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P. Schmoldt, PhD - MTNet - DIAS

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2.2. Electric currents in the magnetosphere<br />

Fig. 2.2.: Annual rate of lightning discharges, indicated by colours; from Global Hydrology Resource Center [2010].<br />

field of thunderstorms in order to assure that the plane wave assumption is satisfied (cf.<br />

Sec. 2.3).<br />

2.2. Electric currents in the magnetosphere<br />

The Earth’s magnetosphere is the region in which behaviour of charged particles is dominated<br />

by the Earth’s internal magnetic field, with the resulting shape determined by interaction<br />

with the electromagnetic components of the solar wind compressing it on the<br />

dayside and causing an elongated tail on the night side (Fig. 2.3). The lowermost part<br />

of the magnetosphere, extending from around 50 km to 1000 km above Earth’s surface,<br />

is the relatively conductive ionosphere. The ionosphere consists of plasma and contains<br />

mostly oxygen and nitrogen gases, ionised by solar radiation [Kelley, 1989; Vozoff , 1987;<br />

Andersen and Fuller-Rowell, 1999] (Fig. 2.4).<br />

Through the interaction of the solar wind, containing charged particles and plasma,<br />

with elements of the Earth’s magnetosphere, various EM fields are generated, forming<br />

the lower end of the MT source spectrum. The strength of generated EM fields are in<br />

the range < 0.1 nT, for frequencies in the region of 1 s, and increases with period until it<br />

reaches a quasi-steady level of around 3 nT, for periods greater than 10 5 s. Superimposed<br />

on this is a multitude of spectral peaks with varying amplitude and sharpness (Fig. 2.1).<br />

A list of the contributing signals together with their characteristics and sources is given in<br />

Table 2.1 and a detailed description is given in Sections 2.2.1 to 2.2.5.<br />

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