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P. Schmoldt, PhD - MTNet - DIAS

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Tab. 2.1 – Continued<br />

2.2. Electric currents in the magnetosphere<br />

Type Symbol τ A (nT) Source<br />

Polar magnetic storms and short-lived substorms Polar (or auroral)<br />

centre of disturbance in<br />

the night-time auroral<br />

zone<br />

with correlated irregular<br />

variations in low latitudes<br />

DP1 10 m - 2 h<br />

DP2 10 m - 2 h<br />

Special effects in connection to polar magnetic storms<br />

bays (substorms as<br />

observed in mid latitudes)<br />

b 30 m -2 h<br />

Sudden storm commencement<br />

1000 (a)<br />

100 (m,l)<br />

100 (a)<br />

10 (m,l)<br />

100 (d,d)<br />

20 - 100 (a,m)<br />

5 - 25 (l)<br />

electrojet PEJ in the<br />

ionosphere with<br />

connecting field-aligned<br />

currents to plasma regions<br />

of the magnetosphere<br />

see DP1<br />

ssc 2 - 5 m 10 - 100 m Impact of intense solar<br />

particle stream on magnetopause<br />

Solar flare effect sfe 10 - 20 m 10 Short-lived enhancement<br />

of Sq currents in the<br />

ionosphere<br />

Ultralow frequency waves<br />

(Pulsations)<br />

regular continuous<br />

pulsations<br />

irregular transient<br />

pulsations<br />

Very low frequency emissions,<br />

including whistlers<br />

ULF (P) 0.2 - 600 s<br />

Pc5 150 - 600 s<br />

100 (a)<br />

10 (m)<br />

Pc4 45 - 150 s 2<br />

Pc3 10 - 45 s 0.5<br />

Pc3 5 - 10 s 0.5<br />

Pc1 0.2 - 5 s 1<br />

Pi2 45 - 150 s 1<br />

Pi1 1 - 45 s 1<br />

VLF 10 −5 − 10 −3 s<br />

2.2.1. Ultralong periodic variation<br />

Standing and propagating<br />

hydromagnetic waves in<br />

the magnetosphere<br />

In this Section geomagnetic variations with extremely long periods are examined that are<br />

not directly related to conventional MT measurements, which are, for logistic reason, usually<br />

limited to a duration of a few months or less. Signals of such ultralong variations are<br />

more suitable for studies using magnetovariational (MV) datasets, recorded at stationary<br />

observatories that provide time series of sufficient length. However, the results of those<br />

MV studies can be used to compare findings of MT methods and help to predict structures<br />

at greater depth, which in turn can aid interpretation of MT studies.<br />

a Schmucker [1985] assigns the Lunar daily variations to have a fundamental period of 1 d but as the<br />

determining value is the time that it takes the Moon to orbit the Earth this variation has a period of<br />

around 24 h 50 m (1 lunar day) instead, e.g. Merrill and McElhinny [1983], p.53; National Oceanic and<br />

Atmospheric Administration (NOAA) [2010].<br />

11

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