Page 255 - The Combined Finite-Discrete Element Method
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238    TRANSITION FROM CONTINUA TO DISCONTINUA



























            Figure 7.6  Fracture sequence in 2D combined finite-discrete element simulation of bench blasting;
            the last picture shows an enlarged fracture pattern.


            is worth noting that the initial finite element mesh employed is a very coarse one. As
            the fracture pattern develops, the finite element mesh is refined to accommodate newly
            created boundaries (as previously described in this section), while the energy dissipation
            mechanisms due to strain softening are controlled in respect to the mesh size.
              A typical sequence for a muck-pile formation is shown in Figure 7.7. Initially, fractured
            rock forms an unstable column with individual rock blocks moving horizontally and
            accelerating downwards under gravity (self-weight). The bottom of the column collapses
            first, and this collapse is propagated toward the upper layers of rock. In the next stage the
            lower layers of rock decelerate due to confinement induced through boundaries, which
            results in contact interaction between rock fragments and intensive energy dissipation.






















                               Figure 7.7 Initial collapse of fractured rock.
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