The Sun continually emits mass, momentum, and energy in the form of magnetized and ionized plasma from its outermost layer known as the solar wind (Hundhausen, 2012). The variation in energy content is closely related to the solar cycle. During the minimum activity phase, the predominant solar structures are the coronal holes (CH), from where the fast solar wind streams continuously emanate (Schwenn, 2006;Gosling, 1997; Gosling et al., 1976, and references therein). The interaction of ambient solar wind and fast solar wind forms the regions known as co-rotating interaction regions or CIR's (Alves et al., 2006;Smith & Wolfe, 1976). During the maximum solar activity phase, the predominant large-scale solar structures are the sunspots and active regions, where continuous magnetic reconfigurations release a large amount of magnetized plasma into the interplanetary space known as Coronal Mass Ejections (CME). A subclass of CMEs identified in the interplanetary medium is the magnetic clouds (MC) (Burlaga & Burlaga, 1995;Burlaga et al., 1998) An important characteristic of MC concerns its signature observed by the satellite when crossing the flux tube magnetic structure, which can be seen as an intense magnetic field with smooth rotation and low plasma beta value, also being able to be defined as a force-free structure having cylindrical symmetry (see, Kilpua et al., 2017;Goldstein, 1983, for more details). These MC-type solar and interplanetary structures in comparison to structures that are predominant in the minimum of solar activity can intensely and abruptly affect the magnetosphere-ionosphere system and upper atmosphere if they have a southward-directed interplanetary magnetic field (IMF) component through magnetic reconnection (Dungey, 1961). The primary evidence of the abrupt penetration of mass, momentum, energy, and magnetic flux into the inner regions of the magnetosphere is the emergence of magnetic storms and substorms (Chapman & Ferraro, 1933;Gonzalez et al., 1994), together with global perturbations in the particle flux which make up the ring current (RC) and the Radiation Belts (RB) that are highly influenced by the occurrence of