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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 />

!

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