Zhabotinskii-Belousov type oscillatory

The analogous, although considerably less pronounced changes in the respective values, the chromatographic peaks concentration profiles, and the specific rotation ([ckId) values were established by means of polarimetry and TLC with densitometric detection in the case of ibuprofen, naproxen, and 2-phenylpropionic acid, when stored as solutions in dichloromethane and physiological salt [2,3], Finally, we arrived at a conclusion that the true reason for all these oscillatory changes was a spontaneous and oscillatory transenantiomerization of the investigated APA solutions in the spirit of the classical Zhabotinskii-Belousov type oscillatory reactions. 

Recently there has been an increasing interest in self-oscillatory phenomena and also in formation of spatio-temporal structure, accompanied by the rapid development of theory concerning dynamics of such systems under nonlinear, nonequilibrium conditions. The discovery of model chemical reactions to produce self-oscillations and spatio-temporal structures has accelerated the studies on nonlinear dynamics in chemistry. The Belousov-Zhabotinskii(B-Z) reaction is the most famous among such types of oscillatory chemical reactions, and has been studied most frequently during the past couple of decades [1,2]. The B-Z reaction has attracted much interest from scientists with various discipline, because in this reaction, the rhythmic change between oxidation and reduction states can be easily observed in a test tube. As the reproducibility of the amplitude, period and some other experimental measures is rather high under a found condition, the mechanism of the B-Z reaction has been almost fully understood until now. The most important step in the induction of oscillations is the existence of auto-catalytic process in the reaction network. 

As we have already commented, mappings of the type discussed above are not in any way easily related to a given set of reaction rate equations. Such mappings have, however, been used for chemical systems in a slightly different way. A quadratic map has been used to help interpret the oscillatory behaviour observed in the Belousov-Zhabotinskii reaction in a CSTR. There, the variable x is not a concentration but the amplitude of a given oscillation. Thus the map correlates the amplitude of one peak in terms of the amplitude of the previous excursion. 

We have investigated the transitions among the types of oscillations which occur with the Belousov-Zhabotinskii reaction in a CSTR. There is a sequence of well-defined, reproducible oscillatory states with variations of the residence time [5]. Similar transitions can also occur with variation of some other parameter such as temperature or feed concentration. Most of the oscillations are periodic but chaotic behavior has been observed in three reproducible bands. The chaos is an irregular mixture of the periodic oscillations which bound it e.g., between periodic two peak oscillations and periodic three peak oscillations, chaotic behavior can occur which is an irregular mixture of two and three peaks. More recently Roux, Turner et. al. 

A particular type of structure, the leading centres, can be generated either by some small auto-oscillatory regions of the medium or by a special type of sources (echo-sources) arising in a medium with nonoscillatory kinetics. Based on the experimental results of Agladze Krinsky (1984) the first mechanism seems to be more probable for the Belousov-Zhabotinskii-system. 

---