TY - JOUR
T1 - Numerical simulation on seismic response of the filled joint under high amplitude stress waves using Finite-Discrete Element Method (FDEM)
AU - Huang, Xiaolin
AU - Zhao, Qi
AU - Qi, Shengwen
AU - Xia, Kaiwen
AU - Grasselli, Giovanni
AU - Chen, Xuguang
N1 - Funding Information:
The author would like to give great thanks to Grasselli's geomechanics group for providing the FDEM code. This research is supported by the National Science Foundation of China under grants of No. 41322020, 41302234, and 41672307, the Chinese Academy of Science under Grants No. KZZD-EW-05-02 and KFJ-EW-STS-094, and General Financial Grant from the China Postdoctoral Science Foundation No. 2016M600129 and No. 2015M581167.
Publisher Copyright:
© 2017 by the authors.
Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 2017
Y1 - 2017
N2 - This paper numerically investigates the seismic response of the filled joint under high amplitude stress waves using the combined finite-discrete element method (FDEM). A thin layer of independent polygonal particles are used to simulate the joint fillings. Each particle is meshed using the Delaunay triangulation scheme and can be crushed when the load exceeds its strength. The propagation of the 1D longitude wave through a single filled joint is studied, considering the influences of the joint thickness and the characteristics of the incident wave, such as the amplitude and frequency. The results show that the filled particles under high amplitude stress waves mainly experience three deformation stages: (i) initial compaction stage; (ii) crushing stage; and (iii) crushing and compaction stage. In the initial compaction stage and crushing and compaction stage, compaction dominates the mechanical behavior of the joint, and the particle area distribution curve varies little. In these stages, the transmission coefficient increases with the increase of the amplitude, i.e., peak particle velocity (PPV), of the incident wave. On the other hand, in the crushing stage, particle crushing plays the dominant role. The particle size distribution curve changes abruptly with the PPV due to the fragments created by the crushing process. This process consumes part of wave energy and reduces the stiffness of the filled joint. The transmission coefficient decreases with increasing PPV in this stage because of the increased amount of energy consumed by crushing. Moreover, with the increase of the frequency of the incident wave, the transmission coefficient decreases and fewer particles can be crushed. Under the same incident wave, the transmission coefficient decreases when the filled thickness increases and the filled particles become more difficult to be crushed.
AB - This paper numerically investigates the seismic response of the filled joint under high amplitude stress waves using the combined finite-discrete element method (FDEM). A thin layer of independent polygonal particles are used to simulate the joint fillings. Each particle is meshed using the Delaunay triangulation scheme and can be crushed when the load exceeds its strength. The propagation of the 1D longitude wave through a single filled joint is studied, considering the influences of the joint thickness and the characteristics of the incident wave, such as the amplitude and frequency. The results show that the filled particles under high amplitude stress waves mainly experience three deformation stages: (i) initial compaction stage; (ii) crushing stage; and (iii) crushing and compaction stage. In the initial compaction stage and crushing and compaction stage, compaction dominates the mechanical behavior of the joint, and the particle area distribution curve varies little. In these stages, the transmission coefficient increases with the increase of the amplitude, i.e., peak particle velocity (PPV), of the incident wave. On the other hand, in the crushing stage, particle crushing plays the dominant role. The particle size distribution curve changes abruptly with the PPV due to the fragments created by the crushing process. This process consumes part of wave energy and reduces the stiffness of the filled joint. The transmission coefficient decreases with increasing PPV in this stage because of the increased amount of energy consumed by crushing. Moreover, with the increase of the frequency of the incident wave, the transmission coefficient decreases and fewer particles can be crushed. Under the same incident wave, the transmission coefficient decreases when the filled thickness increases and the filled particles become more difficult to be crushed.
KW - Amplitude attenuation
KW - FDEM
KW - Filled joint
KW - Grain size reduction
KW - High amplitude stress wave
KW - Particle crushing
UR - http://www.scopus.com/inward/record.url?scp=85011685060&partnerID=8YFLogxK
U2 - 10.3390/ma10010013
DO - 10.3390/ma10010013
M3 - Journal article
AN - SCOPUS:85011685060
SN - 1996-1944
VL - 10
JO - Materials
JF - Materials
IS - 1
M1 - 13
ER -