Computational homogenization of material surfaces: From atomistic simulations to continuum models
[Display omitted] •A Ritz-type homogenization is employed to derive continuum surface properties.•The continuum model is matched with an atomistic model by energy equivalence.•Finite-element (FEAP) and molecular simulations (LAMMPS) are implemented.•Application is illustrated in the linear elastic r...
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Published in | Computational materials science Vol. 175; p. 109431 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
01.04.2020
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ISSN | 0927-0256 1879-0801 |
DOI | 10.1016/j.commatsci.2019.109431 |
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Abstract | [Display omitted]
•A Ritz-type homogenization is employed to derive continuum surface properties.•The continuum model is matched with an atomistic model by energy equivalence.•Finite-element (FEAP) and molecular simulations (LAMMPS) are implemented.•Application is illustrated in the linear elastic range of copper surfaces.•Dependence on strain, thickness and bulk approximation is reported and discussed.
The objective of this work is a numerical multiscale framework that determines mechanical continuum properties of material surfaces based on molecular statics. The key idea is the coupling of representative volume elements in the atomistic and in the continuum model by the principle of energy equivalence. This allows a thermodynamically consistent implementation of various material models and boundary conditions, e.g., to capture size effects in nano scale materials. For the present example of copper, we observe a very good match with literature data. Only the results for the surface stiffness still deviate in the same range as existing data sources do. The presented results concurrently indicate a drastic strain sensitivity. We further eliminate a methodological bulk to surface error propagation by an appropriate strain limit and thickness extrapolation. The latter is calculated by always allowing for fully developed surface regions. Additionally, our method reveals a strain dependence of higher order that is caused by the anharmonic potential and not captured by standard bulk models. The presented multiscale framework finally serves two purposes: validating the reasonableness of a material surface model and determining its parameters. |
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AbstractList | [Display omitted]
•A Ritz-type homogenization is employed to derive continuum surface properties.•The continuum model is matched with an atomistic model by energy equivalence.•Finite-element (FEAP) and molecular simulations (LAMMPS) are implemented.•Application is illustrated in the linear elastic range of copper surfaces.•Dependence on strain, thickness and bulk approximation is reported and discussed.
The objective of this work is a numerical multiscale framework that determines mechanical continuum properties of material surfaces based on molecular statics. The key idea is the coupling of representative volume elements in the atomistic and in the continuum model by the principle of energy equivalence. This allows a thermodynamically consistent implementation of various material models and boundary conditions, e.g., to capture size effects in nano scale materials. For the present example of copper, we observe a very good match with literature data. Only the results for the surface stiffness still deviate in the same range as existing data sources do. The presented results concurrently indicate a drastic strain sensitivity. We further eliminate a methodological bulk to surface error propagation by an appropriate strain limit and thickness extrapolation. The latter is calculated by always allowing for fully developed surface regions. Additionally, our method reveals a strain dependence of higher order that is caused by the anharmonic potential and not captured by standard bulk models. The presented multiscale framework finally serves two purposes: validating the reasonableness of a material surface model and determining its parameters. |
ArticleNumber | 109431 |
Author | Kurzeja, Patrick Sievers, Christian Mosler, Jörn Brendel, Lothar |
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Cites_doi | 10.1006/jcph.1995.1039 10.1016/j.actamat.2006.08.007 10.1016/j.jmps.2005.08.010 10.1103/PhysRevB.71.094104 10.1016/S0020-7683(03)00346-9 10.1093/qjmam/43.1.15 10.1103/PhysRevB.28.1835 10.1063/1.3253150 10.1016/j.cma.2018.03.023 10.1016/j.ijsolstr.2003.07.001 10.1103/PhysRevLett.85.622 10.1016/j.jmps.2011.04.012 10.1016/j.ijsolstr.2010.12.018 10.1002/nme.4465 10.1103/PhysRev.144.411 10.1007/s10035-015-0555-3 10.1051/m2an:2007018 10.1103/PhysRevB.71.241403 10.1103/PhysRevB.29.6443 10.1093/comjnl/7.4.308 10.1177/1081286517699041 10.1557/JMR.1988.0471 |
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