the upper mantle could be connected with ascending and descending branches<br />
of convection cells or with local concentrations of radioactive heat sources,<br />
which may be the underlying cause for the diversified tectonic and magmatic<br />
history of the earth's outermost layers.<br />
Two inherent limitations of geomagnetic depth sounding should be mentioned.<br />
Since the magnetic observations are made within a small area, small<br />
in comparison to the spatial extent of the primary inducing field from above,<br />
a complete separation of internal and external parts of the transient variation<br />
field is not possible. A separation of this kind would be necessary to determine<br />
the overall change of conductivity with depth in the surveyed area (sec.<br />
1. 3). Hence, induction anomalies of the internal part, which are recognized<br />
usually without formal separation of internal and external parts, have to be<br />
interpreted on the basis of a preconceived mean conductivity distribution<br />
which has been inferred as function of depth from other sources of information<br />
(sec. 1. 3).<br />
Second, oceans and continental surface layers form a thin conducting cover<br />
of great complexity. The flow of shallow eddy. currents is therefore highly<br />
distorted, in particular near coastlines because of the outstanding conductivity<br />
contrast of seawater and rock formations on land. This mayor may not<br />
lead to an anomalous behavior of geomagnetic variations, depending on the<br />
relative strength of those eddy currents and their contribution to the internal<br />
part in the area under consideration. Surface effects of this kind have to be<br />
taken into account before postulating a deep-seated cause for a given induction<br />
anomaly.<br />
1.2 Basic Equations<br />
The incident variation field diffuses downward through the conducting layers<br />
of the earth with amplitude reduction and phase rotation. The governing<br />
equations are Maxwell's field equations of the transient electromagnetic vector<br />
field E and F. We use here their quasi-stationary approximation (in<br />
emu):<br />
curl.F :; 417O"E and curl £= -MoFfat (1.1)<br />
I<br />
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