2001
DOI: 10.1103/physreve.64.036218
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Structure and variability of spinning reaction waves in three-dimensional excitable media

Abstract: A mathematical simulation for a reaction wave that propagates in a cylindrical sample is performed. The propagation modes that have not yet been observed experimentally are predicted. The areas of existence for these modes have been determined.

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Cited by 35 publications
(20 citation statements)
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“…38 Finally, we note that the obtained rotating, as well as axially-''frozen,'' patterns were found to emerge in two-variable bistable systems that exhibit ideal fronts in a 1D case, if the ratio of the diffusivities of the inhibitor to the activator exceeds certain critical values. This is contrary to the rotating and nonrotating oscillating patterns in the case of oscillatory kinetics which can emerge 37,38 with Pe C ) Pe T , as well as the contrary to spinning mode of gasless combustion (self-propagating high-temperature synthesis), 39,40 which was revealed for a completely nondiffusive inhibitor under kinetic and thermodynamic conditions corresponding to unstable 1D front propagation. 41 …”
Section: Discussioncontrasting
confidence: 52%
“…38 Finally, we note that the obtained rotating, as well as axially-''frozen,'' patterns were found to emerge in two-variable bistable systems that exhibit ideal fronts in a 1D case, if the ratio of the diffusivities of the inhibitor to the activator exceeds certain critical values. This is contrary to the rotating and nonrotating oscillating patterns in the case of oscillatory kinetics which can emerge 37,38 with Pe C ) Pe T , as well as the contrary to spinning mode of gasless combustion (self-propagating high-temperature synthesis), 39,40 which was revealed for a completely nondiffusive inhibitor under kinetic and thermodynamic conditions corresponding to unstable 1D front propagation. 41 …”
Section: Discussioncontrasting
confidence: 52%
“…With a further increase in Λ, the velocities of the combustion waves increase for all values of R 1 (curves [4][5][6]. It is of interest that the curves for Λ = 0.004 and 10 almost coincide for R 1 < 24.…”
Section: Resultsmentioning
confidence: 97%
“…3b, however, that the front near the rod stays behind the front on the specimen surface if the line with η = 0.9 is considered as the front, while the outer part of the front moves ahead of the inner part of the front if the line with η = 0.2 is used. In both cases, the front near the rod has the form of a cone directed by its narrow side toward the products in the first case [6] and toward the original reagents in the second case. The structure described in [12] could not be obtained.…”
Section: Resultsmentioning
confidence: 99%
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