Modern research in the area of deterministic chaotic systems [1] is oriented on acquiring control of this apparently uncontrollable regime. An outline characteristics of the control of chaos was given in Sect. 1.10.3 of volume I. The reader particularly interested in this area can consult, e.g., a recent specialized monograph on that subject [2]. Two landmark papers on the chaos control appeared in 1990. In one of them Ott et al. [3] have described the (OGY) algorithm of converting a chaotic (strange) attractor to any one of a large number of possible attracting time-periodic motions by making only small time-dependent perturbations of an available system parameter. In other words, by applying the appropriate feedback-based strategy one can suppress chaos by maintaining the system's dynamics on a selected, desired periodic phase trajectory. In the second paper, written by Pecora and Carroll [4], it was shown that certain subsystems of nonlinear, chaotic systems can be made to synchronize by linking them with common signals. These theoretical achievements triggered increasing interest also in achieving the stabilization of any unstable states, both in theoretical models and real systems, including electrochemical processes. Several particular algorithms were employed for such strategies based on appropriate feedbacks.For a highly dissipative system (when the strange attractor has a dimension slightly higher than 2), it is convenient to reduce the original OGY approach to a simple map-based