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Volumn 66, Issue 2, 2002, Pages

Intermittency in two-dimensional Ekman-Navier-Stokes turbulence

Author keywords

[No Author keywords available]

Indexed keywords

FRICTION; INCOMPRESSIBLE FLOW; LYAPUNOV METHODS; NAVIER STOKES EQUATIONS; PROBABILITY DENSITY FUNCTION; STATISTICAL METHODS; TURBULENCE; VISCOSITY; VORTEX FLOW;

EID: 41349105244     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.66.026304     Document Type: Article
Times cited : (62)

References (13)
  • 1
    • 85036236967 scopus 로고    scopus 로고
    • R. Salmon, Geophysical Fluid Dynamics (Oxford University Press, New York, 1998)
    • R. Salmon, Geophysical Fluid Dynamics (Oxford University Press, New York, 1998);
  • 2
    • 0022776226 scopus 로고
    • other well known examples are the Rayleigh friction in stratified fluids, the Hartmann friction in magneto-hydrodynamics [J. Sommeria, J. Fluid Mech. 170, 139 (1986)]
    • (1986) J. Fluid Mech. , vol.170 , pp. 139
    • Sommeria, J.1
  • 3
    • 0034224182 scopus 로고    scopus 로고
    • and the friction induced by surrounding air in soap films [M. Rivera and X.L. Wu, Phys. Rev. Lett. 85, 976 (2000)].
    • (2000) Phys. Rev. Lett. , vol.85 , pp. 976
    • Rivera, M.1    Wu, X.L.2
  • 4
    • 85036339512 scopus 로고    scopus 로고
    • The numerical integration of Eq. (1) starting from a zero field is performed by a fully dealiased pseudospectral code with a second-order Runge-Kutta scheme, on a doubly periodic square domain of size (Formula presented) at different resolutions: (Formula presented) grid points. A small viscosity (depending on the resolution: (Formula presented) for (Formula presented) (Formula presented) for (Formula presented) and (Formula presented) for (Formula presented) is used to remove the remnant enstrophy flux at small scales. The large-scale forcing (Formula presented) is Gaussian, (Formula presented) correlated in time, and limited to a shell of wave numbers around (Formula presented) (Formula presented) for (Formula presented), and (Formula presented) for (Formula presented). Forcing amplitude is chosen to provide an enstrophy injection rate (Formula presented). At variance with other choices for (Formula presented) commonly used (e.g., large-scale shear), this kind of forcing ensures the statistical isotropy and homogeneity of the vorticity field
    • The numerical integration of Eq. (1) starting from a zero field is performed by a fully dealiased pseudospectral code with a second-order Runge-Kutta scheme, on a doubly periodic square domain of size (Formula presented) at different resolutions: (Formula presented) grid points. A small viscosity (depending on the resolution: (Formula presented) for (Formula presented) (Formula presented) for (Formula presented) and (Formula presented) for (Formula presented) is used to remove the remnant enstrophy flux at small scales. The large-scale forcing (Formula presented) is Gaussian, (Formula presented) correlated in time, and limited to a shell of wave numbers around (Formula presented) (Formula presented) for (Formula presented), and (Formula presented) for (Formula presented). Forcing amplitude is chosen to provide an enstrophy injection rate (Formula presented). At variance with other choices for (Formula presented) commonly used (e.g., large-scale shear), this kind of forcing ensures the statistical isotropy and homogeneity of the vorticity field.
  • 8
    • 85036240545 scopus 로고    scopus 로고
    • E. Ott, Chaos in Dynamical Systems (Cambridge University Press, Cambridge, England, 1993)
    • E. Ott, Chaos in Dynamical Systems (Cambridge University Press, Cambridge, England, 1993).
  • 9
    • 85036145496 scopus 로고    scopus 로고
    • T. Bohr, M. H. Jensen, G. Paladin, and A. Vulpiani, Dynamical Systems Approach to Turbulence (Cambridge University Press, Cambridge, England, 1998)
    • T. Bohr, M. H. Jensen, G. Paladin, and A. Vulpiani, Dynamical Systems Approach to Turbulence (Cambridge University Press, Cambridge, England, 1998).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.