Abstract
We show that the large-eddy motions in turbulent fluid flow obey a modified hydrodynamic equation with a stochastic turbulent stress whose distribution is a causal functional of the large-scale velocity field itself. We do so by means of an exact procedure of “statistical filtering” of the Navier-Stokes equations, which formally solves the closure problem, and we discuss the relation of our analysis with the “decimation theory” of Kraichnan. We show that the statistical filtering procedure can be formulated using field-theoretic path-integral methods within the Martin-Siggia-Rose (MSR) formalism for classical statistical dynamics. We also establish within the MSR formalism a “least-effective-action principle” for mean turbulent velocity profiles, which generalizes Onsager's principle of least dissipation. This minimum principle is a consequence of a simple realizability inequality and therefore holds also in any realizable closure. Symanzik's theorem in field theory—which characterizes the static effective action as the minimum expected value of the quantum Hamiltonian over all state vectors with prescribed expectations of fields—is extended to MSR theory with non-Hermitian Hamiltonian. This allows stationary mean velocity profiles and other turbulence statistics to be calculated variationally by a Rayleigh-Ritz procedure. Finally, we develop approximations of the exact Langevin equations for large eddies, e.g., a random-coupling DIA model, which yield new stochastic LES models. These are compared with stochastic subgrid modeling schemes proposed by Rose, Chasnov, Leith, and others, and various applications are discussed.
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References
R. H. Kraichnan, Eddy viscosity in two and three dimensions,J. Atmos. Sci. 33:1521 (1976).
R. H. Kraichnan, Eddy viscosity and diffusivity: Exact formulas and approximations,Complex Systems 1:805 (1987).
L. D. Landau and E. M. Lifshitz,Fluid Mechanics (Pergamon Press, New York, 1959), Chapter 17.
H. A. Rose, Eddy diffusivity, eddy noise, and sub-grid scale modelling,J. Fluid Mech. 81:719 (1977).
C. E. Leith, Stochastic backscatter in a subgrid-scale model: Plane shear mixing layer,Phys. Fluids A 2:297 (1990).
J. R. Chasnov, Simulation of the Kolmogorov inertial subrange using an improved subgrid model,Phys. Fluids A 3:188 (1991).
P. J. Mason and D. J. Thomson, Stochastic backscatter in large-eddy simulations of boundary layers,J. Fluid Mech. 242:51 (1992).
D. Carati, Iterative filtering of the forced Navier-Stokes equation, Preprint (1994).
V. Yakhot and S. A. Orszag, Renormalization group analysis of turbulence, I. Basic theory,J. Sci. Comp. 1:3 (1986).
R. H. Kraichnan, Decimated amplitude equations in turbulence dynamics, inTheoretical Approaches to Turbulence, D. L. Dwoyer, M. Y. Hussaini, and R. G. Voigt, eds. (Springer, New York, 1985).
P. C. Martin, E. D. Siggia, and H. A. Rose, Statistical dynamics of classical systems,Phys. Rev. A 8:423 (1973).
L. Onsager, Reciprocal relations in irreversible processes. I, II,Phys. Rev. 37:405 (1931);38:2265 (1931).
G. L. Eyink, Large-eddy simulation and the “multifractal model” of turbulence:a priori estimates on subgrid flux and locality of energy transfer,Phys. Fluids, submitted (1994).
M. Germano, Turbulence: The filtering approach,J. Fluid Mech. 238:325 (1992).
M. Germano, A proposal for a redefinition of the turbulent stresses in the filtered Navier-Stokes equations,Phys. Fluids 29:2323 (1986).
A. Leonard, On the energy cascade in large-eddy simulations of turbulent flows,Adv. Geophys. 18A:237 (1974).
D. Ruelle, Measures describing a turbulent flow,Ann. N.Y. Acad. Sci. 357:1 (1980).
J.-P. Eckmann and D. Ruelle, Ergodic theory of chaos and strange attractors,Rev. Mod. Phys. 57:617 (1985).
D. Ruelle, Microscopic fluctuations and turbulence,Phys. Lett. A 72:81 (1979).
P. C. Hohenberg and B. Shraiman, Chaotic behavior of an extended system,Physica D 37:109 (1989).
V. Yakhot, Large-scale properties of unstable systems governed by the Kuramoto-Sivashinsky equation,Phys. Rev. A 24:642 (1983).
S. Zaleski, A stochastic model for the large scale dynamics of some fluctuating interfaces,Physica D 34:427 (1989).
K. Sneppenet al., Dynamic scaling and crossover analysis for the Kuramoto-Sivashinsky equation,Phys. Rev. A 46:R7351 (1992).
E. Lorenz, Maximum simplification of the dynamic equations,Tellus 12:243 (1960).
R. Phythian, The operator formalism of classical statistical dynamics,J. Phys. A 8:1423 (1975).
R. Phythian, Further application of the Martin, Siggia, Rose formalism,J. Phys. A 9:269 (1976).
H. K. Janssen, On a Lagrangean for classical field dynamics and renormalization group calculations of dynamical critical properties,Z. Phys. B 23:377 (1976).
C. DeDominicis, Techniques de renormalisation de la théorie des champs et dynamique des phénomènes critiques,J. Phys. (Paris)C 1:247 (1976).
R. Graham, Path integral formulation of general diffusion processes,Z. Phys. B 26:281 (1977).
R. Graham, Short-time propagators in Riemannian geometries, inStatphys 13 (Proceedings of the 13th IUPAP Conference on Statistical Physics, Haifa, 1977).
U. Weiss, Operator ordering schemes and covariant path integrals of quantum and stochastic processes in curved space,Z. Phys. B 30:429 (1978).
C. Wissel, Manifolds of equivalent path integral solutions of the Fokker-Planck equations,Z. Phys. B 35:185 (1979).
L. Arnold,Stochastic Differential Equations: Theory and Applications (Wiley, New York, 1974).
T. D. Lee, On some statistical properties of the hydrodynamical and magnetohydrodynamical fields,Q. Appl. Math. 10:69 (1952).
H. W. Wyld, Formulation of the theory of turbulence in an incompressible fluid,Ann. Phys. (N.Y.)14:143 (1961).
R. H. Kraichnan, Dynamics of nonlinear stochastic systems,J. Math. Phys. 2:124 (1961).
V. E. Zakharov and V. S. L'vov, Statistical description of nonlinear wave fields,Izv. Vyss. Uch. Zav. Radiofiz. 18:1470 (1975).
R. H. Kraichnan, Eulerian and Lagrangian renormalization in turbulence theory,J. Fluid Mech. 83:349 (1977).
G. L. Eyink, The renormalization group method in statistical hydrodynamics,Phys. Fluids 6:3063 (1994).
V. S. L'vovet al., Proof of scale invariant solutions in the Kardar-Parisi-Zhang and Kuramoto-Sivashinsky equations in 1+1 dimensions: Analytical and numerical results,Nonlinearity 6:25 (1993).
K. Symanzik, Renormalizable models with simple symmetry breaking,Commun. Math. Phys. 16:48 (1970).
W. Heisenberg and H. Euler, Folgerungen aus der Diracschen Theorie des Positrons,Z. Phys. 98:714 (1936).
J. Schwinger, On gauge invariance and vacuum polarization,Phys. Rev. 82:664 (1951).
L. Onsager and S. Machlup, Fluctuations and irreversible processes,Phys. Rev. 91:1505 (1953).
R. Graham, Path-integral methods in nonequilibrium thermodynamics and statistics, inStochastic Processes in Nonequilibrium Systems, L. Garrido, P. Seglar, and P. J. Shepherd, eds. (Springer-Verlag, Berlin, 1978).
G. L. Eyink, Dissipation and large thermodynamic fluctuations,J. Stat. Phys. 61:533 (1990).
J. M. Cornwall, R. Jackiw, and E. Tomboulis, Effective action for composite operators,Phys. Rev. D 10:2428 (1974).
H. Risken,The Fokker-Planck Equation (Springer-Verlag, Berlin, 1984).
M. Hausner and J. T. Schwartz,Lie Groups and Their Lie Algebras (Gordon and Breach, New York, 1968).
D. Ruelle, Locating resonances for Axiom A dynamical systems,J. Stat. Phys. 44:281 (1986).
R. Jackiw and A. Kerman, Time-dependent variational principle and effective action,Phys. Lett. A 71:158 (1979).
P. A. M. Dirac, Note on exchange phenomena in the Thomas atom,Proc. Camb. Phil. Soc. 26:376 (1930).
R. H. Kraichnan, Convergents to turbulence functions,J. Fluid Mech. 41:189 (1970).
R. H. Kraichnan, Irreversible statistical mechanics of incompressible hydromagnetic turbulence,Phys. Rev. 109:1407 (1958).
R. H. Kraichnan, Variational method in turbulence theory,Phys. Rev. Lett. 42:1263 (1979).
J. Qian, Variational approach to the closure problem of turbulence theory,Phys. Fluids 26:2098 (1983).
B. Castaing, Conséquences d'un principe d'extrémum en turbulence,J. Phys. (Paris)50:147 (1989).
F. H. Busse, The optimum theory of turbulence,Adv. Appl. Math. 18:77 (1978).
J. R. Herring and R. H. Kraichnan, Comparison of some approximations for isotropic turbulence, inStatistical Models and Turbulence, M. Rosenblatt and C. Van Atta, eds. (Springer, New York, 1972).
C. Meneveau and A. Chhabra, Two-point statistics of multifractal measures,Physica A 164:564 (1990).
C. E. Leith and R. H. Kraichnan, Predictability of turbulent flows,J. Atmos. Sci. 29:1041 (1972).
E. N. Lorenz, Deterministic non-periodic flow,J. Atmos. Sci. 20:130 (1963).
R. A. Pielkeet al., Several unresolved isues in numerical modelling of geophysical flows,Atmos. Oceans, submitted.
C. C. Chow and T. Hwa, Defect-mediated stability: an effective hydrodynamic theory of spatiotemporal chaos, Preprint [chao-dyn@xyz.lanl.gov, #9412041].
C. Jarzynski, Thermalization of a Brownian particle via coupling to low-dimensional chaos,Phys. Rev. Lett. 74:2937 (1995).
D. N. Zubarev and V. G. Morozov, Statistical mechanics of nonlinear hydrodynamic fluctuations,Physica 120A:411 (1983).
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Eyink, G.L. Turbulence noise. J Stat Phys 83, 955–1019 (1996). https://doi.org/10.1007/BF02179551
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DOI: https://doi.org/10.1007/BF02179551