Page 287 - The Combined Finite-Discrete Element Method
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270    FLUID COUPLING


                                               Permeable edge

                                                            x
                                                             d j    d
                                                        Γ
                               Bore-hole










                        Figure 8.5  Gas zone with individual cracks of variable opening.



            The length of individual ducts l is defined as the average length from the borehole to the
            permeable wall of the gas zone, i.e.


                                                  xdϕ
                                                 S
                                            l =                                  (8.47)
                                                   dϕ
                                                 S
            where x is the distance from the borehole to the permeable edge and S is the perme-
            able edge.
              The total number of ducts is thus given as


                                                   d

                                            A =                                  (8.48)
                                                   l


            8.4 COUPLED COMBINED FINITE-DISCRETE ELEMENT SIMULATION
                  OF EXPLOSIVE INDUCED FRACTURE AND FRAGMENTATION

            The equation of state for the detonation gas together with the gas flow model complement
            other numerical algorithms comprising the combined finite-discrete element simulation.
            To demonstrate the combined finite-discrete element simulation coupled with gas flow
            through cracks, simulation of explosive induced fragmentation of a 2 × 2 m square block
            shown in Figure 8.6 is performed. The thickness (depth) of the block is 0.1 m. Initially,
            the block has a continuous cut from the centre to the top end. The ignition of the explosive
            charge takes place at the bottom of the cut, and propagates toward the top of the cut at a
            VOD of 7580 m/s.
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