CONSTRUCTION OF ELLIPSOIDAL PARTICLE DISCRETE ELEMENT MODEL AND CALIBRATION OF SIMULATION PARAMETERS
类椭球形状颗粒离散元模型构建与仿真参数标定
DOI : https://doi.org/10.35633/inmateh-77-108
Authors
Abstract
To further optimize the simulation process of grass seed pellet coating, it is essential to construct an accurate geometric model of the seed particles. In this study, the discrete element method (DEM) was employed to model and analyze the particles with high precision, thereby improving the modeling efficiency and simulation accuracy for forage seeds. Ice grass seeds were selected as the research subject. A three-dimensional geometric model of the particles was constructed based on the hyperquadratic surface (hyperellipsoid) equation, which was then used as the mesh-generation domain for the DEM model. Subsequently, a standardized filling-sphere method tailored for ellipsoid-like particle geometries was proposed. Treating the ice grass seed as an axisymmetric ellipsoid, a maximum filling sphere with a diameter of 1.2 mm was placed at its center. Three multi-sphere models—17-sphere, 9-sphere, and 5-sphere—were developed using 0.25×, 0.5×, and 0.75× of the maximum filling sphere diameter, respectively. The diameter of each filling sphere corresponded to the largest inscribed sphere tangent to the ellipsoid surface. Through simulation experiments, a second-order regression equation for the static angle of repose was obtained. Based on the target static angle of repose (30.54°), parameter optimization was performed, yielding the optimal simulation parameters: a shear modulus of 1.9×10^7 Pa, a seed-to-seed coefficient of restitution of 0.5, and a maximum packing sphere diameter ratio of 0.35. The average simulated static angle of repose was 30.67°, with a relative error of 0.43%. Finally, a rotating drum test was conducted to calibrate the dynamic angle of repose. The drum was filled to 40% of its volume and rotated at 58 r/min. The physical experiment produced a dynamic angle of 38.46°, while the corresponding 10-second simulation yielded a dynamic angle of 38.12°, resulting in a relative error of 0.88% compared with the physical test. These results provide a reference for establishing discrete element models of ellipsoidal particles and support accurate simulations of seed pellet coating processes.
Abstract in Chinese



