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Convective instabilities induced by an exothermic autocatalytic chemical reaction
Phys. Rev. E 52, 1606 – Published 1 August, 1995
DOI: https://doi.org/10.1103/PhysRevE.52.1606
Abstract
A bistable or excitable exothermic chemical reaction can produce a traveling front of chemical reactivity upon being triggered. The dynamics of the wave propagation are greatly influenced by the amount of heat generated at the wave front, which in turn is a function of (nonlinear) reaction kinetics, enthalpy change, and extent of reaction. The chemical reaction investigated here has shown complex propagative patterns, including accelerating big waves, convective rolls, double-diffusive convection, and spatiotemporal patterns. A model devised to explain the patterns involves a laterally heated fluid layer in which the basic flow loses stability in the form of hydrothermal waves. Wave motion is preceded by a global circulation between the hot and cold regions, with the velocity being proportional to the lateral temperature gradient. In this highly exothermic reaction the spatiotemporal patterns can be explained by a stability analysis of the Bénard-Marangoni convection with lateral heating.
References (37)
- M. Orbán, J. Am. Chem. Soc. 102, 4311 (1980).
- M. C. Cross and P. C. Hohenberg, Rev. Mod. Phys. 65, 851 (1993).
- A. M. Turing, Trans. R. Soc. London Ser. B 327, 37 (1952).
- G. Kshirsagar, Z. Noszticzius, W. D. McCormick and H. L. Swinney, Physica D 49, 5 (1991).
- N. Kreisberg, W. D. McCormick and H. L. Swinney, J. Chem. Phys. 91, 6532 (1989).
- M. Diewald and H. R. Brand, Chem. Phys. Lett. 216, 566 (1993).
- M. Lucke, M. Mihelicic and B. Kowalski, Phys. Rev. A 35, 4001 (1987).
- H. Bénard, Rev. Gen. Sci. Pures Appl. 11, 1261 (1990).
- Lord Rayleigh, Philos. Mag. 32, 529 (1916).
- J. R. A. Pearson, J. Fluid Mech. 4, 489 (1958).
- K. A. Smith, J. Fluid Mech. 24, 401 (1966).
- D. A. Nield, J. Fluid Mech. 19, 341 (1964).
- J. Metzger and D. Schwabe, Physicochem. Hydrodyn. 10, 263 (1988).
- L. E. Scriven and C. V. Sternling, J. Fluid Mech. 19, 321 (1965).
- J. A. Szymczyk, Can. J. Chem. Eng. 69, 1271 (1991).
- M.-I. Char and K.-T. Chiang, J. Phys. D: Appl. Phys. 27, 748 (1994).
- M. K. Smith and S. H. Davis, J. Fluid Mech. 132, 145 (1983).
- C. R. Chinake and R. H. Simoyi, J. Phys. Chem. 97, 11569 (1993).
- I. R. Epstein, K. Kustin and R. H. Simoyi, J. Phys. Chem. 96, 5852 (1992).
- G. Peintler, I. Nagypal and I. R. Epstein, J. Phys. Chem. 94, 2954 (1990).
- G. Rábai and M. Orbán, J. Phys. Chem. 97, 5935 (1993).
- H. Taube and H. Dodgen, J. Am. Chem. Soc. 71, 3330 (1949).
- C. R. Chinake and R. H. Simoyi, J. Phys. Chem. 98, 4012 (1994).
- M. J. B. Hauser and R. H. Simoyi, Phys. Lett. A 191, 31 (1994).
- A. Indelli, J. Phys. Chem. 68, 3027 (1964).
- M. J. B. Hauser and R. H. Simoyi, Chem. Phys. Lett. 227, 593 (1994).
- This was first observed in these chemical systems for reactions run in a Petri dish. In this round vessel, the null precipitation ring was much larger. See Ref. [24].
- This was also observed in an unrelated chemical system. See H. Miike, H. Yamamoto, S. Kai and S. C. Muller, Phys. Rev. E 48, 1627 (1993).
- S. Kai and H. Miike, Physica A 204, 346 (1994).
- M. J. B. Hauser and R. H. Simoyi (unpublished results).
- Amount of heat generated is proportional to the enthalpy change of the reaction, which is an extensive property of the system. Higher reagent concentrations produce a sharper thermal gradient at the wave front.
- R. H. Simoyi, J. Masere, C. Muzimbaranda, M. Manyonda and S. Dube, Int. J. Chem. Kinet. 23, 419 (1990).
- A. B. Ezersky, A. Garcimartin, J. Burguete, H. L. Mancini and C. Perez-Garcia, Phys. Rev. E 47, 1126 (1993).
- J. S. Turner, Annu. Rev. Fluid Mech. 17, 11 (1985).
- H. E. Huppert and J. S. Turner, J. Fluid Mech. 106, 299 (1981).
- D. Villers and J. K. Platten, J. Fluid Mech. 234, 487 (1992).
- Spatiotemporal and monocellular steady states were obtained in Ref. [35] in a system with a fixed cavity length. In our chemically driven system the cavity length is constantly changing as the reaction front encroaches towards the other end of the reaction vessel.