2023
DOI: 10.1016/j.compgeo.2023.105708
|View full text |Cite
|
Sign up to set email alerts
|

Coupled material point and level set methods for simulating soils interacting with rigid objects with complex geometry

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

1
13
0

Year Published

2023
2023
2025
2025

Publication Types

Select...
5

Relationship

1
4

Authors

Journals

citations
Cited by 12 publications
(14 citation statements)
references
References 44 publications
1
13
0
Order By: Relevance
“…From the above illustration, the key to the F‐bar approach is to determine the averaged Jacobian normalΔtrueJ¯$\Delta \bar{J}$ in Equation (15). Departing from the research conducted by Zhao et al., 28 we calculate the averaged Jacobian normalΔtrueJ¯$\Delta \bar{J}$ by mapping the original one normalΔJ$\Delta {J}$ to the related grid nodes and then mapping back to the material points. The mathematical formulation of this mapping and remapping procedure is stated as follows: The nodal mass‐weighted Jacobian can be calculated by mapping the product of mass and normalΔJ$\Delta {J}$ from material points as false(mnormalΔJfalse)Ibadbreak=p=1npNIpmpnormalΔJ,$$\begin{equation} (m\Delta {J})_I = \sum _{p=1}^{{n}_{p}} {N}_{Ip} {m}_{p} \Delta {J}, \end{equation}$$where mp${m}_{p}$ is the mass of material point p ; (mΔJ)I$(m\Delta {J})_I$ is the nodal mass‐weighted Jacobian. Then, the nodal Jacobian can be obtained by normalΔJIbadbreak=(mΔJ)ImI,$$\begin{equation} \Delta {J}_I = \frac{(m\Delta {J})_I}{m_I}, \end{equation}$$where mI=p=1npNIpmp${m_I} = \sum _{p=1}^{{n}_{p}} {N}_{Ip} {m_p}$ is the nodal mass. Finally, the nodal Jacobian is mapped back to the ...…”
Section: Description Of the Numerical Modelmentioning
confidence: 99%
See 4 more Smart Citations
“…From the above illustration, the key to the F‐bar approach is to determine the averaged Jacobian normalΔtrueJ¯$\Delta \bar{J}$ in Equation (15). Departing from the research conducted by Zhao et al., 28 we calculate the averaged Jacobian normalΔtrueJ¯$\Delta \bar{J}$ by mapping the original one normalΔJ$\Delta {J}$ to the related grid nodes and then mapping back to the material points. The mathematical formulation of this mapping and remapping procedure is stated as follows: The nodal mass‐weighted Jacobian can be calculated by mapping the product of mass and normalΔJ$\Delta {J}$ from material points as false(mnormalΔJfalse)Ibadbreak=p=1npNIpmpnormalΔJ,$$\begin{equation} (m\Delta {J})_I = \sum _{p=1}^{{n}_{p}} {N}_{Ip} {m}_{p} \Delta {J}, \end{equation}$$where mp${m}_{p}$ is the mass of material point p ; (mΔJ)I$(m\Delta {J})_I$ is the nodal mass‐weighted Jacobian. Then, the nodal Jacobian can be obtained by normalΔJIbadbreak=(mΔJ)ImI,$$\begin{equation} \Delta {J}_I = \frac{(m\Delta {J})_I}{m_I}, \end{equation}$$where mI=p=1npNIpmp${m_I} = \sum _{p=1}^{{n}_{p}} {N}_{Ip} {m_p}$ is the nodal mass. Finally, the nodal Jacobian is mapped back to the ...…”
Section: Description Of the Numerical Modelmentioning
confidence: 99%
“…The BSMPM shows less volumetric locking than the MPMs with linear shape functions. However, fully overcoming the volumetric locking for BSMPM is challenging since its shape functions are associated with adjacent cells 28 . Navas et al 29 .…”
Section: Introduction and Literature Reviewmentioning
confidence: 99%
See 3 more Smart Citations