“…One description in particular (Duncan, 1983), based on an average model of the non-saturated LIM, and later expanded to include saturation (Woronowicz and Safaee, 2014), has been adopted by authors developing LIM control algorithms (Woronowicz and Palka, 2002; Woronowicz and Palka, 2003). The established analytical models of the LIM typically express the excitation currents in the primary coils as infinitely thin current sheet (Nasar and Boldea, 1976; Yamamura, 1979; Freeman and Lowther, 1973; Mosebach et al , 1977; Pierson et al , 1977; Freeman and Papageorgiou, 1978; Gieras et al , 1985; Gieras et al , 1986; Mendrela and Gierczak, 1982). However, in recent decades, LIM modeling and analysis started relying more on finite element analysis (FEA) simulations, such as in studies by Lee et al (2009); Shiri and Shoulaie (2012); Singh et al (2013); Amiri and Mendrela (2014); Abdollahi et al (2015); Jeong et al (2015), instead of analytical solutions.…”