New approximate solution for N-point correlation functions for heterogeneous materials

Abstract Statistical N -point correlation functions are used for calculating properties of heterogeneous systems. The strength and the main advantage of the statistical continuum approach is the direct link to statistical information of microstructure. Two-point correlation functions are the lowest order of correlation functions that can describe the morphology and the microstructure-properties relationship. Experimentally, statistical pair correlation functions are obtained using SEM or small x-ray scattering techniques. Higher order correlation functions must be calculated or measured to increase the precision of the statistical continuum approach. To achieve this aim a new approximation methodology is utilized to obtain N -point correlation functions for non-FGM (functional graded materials) heterogeneous microstructures. Conditional probability functions are used to formulate the proposed theoretical approximation. In this approximation, weight functions are used to connect subsets of ( N −1)-point correlation functions to estimate the full set of N -point correlation function. For the approximation of three and four point correlation functions, simple weight functions have been introduced. The results from this new approximation, for three-point probability functions, are compared to the real probability functions calculated from a computer generated three-phase reconstructed microstructure in three-dimensional space. This three-dimensional reconstruction was based on an experimental two-dimensional microstructure (SEM image) of a three-phase material. This comparison proves that our new comprehensive approximation is capable of describing higher order statistical correlation functions with the needed accuracy.

[1]  S. Ahzi,et al.  3D Reconstruction of Carbon Nanotube Composite Microstructure Using Correlation Functions , 2010 .

[2]  S. Ahzi,et al.  Statistical continuum theory for the effective conductivity of carbon nanotubes filled polymer composites , 2011 .

[3]  S. Ahzi,et al.  Using SAXS approach to estimate thermal conductivity of polystyrene/zirconia nanocomposite by exploiting strong contrast technique , 2011 .

[4]  N. Phan-Thien,et al.  New bounds on the effective thermal conductivity of N-phase materials , 1982, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[5]  D. Jeulin,et al.  Determination of the size of the representative volume element for random composites: statistical and numerical approach , 2003 .

[6]  P. H. Dederichs,et al.  Variational treatment of the elastic constants of disordered materials , 1973 .

[7]  Sen,et al.  Effective conductivity of anisotropic two-phase composite media. , 1989, Physical review. B, Condensed matter.

[8]  J. Willis,et al.  Variational and Related Methods for the Overall Properties of Composites , 1981 .

[9]  Walmir Freitas,et al.  Characteristics of vector surge relays for distributed synchronous generator protection , 2007 .

[10]  S. Torquato,et al.  Random Heterogeneous Materials: Microstructure and Macroscopic Properties , 2005 .

[11]  F. Stillinger,et al.  A superior descriptor of random textures and its predictive capacity , 2009, Proceedings of the National Academy of Sciences.

[12]  J. McCoy On the calculation of bulk properties of heterogeneous materials , 1979 .

[13]  P. Corson,et al.  Correlation functions for predicting properties of heterogeneous materials. II. Empirical construction of spatial correlation functions for two‐phase solids , 1974 .

[14]  Salvatore Torquato,et al.  Effective electrical conductivity of two‐phase disordered composite media , 1985 .

[15]  David T. Fullwood,et al.  A strong contrast homogenization formulation for multi-phase anisotropic materials , 2008 .

[16]  Xin Sun,et al.  Three-phase solid oxide fuel cell anode microstructure realization using two-point correlation functions , 2011 .

[17]  O. Glatter,et al.  19 – Small-Angle X-ray Scattering , 1973 .

[18]  Salvatore Torquato,et al.  Effective stiffness tensor of composite media—I. Exact series expansions , 1997 .

[19]  Martin Ostoja-Starzewski,et al.  Scaling function, anisotropy and the size of RVE in elastic random polycrystals , 2008 .

[20]  William Fuller Brown,et al.  Solid Mixture Permittivities , 1955 .

[21]  S. Ahzi,et al.  Statistical continuum theory for large plastic deformation of polycrystalline materials , 2001 .

[22]  H. Garmestani,et al.  Statistical continuum theory for inelastic behavior of a two-phase medium , 1998 .

[23]  A. Gokhale,et al.  Constraints on microstructural two-point correlation functions , 2005 .

[24]  H. R. Anderson,et al.  Scattering by an Inhomogeneous Solid. II. The Correlation Function and Its Application , 1957 .

[25]  H. Garmestani,et al.  Microstructure design of a two phase composite using two-point correlation functions , 2004 .

[26]  Brent L. Adams,et al.  Description of orientation coherence in polycrystalline materials , 1987 .

[27]  M. Ostoja-Starzewski,et al.  On the Size of RVE in Finite Elasticity of Random Composites , 2006 .

[28]  Dongsheng Li,et al.  Semi-inverse Monte Carlo reconstruction of two-phase heterogeneous material using two-point functions , 2009 .

[29]  Mark J. Beran,et al.  Statistical Continuum Theories , 1968 .

[30]  Yves Rémond,et al.  Effective conductivity in isotropic heterogeneous media using a strong-contrast statistical continuum theory , 2009 .

[31]  The evolution of probability functions in an inelasticly deforming two-phase medium , 2000 .

[32]  S. Ahzi,et al.  A new approximation for the three-point probability function , 2009 .

[33]  S. Torquato,et al.  Reconstructing random media , 1998 .