2018
DOI: 10.1007/978-3-319-90155-8_4
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Contact Modeling in the Discrete Element Method

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Cited by 5 publications
(4 citation statements)
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“…We also assumed that there was no chemical reaction during the condensation and self‐organization, and thus adopted the linear (Hookean) contact model for simulation. [ 30 ] The overlap between particles is allowed and the bonding forces are expressed as a potential function of the overlap V ij = k n [δ ij ] 2 /2 ( k n is the normal spring stiffness). [ 31 ] The simulation was performed in the canonical NVT ensemble (that is, the number N , the volume V , and the temperature T remain constant) with the target temperature of 2000 K (close to the melting point of titanium) at the bottom of the orthorhombic simulation cell, using the large‐scale atomic/molecular massively parallel simulator (LAMMPS) package.…”
Section: Resultsmentioning
confidence: 99%
“…We also assumed that there was no chemical reaction during the condensation and self‐organization, and thus adopted the linear (Hookean) contact model for simulation. [ 30 ] The overlap between particles is allowed and the bonding forces are expressed as a potential function of the overlap V ij = k n [δ ij ] 2 /2 ( k n is the normal spring stiffness). [ 31 ] The simulation was performed in the canonical NVT ensemble (that is, the number N , the volume V , and the temperature T remain constant) with the target temperature of 2000 K (close to the melting point of titanium) at the bottom of the orthorhombic simulation cell, using the large‐scale atomic/molecular massively parallel simulator (LAMMPS) package.…”
Section: Resultsmentioning
confidence: 99%
“…This study does not go into great depth on the various contact models and their related equations. Rojek [27] and Thakur [28] summarize the many contact models that are used in discrete particle simulations. In their works, O'Sullivan [29] and Thornton [30] go into deep details on contact models.…”
Section: Dem's Theoretical Backgroundmentioning
confidence: 99%
“…To solve (1), we use explicit time integration scheme described in Rojek [12]. We use the acceleration of the elements from the previous time step to calculate the internal contact and damping forces, which allows us to calculate the acceleration in the current time step,…”
Section: Equation Of Motionmentioning
confidence: 99%
“…For each type of mesh, using the least squares method, we obtain the coefficients for (12) To prove theory from F. Camborde mentioned at beginning of this section, we going to analyse fixed beam using mesh type 2 with approximated λ as 0.715, see Tab.2. Results going to be compared with FEM solution by software ANSYS [19].…”
Section: Calibration Of λ Coefficientmentioning
confidence: 99%