Page 408 - Mechanics of Asphalt Microstructure and Micromechanics
P. 408

T
   400   Ch a p t e r w e l v e



                                                                  z 0
                                                                        x or r
                        Layer 1        0                h 1
                                                                  z 1

                                                                  z k-1
                        …
                        Layer k                        h k
                                                                  z k


                        …
                                                                   z p-1
                        Layer p                        h p


                                                                    z p
                                      z
              FIGURE 12.5  Illustration of the multiple layered system (courtesy Ernie Pan).


                    u(, , ) =  u  e +  u  e +  u  e
                      xyz
                              xx   y y  z z
                      +∞ +∞  ⎡ ⎡ ⎧ ⎪  S ∂  S ∂ ⎤  ⎡          ∂ ⎤          ⎫ ⎪    (12-7)
                    =    ⎢ ⎨ ∫ ∫  U  M ()  +Uz  ⎥ x  + U () ∂S  −Uz ()  S ⎥ e y  +Uz()Se ⎬ αβ
                                           e
                                     ()
                             z
                                                                           d d
                                              ⎢
                                                  z
                                                                        S
                                                                     L
                                                         N
                                                 M
                                                                          z
                                    N
                      −∞ −∞  ⎣ ⎩ ⎪  x ∂  y ∂  ⎦  ⎣  ∂y       ∂x ⎦         ⎭ ⎪
                     t(, , ) = σ  e +σ  e +σ  e
                      xyz
                               xz x  yz y  zz z
                       +∞ +∞  ⎡ ⎧ ⎪  S ∂  ∂S⎤  ⎡     S ∂     S ∂ ⎤       ⎫ ⎪     (12-8)
                     =     ⎢ ⎨ ∫ ∫  Tz  x ∂  + Tz  S ⎥ e x  +  ⎢ Tz ()  y ∂  − Tz ()  x ∂  ⎥ e  y  +  T (()zSe ⎬ αβ
                              ()
                                      ()
                                                                          d d
                                         y ∂
                                                                         z
                                                                    L
                                                         N
                            M
                                     N
                                                 M
                       −∞ −∞  ⎣ ⎩ ⎪       ⎦    ⎣               ⎦         ⎭ ⎪
                 Finally, through the propagator matrix method, they solved for the stress, strain, and
              displacement fields under various loading and boundary conditions. A program (Mul-
              tiSmart3D) has also been developed by this group to allow convenient computation of the
              stress, strain, and displacement fields. Through Laplace transform, the analytical solu-
              tions have been further derived for the corresponding viscoleastic materials (Chen et al.,
              2009). Pan’s work placed a foundation for considering the anisotropic material properties
              in the flexible layered pavement design.
        12.6  Characterization of the Anisotropic Properties
              Using a True Triaxial Testing Device
              12.6.1 General State
              While significant efforts have been devoted to the study of the fundamental properties
              of soils, limited efforts have been devoted to AC. Properties such as stress path depen-
              dency, anisotropy, yielding, plastic deformation rates, etc. are barely studied in AC.
   403   404   405   406   407   408   409   410   411   412   413