With the widespread adoption of electronic detonators and strengthened safety regulations, millisecond level delay design has become feasible. Nevertheless, field practice still relies largely on empirical settings, and traditional formulas such as th...
With the widespread adoption of electronic detonators and strengthened safety regulations, millisecond level delay design has become feasible. Nevertheless, field practice still relies largely on empirical settings, and traditional formulas such as the Langefors equation, which were developed under the large timing scatter of legacy detonators, do not adequately reflect the timing precision of modern electronic initiation or the mechanisms governing stress wave interference and crack connectivity in rock. Consequently, it remains difficult to achieve a consistent balance between fragmentation quality and environmental performance across varying rock conditions and scales, and the physical basis for selecting delay times is often unclear. This study treats inter-hole delay as a controllable variable in the fracture process and proposes a mechanistic framework for interpreting and predicting fragmentation responses through the coupled interaction among stress waves, cracks, and blast gas pressure. In addition, fragmentation trends are analyzed as a function of delay time normalized by burden, Δt/B (ms/m), and reference criteria for field application are discussed.
A two-hole PMMA model experiment was first conducted to characterize the time history and representative time scale of crack development, and these observations were used to validate the time scale and crack reproduction of the numerical model. A bench scale three dimensional FDEM model was then developed and coupled with a gas zone model so that gas pressure acts selectively only on crack surfaces that are open and connected to the charge hole. Using this coupled framework, the analysis clarifies how inter-hole delay changes the development of connected and opened fracture paths between holes and the effectiveness of gas pressure action along those paths, and how these changes translate into differences in fragmentation metrics. In the three-hole comparison, simultaneous initiation produced dispersed crack trajectories and distributed gas pressure action, leading to coarser and more heterogeneous fragmentation, with Xmax =1.48 m, D50 =302.6 mm, and a uniformity index n =1.24. With a 5 ms delay, alignment between the growth of cracks formed by the leading hole and the arrival of the shock wave from the subsequent hole promoted early establishment of connected and open pathways, yielding Xmax =1.10 m, D50 =160 mm, and n =2.28, indicating suppression of oversize fragments and improved uniformity. A 10 ms delay showed the most pronounced improvement, with Xmax =0.55 m, D50 =146.4 mm, and n =2.43. As delay time increased, both Xmax and D50 decreased sharply over an initial range and then more gradually, implying that fragmentation enhancement is most strongly expressed within a specific range of Δt/B, beyond which sensitivity to further increases in delay diminishes.