메뉴 건너뛰기




Volumn 66, Issue 4, 2002, Pages 6-

Rayleigh-Bénard convection in elliptic and stadium-shaped containers

Author keywords

[No Author keywords available]

Indexed keywords

CRITICAL TEMPERATURE; DEFECT FORMATION; NONLINEAR DISSIPATIVE SYSTEMS; RAYLEIGH-BÉNARD CONVECTION (RBC);

EID: 41349102120     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.66.046308     Document Type: Article
Times cited : (8)

References (32)
  • 4
    • 85036144249 scopus 로고    scopus 로고
    • N. M. Ercolani, R. Indik, A. C. Newell, and T. Passot, Physica D (to be published)
    • N. M. Ercolani, R. Indik, A. C. Newell, and T. Passot, Physica D (to be published).
  • 6
    • 85036378022 scopus 로고    scopus 로고
    • K. M. S. Bajaj, N. Mukolobwiez, and G. Ahlers (unpublished)
    • K. M. S. Bajaj, N. Mukolobwiez, and G. Ahlers (unpublished).
  • 11
    • 85036308168 scopus 로고    scopus 로고
    • Examples of patterns from Rayleigh-Bénard convection, including the ones in Fig. 11, can be found at http://www.nls.physics.ucsb.edu by following the link “picture page.”
    • Examples of patterns from Rayleigh-Bénard convection, including the ones in Fig. 11, can be found at http://www.nls.physics.ucsb.edu by following the link “picture page.”
  • 15
    • 85036425789 scopus 로고    scopus 로고
    • V. Croquette and A. Pocheau, in Cellular Structures in Instabilities, edited by J. E. Wesfreid and S. Zaleski (Springer, Berlin, 1984), p. 104
    • V. Croquette and A. Pocheau, in Cellular Structures in Instabilities, edited by J. E. Wesfreid and S. Zaleski (Springer, Berlin, 1984), p. 104.
  • 24
    • 85036336538 scopus 로고    scopus 로고
    • Lexan is a polycarbonate plastic
    • Lexan is a polycarbonate plastic.
  • 25
    • 85036321089 scopus 로고    scopus 로고
    • M. Paul (private communication)
    • M. Paul (private communication).
  • 27
    • 85036392192 scopus 로고    scopus 로고
    • an attempt to stabilize the roll parallel to the sidewall, we increased the power of the wall heater to 2.6 W
    • In an attempt to stabilize the roll parallel to the sidewall, we increased the power of the wall heater to 2.6 W.
  • 28
    • 85036247666 scopus 로고    scopus 로고
    • The theoretical results from Refs. 24 and 18 are for (Formula presented) The zig-zag and cross-roll instabilities for our (Formula presented) were calculated using a program provided by W. Pesch. The curvature-selected wave number is not expected to be very sensitive to (Formula presented) 18
    • The theoretical results from Refs. 24 and 18 are for (Formula presented) The zig-zag and cross-roll instabilities for our (Formula presented) were calculated using a program provided by W. Pesch. The curvature-selected wave number is not expected to be very sensitive to (Formula presented) 18.
  • 29
    • 85036269030 scopus 로고    scopus 로고
    • For one-dimensional structures, and particularly for Taylor-vortex flow, it has long been known that the bulk instability (the Eckhaus instability in this case) is suppressed 28 29 30. The instability line meets the neutral curve below and above (Formula presented) thus opening a gap in which the structure is stable until its amplitude vanishes on the neutral curve
    • For one-dimensional structures, and particularly for Taylor-vortex flow, it has long been known that the bulk instability (the Eckhaus instability in this case) is suppressed 282930. The instability line meets the neutral curve below and above (Formula presented) thus opening a gap in which the structure is stable until its amplitude vanishes on the neutral curve.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.