Dynamic Behavior of a Nonisothermal Chemical System
 The following nonisothermal reaction system is theoretical. The steps are as follows: Here  is a chemical precursor with constant concentration,  is the final product,  and  are intermediate chemical species,  ,  and  are rate constants for the reactions, and  ,  , and  are the concentrations of the hypothetical chemical species  ,  , and  . The autocatalytic reaction is the following step:  , with  catalyzing its own formation. This step introduces the nonlinear term  in the governing equations. The last reaction, B → C + Heat is exothermic. The rate constant of the first reaction, P → A, follows the Arrhenius rate-law. Thus  depends on the temperature. The governing equations for the two intermediate species and the temperature are usually written in the form: The dimensionless governing equations are:  ,  ,  . Here  ,  , and  are dimensionless concentrations of  ,  , and the dimensionless temperature, and the four parameters  ,  ,  , and  depend on the rate constants of the individual reactions  ,  ,  , and  , the concentration of the precursor  , the molar density  , the molar heat capacity  , the surface heat transfer coefficient  , the surface area  , the surrounding temperature  , the heat of reaction  for the reaction , and the activation energy  of the reaction  . The Demonstration illustrates the dynamics of the concentrations  ,  , and the temperature  for various values of the bifurcation parameter  . Choose "time series" to get a plot of  versus time or "phase space" to get a three-dimensional parametric plot of  . For  = 0.5586, the  phase-space graph is that of a spiral attractor. Reference: S. K. Scott and A. S. Tomlin, "Period Doubling and Other Complex Bifurcations in Non-isothermal Chemical Systems," Philosophical Transactions of the Royal Society of London, Series A: Mathematical and Physical Sciences, 332(1624), 1990 pp. 51–68.
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