2014
DOI: 10.1007/s00170-014-6536-6
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Scratching of copper with rough surfaces conducted by diamond tip simulated using molecular dynamics

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Cited by 32 publications
(9 citation statements)
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“…The cutting force was computed from F = i = 1 N j U ( r i j ) r i j $F \textrm{ } = \textrm{ } \sum_{i = 1}^{N} \underset{j}{\sum} \frac{\partial U \left(\right. r_{i j} \left.\right)}{r_{i j}}$ , [ 29–32 ] where U ( r i j ) $U \left(\right. r_{i j} \left.\right)$ is the potential energy, and r ij is the distance.…”
Section: Methodsmentioning
confidence: 99%
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“…The cutting force was computed from F = i = 1 N j U ( r i j ) r i j $F \textrm{ } = \textrm{ } \sum_{i = 1}^{N} \underset{j}{\sum} \frac{\partial U \left(\right. r_{i j} \left.\right)}{r_{i j}}$ , [ 29–32 ] where U ( r i j ) $U \left(\right. r_{i j} \left.\right)$ is the potential energy, and r ij is the distance.…”
Section: Methodsmentioning
confidence: 99%
“…[ 28 ] The initial workpiece temperature was chosen as 293 K. Meanwhile, the thermostat atoms temperature was kept at 293 K by the velocity‐rescaling approach over the MD‐machining process for achieving heat dissipation. The temperature was derived from T = i = 1 N m i v i 2 false/ 3 N k B $T = \langle\sum_{i = 1}^{N} m_{i} v_{i}^{2}\rangle/ 3 N k_{\text{B}}$ , [ 29–32 ] where k B is the Boltzmann constant, N is the number of atoms, m i is the mass of the i th atom, v i is the velocity of the i th atom, and is the statistical averaging over the entire simulation time. The cutting force was computed from F = i = 1 N j U ( r i j ) r i j $F \textrm{ } = \textrm{ } \sum_{i = 1}^{N} \underset{j}{\sum} \frac{\partial U \left(\right.…”
Section: Methodsmentioning
confidence: 99%
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“…Recently, this method has been effectively used to solve a wide variety of tasks at the atomic level concerned with single crystals. These studies were most often related to the study of the evolution of plastic deformation in crystals subjected to torsion [19], tension-compression [20][21][22][23][24][25][26], different surface impacts such as nanoindentation [27], scratching [12,[28][29][30], cutting [31][32][33], burnishing [34], etc. A. Dmitriev et al [35] performed simulation of uniaxial compression of FCC metal single crystals along the <001> direction and showed that the evolution of deformation relief and dislocation structure in these crystals is determined by their energetic characteristics, in particular, by the stacking fault energy (SFE).…”
Section: Introductionmentioning
confidence: 99%
“…The following are available online at , Figure S1: Evaluation of simulation box size: (a) the tangential forces for three models, and (b) the friction coefficient at three scratch depths; Figure S2: (a) Tangential force and normal force at the depth of 3.0 r 0 in three samples, and (b) the friction coefficient at different scratch depths. References [ 33 , 55 , 56 ] were cited in Supplementary Materials.…”
mentioning
confidence: 99%