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Volumn 61, Issue 5, 2000, Pages 4943-4953

Spiral wave dynamics in oscillatory inhomogeneous media

Author keywords

[No Author keywords available]

Indexed keywords

KINETICS; OSCILLOMETRY; THEORETICAL MODEL;

EID: 0034183285     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.61.4943     Document Type: Article
Times cited : (38)

References (37)
  • 1
    • 0001928973 scopus 로고    scopus 로고
    • and references therein
    • A. T. Winfree, Chaos 8, 1 (1998), and references therein.
    • (1998) Chaos , vol.8 , pp. 1
    • Winfree, A.T.1
  • 3
    • 0004095143 scopus 로고
    • R. Kapral, K. Showalter, Kluwer Academic, Dordrecht
    • Chemical Waves and Patterns, edited by R. Kapral and K. Showalter (Kluwer Academic, Dordrecht, 1993).
    • (1993) Chemical Waves and Patterns
  • 31
    • 0001147755 scopus 로고
    • This homogeneous mechanism becomes exponentially slow as the domains grow in size. Thus it is not responsible for the relatively fast domination of a single spiral in our inhomogeneous computations [e.g., Fig. 11 (homogeneous) at (Formula presented) and Fig. 22(c) (inhomogeneous) at the earlier time (Formula presented) are for the same values of (Formula presented) and (Formula presented) and the same initial conditions]
    • I. Aranson, L. Kramer, and A. Weber, Phys. Rev. E 48, R9 (1993). This homogeneous mechanism becomes exponentially slow as the domains grow in size. Thus it is not responsible for the relatively fast domination of a single spiral in our inhomogeneous computations [e.g., Fig. 11 (homogeneous) at (Formula presented) and Fig. 22(c) (inhomogeneous) at the earlier time (Formula presented) are for the same values of (Formula presented) and (Formula presented) and the same initial conditions].
    • (1993) Phys. Rev. E , vol.48
    • Aranson, I.1    Kramer, L.2    Weber, A.3
  • 33
    • 85036215325 scopus 로고    scopus 로고
    • This argument neglects motion of the vortices such as the slow drift due to the inhomogeneity, Eq. (34)
    • This argument neglects motion of the vortices such as the slow drift due to the inhomogeneity, Eq. (34).
  • 34
    • 85036136972 scopus 로고    scopus 로고
    • For (Formula presented) the wave numbers (Formula presented) and the dominant spiral will have the highest frequency
    • For (Formula presented) the wave numbers (Formula presented) and the dominant spiral will have the highest frequency.
  • 35
    • 85036365452 scopus 로고    scopus 로고
    • Otherwise the transformation (Formula presented) (Formula presented) and (Formula presented) could be used to rescale (Formula presented) to unity
    • Otherwise the transformation (Formula presented) (Formula presented) and (Formula presented) could be used to rescale (Formula presented) to unity.
  • 37
    • 85036274539 scopus 로고    scopus 로고
    • Chaotic or quasiperiodic vortex motion could result if the inhomogeneity had a slow periodic time dependency, or if the gradient length were short enough so that our analysis yielding (Formula presented) did not apply. In regard to the latter, see Aranson et al. 19, who observe quasiperiodic motion in the case of a strong localized gradient
    • Chaotic or quasiperiodic vortex motion could result if the inhomogeneity had a slow periodic time dependency, or if the gradient length were short enough so that our analysis yielding (Formula presented) did not apply. In regard to the latter, see Aranson et al. 19, who observe quasiperiodic motion in the case of a strong localized gradient.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.