Schmucker-Weidelt Lecture Notes, Aarhus, 1975 - MTNet
Schmucker-Weidelt Lecture Notes, Aarhus, 1975 - MTNet
Schmucker-Weidelt Lecture Notes, Aarhus, 1975 - MTNet
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that the upper mantle beneath oceans is hotter than the mantle<br />
beneath continents down to a depth of a few hundred kilometers.<br />
If this is so, a corresphndingly higher conductivity should exist<br />
beneath oceans which could be recognised from a reduced depth<br />
of penetration in comparison to continents. Once a characteristic<br />
conductivity difference between an oceanic and a. continental<br />
substructure has been established, this could be used tb recog-<br />
nize former oceanic mantle material beneath present-day con-<br />
tinents and vice versa.<br />
First houndings with recording instruments at the bottom of the<br />
sea have been carrred out. They confirmed to some extent the<br />
expectation of h'igh conductivities at extremely shallow depth,<br />
but these punctual soundings may not be representative for the<br />
oceans as a whole. Here the development of new experimental<br />
techniques for expedient seafloor operations of magnetic and<br />
geolectric instruments has. to be awaited.<br />
~~sarvatioAs,on. . mid-oceanic islands provide a less expensive<br />
way to study the induction in the oceans which in he case of<br />
substorms and Sq is strongly coupled to the crustal and subthe<br />
ocea s<br />
crustal conductivities beneath . Buf again oceanic islands<br />
are usually volcanic and their substructure may differ from that<br />
of ordinary parts of ocean basins.<br />
The island-effect itself is no obstacle fo$ soundings into the<br />
deep structure. In fact, this effect represents a powerful tool<br />
to investigate the inductive response in the surrounding open<br />
'ocean, since the.theoretica1 distortion of the varia-tion fields<br />
due to the islands can be regarded at sufficiently Low frequency<br />
as a direct current problem for a given pattern of oceanic in-<br />
duction currents at some distance from the island. Setting the<br />
. ..<br />
.density of these currents in relation to the observed magnetic<br />
field on the island gives the impedance of the variation field<br />
, for the surrounding oceari of known integrated conductivity. To a<br />
first approximation induced currents in the ocean do not contribute<br />
to the horizontal magnetic field on the island. Hence, by<br />
knowing their density the horizontal magnetic field on the sea<br />
s<br />
I<br />
i<br />
I:<br />
floor can be calculated from which the inductive response function<br />
for the oceanic substructure follows.<br />
j<br />
!