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Boreskov Institute of Catalysis of the Siberian Branch of Russian ...

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OP-I-9This work is a continuation <strong>of</strong> [2], which was devoted to <strong>the</strong> development <strong>of</strong> a lowdimensionalkinetic model <strong>of</strong> CO oxidation on a metallic catalyst surface and <strong>the</strong> <strong>the</strong>oreticalstudy <strong>of</strong> arising nonlinear phenomena and relaxation oscillations <strong>of</strong> <strong>the</strong> reaction rate. In <strong>the</strong>paper [2], <strong>the</strong> conventional Langmuir-Hinshelwood mechanism <strong>of</strong> catalytic CO oxidation wasconsidered under assumption <strong>of</strong> <strong>the</strong> possibility <strong>of</strong> a metal surface modification in <strong>the</strong> course<strong>of</strong> catalytic reaction due to <strong>the</strong> oxygen penetration into subsurface layers.The rate <strong>of</strong> changing <strong>the</strong> third coordinate z is smaller <strong>the</strong>n <strong>the</strong> rates <strong>of</strong> <strong>the</strong> o<strong>the</strong>r reactionstages, and <strong>the</strong> dynamic properties <strong>of</strong> <strong>the</strong> whole system are inherently determined by <strong>the</strong>structure <strong>of</strong> limit sets <strong>of</strong> <strong>the</strong> one-parameter family <strong>of</strong> submodels with two variables x, y andparameter z. These submodels have a hysteresis <strong>of</strong> steady states and two maximal families <strong>of</strong>periodic solutions at some K i values (i = 1, -1, 2, 3). For each family, <strong>the</strong> periodic solutions atone <strong>of</strong> <strong>the</strong> boundaries degenerate into <strong>the</strong> homoclinic orbit that is a saddle-loop separatrix. Inthis case <strong>the</strong> periodic solutions are highly parametric sensitive. Moreover, <strong>the</strong>re are twoscenarios <strong>of</strong> <strong>the</strong> chaotic dynamics birth in <strong>the</strong> model at some values <strong>of</strong> K 4 and K 5 , namely: bymeans <strong>of</strong> a cascade <strong>of</strong> period-doubling bifurcations and owing to <strong>the</strong> mixed-mode oscillations(see Fig. 1).Figure 1. The examples <strong>of</strong> a strange attractor as a result <strong>of</strong> <strong>the</strong> cascade <strong>of</strong> period-doubling bifurcations (left part)and chaotic oscillations as a result <strong>of</strong> <strong>the</strong> development <strong>of</strong> mixed-mode oscillations (right part)References:1. G.A. Chumakov, M.G. Slinko. Dokl. Akad. Nauk SSSR, 1982, 266, 5, 1194-1198.2. E. Ivanova, N. Chumakova, G. Chumakov, A. Boronin. Chem. Eng. J. 2005, 107, 191-198.43

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