Page 381 - Mechanics of Asphalt Microstructure and Micromechanics
P. 381

Simulation of  Asphalt Compaction   373


                          55

                                   Center
                          50       Joint Side
                                   Shoulder Side
                          Eα (MN/m)  45                           R =0.56
                        2


                                                                   2

                          40



                          35
                           88.0     90.0     92.0     94.0     96.0     98.0
                                        Percentage of TMD [CORE] (%)
              FIGURE 11.8  Stiffness versus density during breakdown rolling (Sakai).



              composite spheres model and the arbitrary phase geometry model, do not adequately
              describe the complex microstructure of asphalt mixture. Most micromechanical mod-
              els (Li et al. 1999; Papagiannakis et al., 2002; Li and Metcalf, 2005) may either over- or
              under-predict the stiffness (or modulus) of asphalt mixtures (Buttlar and You, 2001;
              Buttlar and Dave, 2005). This is primarily attributed to the inability of the models to
              account for the contribution of the aggregate interlock (i.e., lack of microstructure in
              the model) to the overall response of the mixture (You and Buttlar, 2004, 2005). Never-
              theless, these models may serve as the basis formula on which modifications may be
              developed to include experimental calibrations.
                 Evaluations of the mixture modulus from the modulus of the components and their
              volume fractions are quite often used in AC with the use of experimental calibrations.
              Tremendous work has been done in this area. From the rule of mixture, to Eshelby ten-
              sor, to computational assessments, these micromechanics models present tools to pre-
              dict the mixture properties for guiding mix design. A model that is popularly used in
              the AC area is the Hirsch model (Christensen et al., 2003; Chapter 5), which is actually
              the application of the rule of mixture. To avoid complicated formulas, this model basi-
              cally shows that the mixture modulus is a function of the aggregate modulus, binder
              modulus (or mastic modulus), their corresponding volume fractions, and voids in min-
              eral aggregate (VMA) and voids filled with asphalt (VFA).
                                            f E E VMA VFA)
                                        E = (,    ,    ,                         (11-5)
                                         c    a  b
                 E c , E a and E b are the mixture, aggregate, and binder modulus, respectively. It should
              be noted that VMA, VFA, V beffective  (effective volume of binder), and Va (air-void content)
              are related.
                 Therefore, the mixture modulus is related to air-void content. When air-void con-
              tent decreases, the mixture modulus increases. To a certain degree this model shows
              that the consolidation process will stiffen the mixture. It should be noted that E b , the
   376   377   378   379   380   381   382   383   384   385   386