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P. Schmoldt, PhD - MTNet - DIAS

P. Schmoldt, PhD - MTNet - DIAS

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2. Sources for magnetotelluric recording<br />

Fig. 2.10.: Top: possible interaction between field-aligned currents with convection electrojets and cross-polar cap current flow the<br />

sunlit polar ionosphere; from [Zanetti et al., 1983]. Bottom: Schematic representation of a substorm current system intrusion into<br />

the convection electrojets system for a dark ionosphere (left) causing vibrations of the Hall current system (right) represents fieldaligned<br />

currents into the ionosphere, out of it; from Mareschal [1986].<br />

Polar electrojets<br />

The exact mechanisms of current flow in the Polar Regions are not yet fully understood,<br />

but different models have been presented in order to explain certain aspects of the present<br />

current system: e.g. Birkeland and Pedersen field align currents generating Hall currents<br />

in the polar region that flow towards the Harang discontinuity at local midnight [e.g. Kisabeth<br />

and Rostoker, 1977; Rostoker et al., 1982; Baumjohann, 1983; Zanetti et al., 1983]<br />

(Fig. 2.10). As polar electrojets (PEJ) are an important contributor to local polar MT<br />

signals, a great deal of effort has been spent on investigating their characteristics in terms<br />

of height above the surface, length and the related pulsation structure, e.g. Walker and<br />

Greenwald [1981]; Andre and Baumjohann [1982]; Baumjohann [1983]; Pirjola [1998].<br />

This led to the conclusion that the PEJ is usually constrained to a height of 100 – 120 km<br />

16

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