TY - JOUR
T1 - Enhanced flow rate by the concentration mechanism of Tetris particles when discharged from a hopper with an obstacle
AU - Gao, Guo-Jie Jason
AU - Yang, Fu-Ling
AU - Holcomb, Michael
AU - Blawzdziewicz, Jerzy
N1 - Funding Information:
We thank Corey S. O'Hern for useful discussions. We also thank the reviewers for helpful comments. G.J.G. acknowledges financial support from National Taiwan University funding 104R7417, MOST Grant No. 104-2218-E-002-019 from Ministry of Science and Technology (Taiwan), and the computational facility made available by the startup funding of Shizuoka University (Japan). F.-L.Y. acknowledges MOST Grant No. 109-2628-E-002-002-MY3 from Ministry of Science and Technology (Taiwan). M.C.H. acknowledges startup funding from Angelo State University (USA). J.B. was supported by NSF Grant No. CBET-1603627 (USA).
Publisher Copyright:
© 2021 American Physical Society.
PY - 2021/6
Y1 - 2021/6
N2 - We apply a holistic two-dimensional (2D) Tetris-like model, where particles move based on prescribed rules, to investigate the flow rate enhancement from a hopper. This phenomenon was originally reported in the literature as a feature of placing an obstacle at an optimal location near the exit of a hopper discharging athermal granular particles under gravity. We find that this phenomenon is limited to a system of sufficiently many particles. In addition to the waiting room effect, another mechanism able to explain and create the flow rate enhancement is the concentration mechanism of particles on their way to reaching the hopper exit after passing the obstacle. We elucidate the concentration mechanism by decomposing the flow rate into its constituent variables: the local area packing fraction φlE and the averaged particle velocity vyE at the hopper exit. In comparison to the case without an obstacle, our results show that an optimally placed obstacle can create a net flow rate enhancement of relatively weakly driven particles, caused by the exit-bottleneck coupling if φlE>φoc, where φoc is a characteristic area packing fraction marking a transition from fast to slow flow regimes of Tetris particles. Utilizing the concentration mechanism by artificially guiding particles into the central sparse space under the obstacle or narrowing the hopper exit angle under the obstacle, we can create a manmade flow rate peak of relatively strongly driven particles that initially exhibit no flow rate peak. Additionally, the enhanced flow rate can be maximized by an optimal obstacle shape, particle acceleration rate toward the hopper exit, or exit geometry of the hopper.
AB - We apply a holistic two-dimensional (2D) Tetris-like model, where particles move based on prescribed rules, to investigate the flow rate enhancement from a hopper. This phenomenon was originally reported in the literature as a feature of placing an obstacle at an optimal location near the exit of a hopper discharging athermal granular particles under gravity. We find that this phenomenon is limited to a system of sufficiently many particles. In addition to the waiting room effect, another mechanism able to explain and create the flow rate enhancement is the concentration mechanism of particles on their way to reaching the hopper exit after passing the obstacle. We elucidate the concentration mechanism by decomposing the flow rate into its constituent variables: the local area packing fraction φlE and the averaged particle velocity vyE at the hopper exit. In comparison to the case without an obstacle, our results show that an optimally placed obstacle can create a net flow rate enhancement of relatively weakly driven particles, caused by the exit-bottleneck coupling if φlE>φoc, where φoc is a characteristic area packing fraction marking a transition from fast to slow flow regimes of Tetris particles. Utilizing the concentration mechanism by artificially guiding particles into the central sparse space under the obstacle or narrowing the hopper exit angle under the obstacle, we can create a manmade flow rate peak of relatively strongly driven particles that initially exhibit no flow rate peak. Additionally, the enhanced flow rate can be maximized by an optimal obstacle shape, particle acceleration rate toward the hopper exit, or exit geometry of the hopper.
UR - http://www.scopus.com/inward/record.url?scp=85108543557&partnerID=8YFLogxK
U2 - 10.1103/PhysRevE.103.062904
DO - 10.1103/PhysRevE.103.062904
M3 - Article
C2 - 34271757
SN - 2470-0045
VL - 103
JO - Physical Review E
JF - Physical Review E
IS - 6
M1 - 062904
ER -