J 2023

Two reasons for the appearance of pushed wavefronts in the Belousov-Zhabotinsky system with spatiotemporal interaction

HASÍK, Karel, Jana KOPFOVÁ, Petra NÁBĚLKOVÁ, Olena TROFYMCHUK, Sergei TROFIMCHUK et. al.

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

Language

English

Type of outcome

Článek v odborném periodiku

Field of Study

10101 Pure mathematics

Country of publisher

United States of America

Confidentiality degree

není předmětem státního či obchodního tajemství

RIV identification code

RIV/47813059:19610/23:A0000135

Organization unit

Mathematical Institute in Opava

UT WoS

001076174800001

Keywords in English

Nonlocal delay; Wavefront; Reaction-diffusion; Belousov-Zhabotinsky reaction

Tags

Tags

International impact, Reviewed
Změněno: 8/4/2024 12:46, Mgr. Aleš Ryšavý

Abstract

V originále

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