Natural Convection in a Closed Cavity under Stochastic Non-Boussinesq Conditions

A stochastic projection method (SPM) is developed for quantitative propagation of uncertainty in compressible zero-Mach-number flows. The formulation is based on a spectral representation of uncertainty using the polynomial chaos (PC) system, and on a Galerkin approach to determining the PC coefficients. Governing equations for the stochastic modes are solved using a mass-conservative projection method. The formulation incorporates a specially tailored stochastic inverse procedure for exactly satisfying the mass-conservation divergence constraints. A brief validation of the zero-Mach-number solver is first performed, based on simulations of natural convection in a closed cavity. The SPM is then applied to analyze the steady-state behavior of the heat transfer and of the velocity and temperature fields under stochastic non-Boussinesq conditions.

[1]  M. Hortmann,et al.  Finite volume multigrid prediction of laminar natural convection: Bench-mark solutions , 1990 .

[2]  P. S. Wyckoff,et al.  A Semi-implicit Numerical Scheme for Reacting Flow , 1998 .

[3]  P. Le Quéré,et al.  Computation of natural convection in two-dimensional cavities with Chebyshev polynomials , 1985 .

[4]  N. Wiener The Homogeneous Chaos , 1938 .

[5]  S. Paolucci,et al.  Natural convection in an enclosed vertical air layer with large horizontal temperature differences , 1986, Journal of Fluid Mechanics.

[6]  M. Loève,et al.  Elementary Probability Theory , 1977 .

[7]  F. Maltz,et al.  Variance reduction in Monte Carlo computations using multi-dimensional hermite polynomials , 1979 .

[8]  G. H. Canavan,et al.  Relationship between a Wiener–Hermite expansion and an energy cascade , 1970, Journal of Fluid Mechanics.

[9]  R. Ghanem,et al.  A stochastic projection method for fluid flow. I: basic formulation , 2001 .

[10]  A. Chorin Gaussian fields and random flow , 1974, Journal of Fluid Mechanics.

[11]  P. LeQuéré,et al.  Accurate solutions to the square thermally driven cavity at high Rayleigh number , 1991 .

[12]  H. Najm,et al.  A stochastic projection method for fluid flow II.: random process , 2002 .

[13]  O. L. Maître,et al.  Protein labeling reactions in electrochemical microchannel flow: Numerical simulation and uncertainty propagation , 2003 .

[14]  James A. Sethian,et al.  THE DERIVATION AND NUMERICAL SOLUTION OF THE EQUATIONS FOR ZERO MACH NUMBER COMBUSTION , 1985 .

[15]  G. de Vahl Davis,et al.  Natural convection in a square cavity: A comparison exercise , 1983 .

[16]  R. Ghanem,et al.  Stochastic Finite Elements: A Spectral Approach , 1990 .

[17]  Habib N. Najm,et al.  Regular Article: A Semi-implicit Numerical Scheme for Reacting Flow , 1999 .

[18]  P. Le Quéré,et al.  A Chebyshev collocation algorithm for 2D non-Boussinesq convection , 1992 .

[19]  W. Meecham,et al.  Use of the Wiener—Hermite expansion for nearly normal turbulence , 1968, Journal of Fluid Mechanics.

[20]  W. T. Martin,et al.  The Orthogonal Development of Non-Linear Functionals in Series of Fourier-Hermite Functionals , 1947 .

[21]  Roger Ghanem,et al.  Stochastic Finite Element Analysis for Multiphase Flow in Heterogeneous Porous Media , 1998 .

[22]  H. Paillere,et al.  Comparison of low Mach number models for natural convection problems , 2000 .

[23]  A. Chorin Hermite expansions in Monte-Carlo computation , 1971 .

[24]  R. Ghanem Probabilistic characterization of transport in heterogeneous media , 1998 .