Despite the crucial role of breakable particles in numerous natural processes and industrial applications, accurately simulating particle breakage and its distinct variants remains a significant challenge for realistic discrete element method (DEM) simulations. In this work, we employ the bonded cell method (BCM), in which the particle is modeled as an aggregate of polyhedral cells whose common surfaces obey the Griffith fracture criterion, to simulate the fracture behavior of a single particle impacting a rigid plane. We focus on the influence of the restitution coefficient of cohesive bonds between cells on the particle fracture regimes and dissipated energy. We find that the crossover values of the damage potential , separating the three fracture regimes, follow a power-law relationship with the intercell restitution coefficient. Interestingly, at low values of corresponding to the first regime, where the particle undergoes the elastic rebound without crack formation, the effective restitution coefficient is independent of the intercell restitution coefficient. Our simulation data also reveal that the evolution of normalized energy dissipated by contact inelasticity and friction is well captured by a power-law function of . In the fragmented state, the power-law exponent is approximately 1 and remains independent of the intercell restitution coefficient, implying a linear dependence between the dissipated energy and the supplied kinetic energy. We show that the fraction of supplied energy lost to inelastic and frictional dissipation increases from about 50% to nearly 95% as the intercell restitution coefficient decreases. In contrast, in the damaged state, the power-law exponent is greater than 1 and decreases with decreasing intercell restitution coefficient. Finally, the dependence of several physical variables such as particle damage and fracture efficiency on the intercell restitution coefficient and impact velocity is also investigated.
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