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Volumn 61, Issue 2, 2000, Pages 1403-1406

Logarithmically slow expansion of hot bubbles in gases

Author keywords

[No Author keywords available]

Indexed keywords

COMPACT SUPPORT; DYNAMIC SCALING; LOGARITHMIC CORRECTIONS; MATCHED ASYMPTOTIC EXPANSION; MODEL PROBLEMS; TEMPERATURE PROFILES;

EID: 0000316279     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.61.1403     Document Type: Article
Times cited : (5)

References (18)
  • 1
    • 0346505865 scopus 로고
    • A.-L. Barabási and H.E. Stanley, Fractal Concepts in Surface Growth (Cambridge University Press, Cambridge, England, 1995)
    • A.J. Bray, Adv. Phys. 43, 357 (1994);A.-L. Barabási and H.E. Stanley, Fractal Concepts in Surface Growth (Cambridge University Press, Cambridge, England, 1995)
    • (1994) Adv. Phys. , vol.43 , pp. 357
    • Bray, A.J.1
  • 3
    • 84953280783 scopus 로고    scopus 로고
    • G.I. Barenblatt, Scaling, Self-similarity, and Intermediate Asymptotics (Cambridge University Press, Cambridge, England, 1996)
    • G.I. Barenblatt, Scaling, Self-similarity, and Intermediate Asymptotics (Cambridge University Press, Cambridge, England, 1996).
  • 5
    • 85036424938 scopus 로고    scopus 로고
    • Ya.B. Zel’dovich and Yu.P. Raizer, The Physics of Shock Waves and High Temperature Hydrodynamic Phenomena (Academic, New York, 1967)
    • Ya.B. Zel’dovich and Yu.P. Raizer, The Physics of Shock Waves and High Temperature Hydrodynamic Phenomena (Academic, New York, 1967).
  • 10
    • 85036146032 scopus 로고    scopus 로고
    • Alternatively, one obtains a nonlinear diffusion equation for the gas density, (Formula presented), with the effective diffusion coefficient decreasing with (Formula presented). This equation appeared in a number of nonlinear diffusion problems where (Formula presented) decays at (Formula presented) 17. In the hot bubble problem (Formula presented) at (Formula presented), and this difference results in quite a different dynamics
    • Alternatively, one obtains a nonlinear diffusion equation for the gas density, (Formula presented), with the effective diffusion coefficient decreasing with (Formula presented). This equation appeared in a number of nonlinear diffusion problems where (Formula presented) decays at (Formula presented) 17. In the hot bubble problem (Formula presented) at (Formula presented), and this difference results in quite a different dynamics.
  • 12
    • 85036269777 scopus 로고    scopus 로고
    • The heat flux (Formula presented) should be continuous. For (Formula presented) it implies (Formula presented)
    • The heat flux (Formula presented) should be continuous. For (Formula presented) it implies (Formula presented).
  • 13
    • 85036325554 scopus 로고    scopus 로고
    • Shrinking is possible when a cold “cloud” is heated by a hot and underdense peripheral gas. A problem mathematically equivalent to this one was considered in Ref. 17
    • Shrinking is possible when a cold “cloud” is heated by a hot and underdense peripheral gas. A problem mathematically equivalent to this one was considered in Ref. 17.
  • 14
    • 85036187702 scopus 로고    scopus 로고
    • reality, the temperature should approach a finite value at large distances. Correspondingly, the solution we are interested in represents an intermediate asymptotics 2
    • In reality, the temperature should approach a finite value at large distances. Correspondingly, the solution we are interested in represents an intermediate asymptotics 2.
  • 15
    • 85036266985 scopus 로고    scopus 로고
    • If (Formula presented) is a solution of Eq. (3), then (Formula presented) is also a solution for any (Formula presented). This property enables one to restore the k dependence in the final results
    • If (Formula presented) is a solution of Eq. (3), then (Formula presented) is also a solution for any (Formula presented). This property enables one to restore the k dependence in the final results.
  • 16


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.