2020
DOI: 10.1007/s00603-020-02047-w
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Non-parameterized Numerical Analysis Using the Distinct Lattice Spring Model by Implementing the Duncan–Chang Model

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Cited by 17 publications
(6 citation statements)
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“…In a previous study by Zhao et al., 29 the multibody failure criterion based on the modified Mohr–Coulomb model was implemented into 4D‐LSM to address the low ratio of uniaxial compressive strength (UCS) to uniaxial tensile strength (UTS) encountered in the conventional DEM, which is an important indicator for rock‐like materials. In this criterion, the multibody stress state was determined by the introduction of fiber stress, whose validity was demonstrated by Zhao et al 32 . in the DLSM, and the formula takes the form of: σijIbadbreak=12VIfinijl0\begin{equation}\sigma _{ij}^I = \frac{1}{{2{V}^I}}\sum {{f}_i{n}_{ij}{l}_0} \end{equation}where σijI$\sigma _{ij}^I$ and VI${V}^I$ are the stress tensor and the representative volume of particle I , fi${f}_i$, nij${n}_{ij}$, and l 0 are the total bond force, normal unit vector, and initial spring length among particle I and its neighbor particles, respectively.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…In a previous study by Zhao et al., 29 the multibody failure criterion based on the modified Mohr–Coulomb model was implemented into 4D‐LSM to address the low ratio of uniaxial compressive strength (UCS) to uniaxial tensile strength (UTS) encountered in the conventional DEM, which is an important indicator for rock‐like materials. In this criterion, the multibody stress state was determined by the introduction of fiber stress, whose validity was demonstrated by Zhao et al 32 . in the DLSM, and the formula takes the form of: σijIbadbreak=12VIfinijl0\begin{equation}\sigma _{ij}^I = \frac{1}{{2{V}^I}}\sum {{f}_i{n}_{ij}{l}_0} \end{equation}where σijI$\sigma _{ij}^I$ and VI${V}^I$ are the stress tensor and the representative volume of particle I , fi${f}_i$, nij${n}_{ij}$, and l 0 are the total bond force, normal unit vector, and initial spring length among particle I and its neighbor particles, respectively.…”
Section: Methodsmentioning
confidence: 99%
“…In a previous study by Zhao et al, 29 the multibody failure criterion based on the modified Mohr-Coulomb model was implemented into 4D-LSM to address the low ratio of uniaxial compressive strength (UCS) to uniaxial tensile strength (UTS) encountered in the conventional DEM, which is an important indicator for rock-like materials. In this criterion, the multibody stress state was determined by the introduction of fiber stress, whose validity was demonstrated by Zhao et al 32 in the DLSM, and the formula takes the form of:…”
Section: D-lsm With a Multibody Failure Criterionmentioning
confidence: 99%
“…As the negative impact of freeze-thaw cycles intensifies, the cohesion does not continue to increase and reaches a stable state. The Duncan-Chang (DC) model is widely used in theoretical calculations and engineering guidance models (Zhao G. F. et al, 2020), and its formula is:…”
Section: Strength and Parameter Analysis Of Artificially Frozen Silty...mentioning
confidence: 99%
“…The DC model is a nonlinear elastic model (Zhao G. F. et al, 2020). It can be directly obtained from triaxial tests.…”
Section: Introductionmentioning
confidence: 99%
“…The Zienkiewicz-Pande (ZP) model was further developed and used to analyze foundation deformations in a real project [24]. The Duncan-Chang (DC) nonlinear elastic model was also incorporated into the DLSM to simulate dam deformations during multiple construction stages, and a non-parametric numerical analysis was proposed to minimize human error [25].…”
mentioning
confidence: 99%