Page 92 - Mechanics of Asphalt Microstructure and Micromechanics
P. 92

Microstructure Characterization   85


              Strain-Fabric Tensor Relation
              In continuum mechanics, the deformation rate tenor (D ij ) and the spin tensor (W ij ) are
              used to represent the strain characteristics. Mehrabadi and Nemat-Nasser (1983) also
              derived the relations relating D ij  and W ij  to contact normal tensor J ij and local strain
              rates E ij .
                                              1
                                          D = ( E J + E J )                      (3-19)
                                           ij    ik kj  jk ki
                                              2
                                              1
                                         W = (  E J −  E J )                     (3-20)
                                                 ik kj
                                                       jk ki
                                           ij
                                              2
                 Kanatani (1984a, 1985) offers relationships between strains and fabric evolution as
              well.
              Other Relationships
              Tobita (1988), through introducing the modified stress tensor, derived a new yielding
              function. Tobita and Yanagisawa (1992) systematically introduced the modified stress
              tensor that is explicitly related to the fabric tensors. Cowin (1985, 1986) introduced the
              relationships between fabric tensors, elasticity tensor, and strength.
                 Oda and Nakayama (1989), through modifying the first and second stress invari-
              ants by the following equations, related the stress invariants with the particle orienta-
              tion tensor R ij defined with 2D datasets.

                                          −
                                          I = ( δ  + a R )σ                      (3-21)
                                              a
                                           1
                                               1  ij  2  ij  ij
                                       −
                                       J = 2(  b δδ  + 4 b R δ  ) S S            (3-22)
                                       2
                                             6  ik  jl  7  ik lj  ij kl
                 Where a 1 ,a 2  and b 6 ,b 7  are functions of the orientation tensor constant of R ij . S ij  is the
              deviatoric stress tensor.
                 The 3D non-destructive quantification of these fabric tensors provides a viable tool
              to verify these relations.
              Significances
              The quantification methods presented offer potential applications in characterizing the
              parameters needed in constitutive models that incorporate material microstructural
              quantities. They can also provide applications in correlating microstrutural quantities
              with anisotropic behavior of granular materials (or weakly bonded materials in discrete
              senses). More importantly, these methods place a foundation to better understand the
              deformation and strength mechanisms of granular materials on the basis of microme-
              chanics, microstructure, and statistics. A rational elasto-plasticity constitutive model
              based on the fabric description can be conceived to include 1) the anisotropic elasticity
              base on the anisotropic fabric distribution; 2) anisotropic yielding strength that is based
              on material properties and fabric distributions; and 3) non-associated flow.



        3.5  Microstructural Quantities in View of Damaged Continuum
              Another set of parameters is related to the general concept of damage or weakness in a
              broader sense. For example, from a pure mechanics point of view, voids will weaken
              the material due to the stress concentration. The interface between aggregates and
   87   88   89   90   91   92   93   94   95   96   97