HASÍK, Karel, Jana KOPFOVÁ, Petra NÁBĚLKOVÁ, Olena TROFYMCHUK and Sergei TROFIMCHUK. Two reasons for the appearance of pushed wavefronts in the Belousov-Zhabotinsky system with spatiotemporal interaction. Journal of Differential Equations. San DIego: Academic Press Inc. Elsevier Science, 2023, vol. 376, december, p. 102-125. ISSN 0022-0396. Available from: https://dx.doi.org/10.1016/j.jde.2023.08.013.
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Basic information
Original name Two reasons for the appearance of pushed wavefronts in the Belousov-Zhabotinsky system with spatiotemporal interaction
Authors HASÍK, Karel (203 Czech Republic, belonging to the institution), Jana KOPFOVÁ (703 Slovakia, belonging to the institution), Petra NÁBĚLKOVÁ (203 Czech Republic, belonging to the institution), Olena TROFYMCHUK (804 Ukraine) and Sergei TROFIMCHUK (804 Ukraine, guarantor).
Edition Journal of Differential Equations, San DIego, Academic Press Inc. Elsevier Science, 2023, 0022-0396.
Other information
Original language English
Type of outcome Article in a journal
Field of Study 10101 Pure mathematics
Country of publisher United States of America
Confidentiality degree is not subject to a state or trade secret
WWW Journal of Differential Equations
RIV identification code RIV/47813059:19610/23:A0000135
Organization unit Mathematical Institute in Opava
Doi http://dx.doi.org/10.1016/j.jde.2023.08.013
UT WoS 001076174800001
Keywords in English Nonlocal delay; Wavefront; Reaction-diffusion; Belousov-Zhabotinsky reaction
Tags
Tags International impact, Reviewed
Changed by Changed by: Mgr. Aleš Ryšavý, učo 28000. Changed: 8/4/2024 12:46.
Abstract
We prove the existence of the minimal speed of propagation c(*)(r, b, K) is an element of [2 root 1 - r, 2] for wavefronts in the Belousov-Zhabotinsky system with a spatiotemporal interaction defined by the convolution with (possibly, "fat-tailed") kernel K. The model is assumed to be monostable non-degenerate, i.e. r is an element of (0, 1). The slowest wavefront is termed pushed or nonlinearly determined if its velocity c(*)(r, b, K) > 2 root/1 - r. We show that c(*)(r, b, K) is close to 2 if i) positive system's parameter b is sufficiently large or ii) K is spatially asymmetric to one side (e.g. to the left: in such a case, the influence of the right side concentration of the bromide ion on the dynamics is more significant than the influence of the left side). Consequently, this reveals two reasons for the appearance of pushed wavefronts in the Belousov-Zhabotinsky reaction
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