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Some properties of two-dimensional inverse energy cascade dynamics
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Citations
29
References
1997
Year
Steady StateEngineeringPhysicsEnergy CascadeTurbulent Flow Heat TransferFluid MechanicsDiscrete Dynamical SystemTurbulence ModelingInverse Energy CascadeTransport PhenomenaBifurcation TheoryChaotic MixingNonlinear ResonanceHydrodynamic StabilityRarest Transfers
In this work we analyze the degree of homogeneity and stationarity of the transfers in the inverse energy cascade of two-dimensional turbulence. Two extreme cases, namely, a well-developed inverse energy cascade in a robust statistically steady state and the collision of two vortices of the same sign, which is a clear illustration of a nonstationary cascade regime, are studied. We consider the absolute transfer ${\mathrm{\ensuremath{\eta}}}_{\mathrm{l}}$ at scale l produced by the nonlinear term of the Navier-Stokes equation. The scaling properties of the transfer hierarchy 〈\ensuremath{\eta}${\mathrm{}}_{\mathrm{l}}^{\mathrm{p}+1}$〉/〈\ensuremath{\eta}${\mathrm{}}_{\mathrm{l}}^{\mathrm{p}}$〉\ensuremath{\sim}${\mathrm{l}}^{\mathrm{\ensuremath{-}}{\mathrm{\ensuremath{\delta}}}_{\mathrm{p}}}$ are examined. We define \ensuremath{\Delta}=(${\mathrm{\ensuremath{\delta}}}_{\mathrm{\ensuremath{\infty}}}$-${\mathrm{\ensuremath{\delta}}}_{0}$)/${\mathrm{\ensuremath{\zeta}}}_{3}^{\mathrm{*}}$, where ${\mathrm{\ensuremath{\zeta}}}_{3}^{\mathrm{*}}$ is the scaling of the third-order structure function of absolute velocity increments, ${\mathrm{\ensuremath{\delta}}}_{0}$ is a quantity tracing the smallest but most frequent transfers, and ${\mathrm{\ensuremath{\delta}}}_{\mathrm{\ensuremath{\infty}}}$ characterizes the largest but rarest transfers. We show that \ensuremath{\Delta} plays a fundamental role in the scaling description of the cascade dynamics. In two-dimensional energy cascade, the important property of the relationship between the scaling of the structure functions and the distribution of the heterogeneities in the physical space given by (${\mathrm{\ensuremath{\delta}}}_{\mathrm{\ensuremath{\infty}}}$ -${\mathrm{\ensuremath{\delta}}}_{0}$ ) is the invariance of \ensuremath{\Delta}. Finally, we determine the physical meaning of the formally introduced adjustable parameters in She-Leveque [Phys. Rev. Lett. 72, 336 (1994)] and Dubrulle [Phys Rev. Lett. 73, 7 (1994); 73, 959 (1994)] intermittency models.
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