Geomagnetic storms occur when solar activity increases and solar wind interacts with the Earth's magnetic field. This interaction can result in rapid changes in the geomagnetic field and induce geoelectric fields at the Earth's surface and interior, according to Faraday's law of electromagnetic (EM) induction. The geoelectric fields drive currents in the ground through power systems, pipelines, and other electrically earthed technological systems. The frequency of the current is substantially lower than the operational frequency of electric power transmission grids; therefore, it is considered quasi-direct current (DC) and is commonly known as geomagnetically induced current (GIC; e.g., Boteler, 1994;Pirjola, 2000). GICs can cause substantial damage to pipelines through increased corrosion and can affect power networks through premature aging of transformers (Pirjola et al., 2000).Larger GICs (100 to −500 A, Viljanen et al., 2013) observed at high latitudes have been attributed to amplification by intense ionospheric current systems in the vicinity of auroral ovals (Pirjola, 2000). However, as a result of the Abstract Geomagnetically induced currents (GICs) result from the interaction of the time variation of ground magnetic field during a geomagnetic disturbance with the Earth's deep electrical resistivity structure. In this study, we simulate induced GICs in a hypothetical representation of a low-latitude power transmission network located mainly over the large Paleozoic Paraná basin (PB) in southern Brazil. Two intense geomagnetic storms in June and December 2015 are chosen and geoelectric fields are calculated by convolving a three-dimensional (3-D) Earth resistivity model with recorded geomagnetic variations. The dB/dt proxy often used to characterize GIC activity fails during the June storm mainly due to the relationship of the instantaneous geoelectric field to previous magnetic field values. Precise resistances of network components are unknown, so assumptions are made for calculating GIC flows from the derived geoelectric field. The largest GICs are modeled in regions of low conductance in the 3-D resistivity model, concentrated in an isolated substation at the northern edge of the network and in a cluster of substations in its central part where the east-west (E-W) oriented transmission lines coincide with the orientation of the instantaneous geoelectric field. The maximum magnitude of the modeled GIC was obtained during the main phase of the June storm, modeled at a northern substation, while the lowest magnitudes were found over prominent crustal anomalies along the PB axis and bordering the continental margin. The simulation results will be used to prospect the optimal substations for installation of GIC monitoring equipment.
Plain Language SummaryThe Sun is a source of explosive space weather events in which large amounts of radiation and atomic particles are released in short periods of time. When these bursts of energy impact the Earth's environment, electrical current systems in the magnetosphere...