“…Thus, (1) can be regarded as the fractional analogue of equation of motion. In case we fix p = α, q = β, f (t, x(t)) = (R Z /L)x(t), f (t, x(t)) = (1/LC)[−x(t) + e(t)], (1) takes the form of a fractional-order differential equation of the voltage function x(t), see Equation (4) in [2]. The nonlocal conditions involved in the problem (1) appear in several applications of diffusion processes, computational fluid dynamics (CFD) studies of blood flow problems, bacterial self-regularization models, for instance, see [3][4][5].…”