Abstract

This research focuses on the inversion of geomagnetic variation field measurements to obtain the source currents in the ionosphere and magnetosphere, and to determine the geoelectric fields at the Earth’s surface. During geomagnetic storms, the geoelectric fields create geomagnetically induced currents (GIC) in power networks. These GIC may disturb the operation of power systems, cause damage to power transformers, and even result in power blackouts. In this model, line currents running east–west along given latitudes are postulated to exist at a certain height above the Earth’s surface. This physical arrangement results in the fields on the ground being composed of a zero magnetic east component and a nonzero electric east component. The line current parameters are estimated by inverting Fourier integrals (over wavenumber) of elementary geomagnetic fields using the Levenberg–Marquardt technique. The output parameters of the model are the ionospheric current strength and the geoelectric east component at the Earth’s surface. A conductivity profile of the Earth is adapted from a shallow layered-Earth model for one observatory, together with a deep-layer model derived from satellite observations. This profile is used to obtain the ground surface impedance and therefore the reflection coefficient in the integrals. The inputs for the model are a spectrum of the geomagnetic data for 31 May 2013. The output parameters of the model are spectrums of the ionospheric current strength and of the surface geoelectric field. The inverse Fourier transforms of these spectra provide the time variations on the same day. The geoelectric field data can be used as a proxy for GIC in the prediction of GIC for power utilities. The current strength data can assist in the interpretation of upstream solar wind behaviour.

Highlights

  • We found the geographic latitude of the equatorial electrojet (EEJ) at this longitude to be around 8.17°N for Apex(epoch 2013.5) and 8.15°N for International Geomagnetic Reference Field (IGRF)(epoch 2013), by virtue of the fact that the geomagnetic vertical component and inclination must be zero (Bz = 0 nT; BI = 0°) at the EEJ

  • Addis Ababa [95.8 km north of the EEJ] along the geographic meridian and Addis Ababa. This figure is shown as an example for only one sampled frequency (f0) of the spectrum of the Fourier transform of ΔBx(x, ω) and ΔBz(x, ω)

  • If the inversion is repeatedly run using data from all sampled frequencies, the performance is similar to Fig. 6

Read more

Summary

Introduction

Induced currents (GIC) can occur in grounded technical networks, such as electric power transmission grids (Bolduc 2002; Molinski 2002; Kappenman 2003; Pirjola 2005; Pulkkinen et al 2005; Viljanen et al 2012), oil and gas pipelines (Pulkkinen et al 2001; Gummow 2002; Trichtchenko and Boteler 2002), and telecommunication cables and railway circuits (Ptitsyna et al 2008; Wik et al 2009; Eroshenko et al 2010) Solar events, such as geoeffective coronal mass ejections (CME), create disturbances within the Earth’s magnetosphere, which can give rise to geomagnetic storms and substorms.

Methods
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call