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

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PP-II-3exist around <strong>the</strong> steady state – a stable and an unstable ones. If a steady state is located farfrom <strong>the</strong> borders <strong>of</strong> <strong>the</strong> unstable part <strong>of</strong> <strong>the</strong> <strong>the</strong>rmal isoclinal line, so s<strong>of</strong>t birth <strong>of</strong> selfoscillations(limit cycle) takes place. In this case <strong>the</strong> amplitude <strong>of</strong> self-oscillations is growingsmoothly. The solution <strong>of</strong> <strong>the</strong> non-steady problem has confirmed <strong>the</strong> detected mechanisms <strong>of</strong><strong>the</strong> birth/death <strong>of</strong> self-oscillations.Consecutive reactions. For CSTR with a two-step consecutive reaction (both stagesbeing exo<strong>the</strong>rmal first-order processes), analysis <strong>of</strong> <strong>the</strong> multiplicity <strong>of</strong> <strong>the</strong> steady states and<strong>the</strong> mechanism <strong>of</strong> birth/death <strong>of</strong> self-oscillations have been carried out. A region <strong>of</strong> fivesteady states was discovered for <strong>the</strong> first time. Its evolution with <strong>the</strong> change <strong>of</strong> <strong>the</strong> ratio <strong>of</strong> <strong>the</strong>activation energy <strong>of</strong> <strong>the</strong> first stage to that <strong>of</strong> <strong>the</strong> second stage has been investigated. It wasshown that this region arises within <strong>the</strong> region <strong>of</strong> three steady states. With <strong>the</strong> growth <strong>of</strong> <strong>the</strong>above ratio, it is elongated and partly oversteps <strong>the</strong> limits <strong>of</strong> <strong>the</strong> region <strong>of</strong> three steady states.This part <strong>of</strong> <strong>the</strong> domain contains just only three stationary states.For a definite set <strong>of</strong> kinetic parameters in <strong>the</strong> parametric space Semenov criterion –Damköhler criterion, a region <strong>of</strong> <strong>the</strong> existence <strong>of</strong> self-oscillations was found. For <strong>the</strong> region<strong>of</strong> one steady state, it was shown that at <strong>the</strong> lower border <strong>of</strong> <strong>the</strong> self-oscillation region (smallvalues <strong>of</strong> Semenov parameter) <strong>the</strong>ir birth occurs by a s<strong>of</strong>t way. The steady state becomesunstable and gives rise to a stable limit cycle. At <strong>the</strong> upper border <strong>of</strong> <strong>the</strong> self-oscillationregion (large values <strong>of</strong> Semenov parameter), stiff death <strong>of</strong> self-oscillations takes place: astable limit cycle is joined with an unstable limit cycle. The unstable limit cycle arises at <strong>the</strong>change <strong>of</strong> <strong>the</strong> steady state stability.For <strong>the</strong> region <strong>of</strong> three steady states it was demonstrated that at lower border <strong>of</strong> <strong>the</strong> selfoscillationregion, <strong>the</strong> oscillation arise by a stiff way, by <strong>the</strong> mechanism <strong>of</strong> a loop formation.This work was supported by <strong>the</strong> <strong>Russian</strong> Foundation <strong>of</strong> Fundamental Researches, <strong>the</strong>grant No. 06–03–32053–a.Reference1. D.A. Vaganov, N.G. Samoilenko, V.G. Abramov, Periodic Regimes <strong>of</strong> Continuous Stirred Tank Reactors,Chem. Eng. Science, Vol. 33, pp. 1133-1140 (1978).278

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