Energy cascade and spatial fluxes in wall turbulence

Real turbulent flows are difficult to classify as either spatially homogeneous or isotropic. Nonetheless these idealizations allow the identification of certain universal features associated with the small-scale motions almost invariably observed in a variety of different conditions. The single most significant aspect is a flux of energy through the spectrum of inertial scales related to the phenomenology commonly referred to as the Richardson cascade. Inhomogeneity, inherently present in near-wall turbulence, generates additional energy fluxes of a different nature, corresponding to the spatial redistribution of turbulent kinetic energy. Traditionally the spatial flux is associated with a single-point observable, namely the turbulent kinetic energy density. The flux through the scales is instead classically related to two-point statistics, given in terms of an energy spectrum or, equivalently, in terms of the second-order moment of the velocity increments. In the present paper, starting from a suitably generalized form of the classical Kolmogorov equation, a scale-by-scale balance for the turbulent fluctuations is evaluated by examining in detail how the energy associated with a specific scale of motion – hereafter called the scale energy – is transferred through the spectrum of scales and, simultaneously, how the same scale of motion exchanges energy with a properly defined spatial flux. The analysis is applied to a data set taken from a direct numerical simulation (DNS) of a low-Reynolds-number turbulent channel flow. The detailed scale-by-scale balance is applied to the different regions of the flow in the various ranges of scales, to understand how – i.e. through which mechanisms, at which scales and in which regions of the flow domain – turbulent fluctuations are generated and sustained. A complete and formally precise description of the dynamics of turbulence in the different regions of the channel flow is presented, providing rigorous support for previously proposed conceptual models.

[1]  S. Ciliberto,et al.  Scaling properties of the streamwise component of velocity in a turbulent boundary layer , 2000 .

[2]  Javier Jiménez,et al.  THE PHYSICS OF WALL TURBULENCE , 1999 .

[3]  C. Casciola,et al.  Experimental assessment of a new form of scaling law for near-wall turbulence , 2001, nlin/0102015.

[4]  John Kim,et al.  Regeneration mechanisms of near-wall turbulence structures , 1995, Journal of Fluid Mechanics.

[5]  John Kim,et al.  DIRECT NUMERICAL SIMULATION OF TURBULENT CHANNEL FLOWS UP TO RE=590 , 1999 .

[6]  K. Sreenivasan,et al.  Dynamical equations for high-order structure functions, and a comparison of a mean-field theory with experiments in three-dimensional turbulence. , 2001, Physical review. E, Statistical, nonlinear, and soft matter physics.

[7]  P. Moin,et al.  Turbulence statistics in fully developed channel flow at low Reynolds number , 1987, Journal of Fluid Mechanics.

[8]  V. Nikora Origin of the “−1” Spectral Law in Wall-Bounded Turbulence , 1999 .

[9]  P. S. Klebanoff,et al.  Characteristics of turbulence in a boundary layer with zero pressure gradient , 1955 .

[10]  M. Oberlack A unified approach for symmetries in plane parallel turbulent shear flows , 2001, Journal of Fluid Mechanics.

[11]  E. Lindborg,et al.  CORRECTION TO THE FOUR-FIFTHS LAW DUE TO VARIATIONS OF THE DISSIPATION , 1999 .

[12]  Helmut Eckelmann,et al.  The structure of the viscous sublayer and the adjacent wall region in a turbulent channel flow , 1974, Journal of Fluid Mechanics.

[13]  Mohamed Gad-el-Hak,et al.  Reynolds Number Effects in Wall-Bounded Turbulent Flows , 1994 .

[14]  Roberto Benzi,et al.  Scale-by-scale budget and similarity laws for shear turbulence , 2002, Journal of Fluid Mechanics.

[15]  F. Toschi,et al.  Intermittency and scaling laws for wall bounded turbulence , 1998, chao-dyn/9812009.

[16]  S. K. Robinson,et al.  Coherent Motions in the Turbulent Boundary Layer , 1991 .

[17]  Seyed G. Saddoughi,et al.  Local isotropy in turbulent boundary layers at high Reynolds number , 1994, Journal of Fluid Mechanics.

[18]  Reginald J. Hill,et al.  Exact second-order structure-function relationships , 2002, Journal of Fluid Mechanics.

[19]  F. Clauser The Structure of Turbulent Shear Flow , 1957, Nature.

[20]  A. Kolmogorov The local structure of turbulence in incompressible viscous fluid for very large Reynolds numbers , 1991, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[21]  V. Yakhot Mean-field approximation and a small parameter in turbulence theory. , 2000, Physical review. E, Statistical, nonlinear, and soft matter physics.

[22]  Roberto Benzi,et al.  Intermittency and Structure Functions in Channel Flow Turbulence , 1998, chao-dyn/9807027.

[23]  P. Moin,et al.  The minimal flow unit in near-wall turbulence , 1991, Journal of Fluid Mechanics.

[24]  R. Benzi,et al.  Scaling laws and intermittency in homogeneous shear flow , 2000, nlin/0011040.

[25]  M. S. Chong,et al.  A theoretical and experimental study of wall turbulence , 1986, Journal of Fluid Mechanics.

[26]  Javier Jiménez,et al.  The autonomous cycle of near-wall turbulence , 1999, Journal of Fluid Mechanics.

[27]  Reginald J. Hill,et al.  Next-order structure-function equations , 2001 .

[28]  Alexander J. Smits,et al.  Scaling of the mean velocity profile for turbulent pipe flow , 1997 .

[29]  Tongming Zhou,et al.  Turbulent energy scale budget equations in a fully developed channel flow , 2001, Journal of Fluid Mechanics.