P. Schmoldt, PhD - MTNet - DIAS
P. Schmoldt, PhD - MTNet - DIAS P. Schmoldt, PhD - MTNet - DIAS
2. Sources for magnetotelluric recording Fig. 2.4.: Layers of the ionosphere with their electron density and predominant ion populations; from Andersen and Fuller-Rowell [1999]. Solar cycle variation Regular solar variations are connected with wave radiation of the Sun with the fundamental period for the solar cycle variations of 11 years [Schmucker, 1985], most easily observed by the annual number of sunspots (Fig. 2.5). Even though the cause of the cycle is not yet fully understood, changes in activity can be used to predict the observable signal strength during a fieldwork campaign as the increased magnetic activity intensifies pre-existing current systems used as MT sources [Mareschal, 1986]. Presently we are situated in an elongated minimum of the twenty third 11 year cycle (Fig. 2.6) causing the signal, and hence the signal-to-noise ratio (SNR), to be noticeably lower at mid-latitudes. Moreover, the decreasing maximum field strength of annual sunspots, as observed by Livingston and Penn [2009] using measured infrared intensity in the darkest position of the sunspot umbrae, is raising the question of whether we are actually experiencing a new period of severely reduced activity, similar to the Maunder Minimum from 1675 to 1715 AD [Luterbacher et al., 2001]. The present time frame, limited by the emergence of the required instruments, is too short to verify such hypothesis. (Semi-)Annual variation Annual and semi-annual variations penetrate into the Earth down to a depth of approximately 1000 km and deeper but are commonly not used for MT investigation due to the required extensive recording time. Furthermore, semi-annual variations exhibit very 12
2.2. Electric currents in the magnetosphere Fig. 2.5.: Monthly average of observed sunspot numbers since 1749 (in blue) and the more sporadic observations prior to 1749 (in red) until 2001, exhibiting a prominent 11 year cycle and periods of altered activity, after Hoyt and Schatten [1998a,b]. Fig. 2.6.: Monthly (blue) and monthly smoothed (red) sunspot numbers since 1950 until 2010 showing a minimum of solar activity for the time of the fieldwork campaign in 2007, from Solar Influence Data Analysis Center (SIDC), Royal Observatory of Belgium [2010] small amplitudes, which makes the response estimation very difficult given the insufficient baseline stability of electric sensor systems for such a long duration. Special setups are necessary to utilise semi-annual variation signal, e.g. the experiment by Schultz et al. [1993] in which electric recording instruments (electrodes) were placed in lakes for thermal and chemical stability. 2.2.2. Regular variations Regular variations terms effects that occur constantly but are variable in intensity, depending on the present strength of the solar activity and the resulting solar wind. 13
- Page 1: Multidimensional isotropic and anis
- Page 4 and 5: Contents 2.3. Deviation from plane
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- Page 9 and 10: List of Figures 2.1. Amplitude of t
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- Page 17: List of Figures A.15.Result of anis
- Page 20 and 21: List of Tables xviii 5.5. Parameter
- Page 22 and 23: List of Acronyms FE finite element
- Page 25 and 26: List of Symbols Below is a list of
- Page 27 and 28: Symbol SI unit Denotation φ · pha
- Page 29: Abstract The Tajo Basin and Betic C
- Page 32 and 33: Publications Poster presentations x
- Page 34 and 35: Acknowledgements Team, namely Colin
- Page 37 and 38: Introduction 1 The Iberian Peninsul
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- Page 41: Part I Theoretical background of ma
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2. Sources for magnetotelluric recording<br />
Fig. 2.4.: Layers of the ionosphere with their electron density and predominant ion populations; from Andersen and Fuller-Rowell<br />
[1999].<br />
Solar cycle variation<br />
Regular solar variations are connected with wave radiation of the Sun with the fundamental<br />
period for the solar cycle variations of 11 years [Schmucker, 1985], most easily<br />
observed by the annual number of sunspots (Fig. 2.5). Even though the cause of the cycle<br />
is not yet fully understood, changes in activity can be used to predict the observable<br />
signal strength during a fieldwork campaign as the increased magnetic activity intensifies<br />
pre-existing current systems used as MT sources [Mareschal, 1986]. Presently we are<br />
situated in an elongated minimum of the twenty third 11 year cycle (Fig. 2.6) causing the<br />
signal, and hence the signal-to-noise ratio (SNR), to be noticeably lower at mid-latitudes.<br />
Moreover, the decreasing maximum field strength of annual sunspots, as observed by<br />
Livingston and Penn [2009] using measured infrared intensity in the darkest position of<br />
the sunspot umbrae, is raising the question of whether we are actually experiencing a<br />
new period of severely reduced activity, similar to the Maunder Minimum from 1675 to<br />
1715 AD [Luterbacher et al., 2001]. The present time frame, limited by the emergence of<br />
the required instruments, is too short to verify such hypothesis.<br />
(Semi-)Annual variation<br />
Annual and semi-annual variations penetrate into the Earth down to a depth of approximately<br />
1000 km and deeper but are commonly not used for MT investigation due to<br />
the required extensive recording time. Furthermore, semi-annual variations exhibit very<br />
12