Page 102 - MODELING OF ASPHALT CONCRETE
P. 102

80    Cha pte r  T h ree


                    method (Schapery 1962, 1965). Because there are different methods of estimating the
                    bulk and shear moduli of elastic composite, it is usually necessary to verify that the
                    conversion produces reliable results by comparison with actual measurements made
                    on the composite. A similar transformation can be used to convert the complex moduli
                    of the components into the effective complex moduli of the composite. In this way, the
                    formula for the elastic bulk modulus of the composite is converted into the formula for
                    the complex bulk modulus of the composite as in Eq. (3-13) (Christensen 1991).
                                        K −  K  *        4 G +  3 K *
                                                           *
                                          *
                                              m  =  c      m     m                      (3-13)
                                        K −  K  *  i  4 [  G + 3 K + 3( K −  Kc)]
                                                                     *
                                                                *
                                                           *
                                                      *
                                          *
                                          i   m       m    i    m m  i  i
                    The K and G terms with the asterisks in this equation are the complex bulk and shear
                    modulus of the matrix and the inclusion, all of which have a real and an imaginary
                    component as in Eqs. (3-14a), (3-14b), and (3-14c) (Christensen 1991):
                                                               ′′
                                              K ()ω = ′      i K ()ω                   (3-14a)
                                                *
                                                     K ()ω +
                                                m      m       m
                                               K ()ω = ′    i K ()ω                    (3-14b)
                                                              ′′
                                                *
                                                      K ()ω +
                                                i      i      i
                                              G ()ω = ′ m    i G ()ω                   (3-14c)
                                                               ′′
                                                *
                                                     G ()ω +
                                                m
                                                               m
                    If the material is nonlinear viscoelastic, the equations given above must be treated as
                    approximations, but they provide correct forms of equations that take into account the
                    strain-energy storage of each of the components of the composite material.
                    Effects of Microcracks on Stiffness
                    Because of the ability to use the correspondence principle to convert elastic solutions
                    into viscoelastic equations for asphalt concrete stiffness, it is possible to derive relations
                    using elastic theory with the confidence that they can be converted into the appropriate
                    viscoelastic form, either the creep compliance, the relaxation modulus, the complex
                    compliance, or the complex modulus. When a repeated load test is made on an asphalt
                    concrete, its stiffness appears to decrease with increasing numbers of load applications.
                    However, what is really happening is that small microcracks are forming in the material,
                    producing an apparently smaller modulus. This is illustrated in Fig. 3-8 with two straps
                    being subjected to the same tensile stress.
                                                   Microcrack size
                                              Actual          Apparent
                                               E                E′

                                               2 c




                                                    Same stretch
                                                      E′ < E

                    FIGURE 3-8  Effect of microcrack size on apparent modulus.
   97   98   99   100   101   102   103   104   105   106   107