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Research Article

Engineering size-scaling of plastic deformation in nanoscale asperities

D. K. Ward, D. Farkas, J. Lian, W. A. Curtin, J. Wang, K.-S. Kim, and Y. Qi
PNAS June 16, 2009 106 (24) 9580-9585; https://doi.org/10.1073/pnas.0900804106
D. K. Ward
aDivision of Engineering, Brown University, Providence, RI 02912;
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  • For correspondence: dward@cavs.msstate.edu
D. Farkas
bDepartment of Materials Science and Engineering, Virginia Polytechnic Institute and State University, Blacksburg, VA 24061-023; and
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J. Lian
cDepartment of Mechanical Engineering, University of Washington, Seattle, WA 98195;
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W. A. Curtin
aDivision of Engineering, Brown University, Providence, RI 02912;
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J. Wang
cDepartment of Mechanical Engineering, University of Washington, Seattle, WA 98195;
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K.-S. Kim
aDivision of Engineering, Brown University, Providence, RI 02912;
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Y. Qi
dGeneral Motors R&D Center, 30500 Mound Road, Warren, MI 48090-9055
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  1. Edited by William D. Nix, Stanford University, Stanford, CA, and approved March 24, 2009 (received for review January 27, 2009)

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Abstract

Size-dependent plastic flow behavior is manifested in nanoindentation, microbending, and pillar-compression experiments and plays a key role in the contact mechanics and friction of rough surfaces. Recent experiments using a hard flat plate to compress single-crystal Au nano-pyramids and others using a Berkovich indenter to indent flat thin films show size scaling into the 100-nm range where existing mechanistic models are not expected to apply. To bridge the gap between single-dislocation nucleation at the 1-nm scale and dislocation-ensemble plasticity at the 1-μm scale, we use large-scale molecular dynamics (MD) simulations to predict the magnitude and scaling of hardness H versus contact size ℓc in nano-pyramids. Two major results emerge: a regime of near-power-law size scaling H ≈ ℓc−η exists, with ηMD ≈ 0.32 compared with ηexpt ≈ 0.75, and unprecedented quantitative and qualitative agreement between MD and experiments is achieved, with HMD ≈ 4 GPa at ℓc = 36 nm and Hexpt ≈ 2.5 GPa at ℓc = 100 nm. An analytic model, incorporating the energy costs of forming the geometrically necessary dislocation structures that accommodate the deformation, is developed and captures the unique magnitude and size scaling of the hardness at larger MD sizes and up to experimental scales while rationalizing the transition in scaling between MD and experimental scales. The model suggests that dislocation–dislocation interactions dominate at larger scales, whereas the behavior at the smallest MD scales is controlled by nucleation over energy barriers. These results provide a basic framework for understanding and predicting size-dependent plasticity in nanoscale asperities under contact conditions in realistic engineered surfaces.

  • atomistics
  • dislocation interactions
  • plasticity
  • size-effects
  • surfaces

Footnotes

  • ↵1To whom correspondence should be addressed at: Center for Advanced Vehicular Systems, Box 5405, Mississippi State University, Mississippi State, MS 39762-5404. E-mail: dward{at}cavs.msstate.edu
  • Author contributions: D.K.W., D.F., W.A.C., J.W., K.-S.K., and Y.Q. designed research; D.K.W., J.L., and J.W. performed research; D.K.W., W.A.C., and K.-S.K. contributed new reagents/analytic tools; D.K.W., J.L., and W.A.C. analyzed data; and D.K.W. and W.A.C. wrote the paper.

  • The authors declare no conflict of interest.

  • This article is a PNAS Direct Submission.

  • Received January 27, 2009.
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Engineering size-scaling of plastic deformation in nanoscale asperities
D. K. Ward, D. Farkas, J. Lian, W. A. Curtin, J. Wang, K.-S. Kim, Y. Qi
Proceedings of the National Academy of Sciences Jun 2009, 106 (24) 9580-9585; DOI: 10.1073/pnas.0900804106

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Engineering size-scaling of plastic deformation in nanoscale asperities
D. K. Ward, D. Farkas, J. Lian, W. A. Curtin, J. Wang, K.-S. Kim, Y. Qi
Proceedings of the National Academy of Sciences Jun 2009, 106 (24) 9580-9585; DOI: 10.1073/pnas.0900804106
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Proceedings of the National Academy of Sciences: 106 (24)
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