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Research Article

An interpretation of size-scale plasticity in geometrically confined systems

H. D. Espinosa, S. Berbenni, M. Panico, and K. W. Schwarz
  1. *Department of Mechanical Engineering, Northwestern University, 2145 Sheridan Road, Evanston, IL 60208-3111; and §IBM Watson Research Center, Yorktown Heights, NY 10598

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PNAS November 22, 2005 102 (47) 16933-16938; https://doi.org/10.1073/pnas.0508572102
H. D. Espinosa
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S. Berbenni
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M. Panico
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K. W. Schwarz
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  1. Communicated by Zdenek P. Bazant, Northwestern University, Evanston, IL, October 3, 2005 (received for review April 19, 2005)

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    Fig. 1.

    Self-similar experiments in pure tension Cu films. Comparison between the mechanical response of submicronic ultrafine-grained thin films (MDE) and millimeter-thick coarse-grained films (Fullam tensile stage).

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    Fig. 2.

    TEM and SEM observations on MDE-tested Au films. (a and b) Study of the plastic activity of 0.3-μm-thick Au films (a) (SEM picture showing the fracture surface) and 1-μm-thick Au films (b) (SEM picture showing large deformation slip bands close to the fracture edge). (c) Cross-sectional TEM view of fracture region. (d) High-aspect-ratio grain exhibiting dislocation network.

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    Fig. 3.

    Problem definition for DDD calculations. (a) Columnar grains simulating by rectangular boxes with various heights. (b) Present study: single crystal (grain) considered as a rectangular box [thickness: h; grain size: d with a crystallographic direction Embedded Image perpendicular to the film plane (consistent with the strong 〈111 〉 texture of the film) and with an applied tensile loading parallel to the 〈112 〉 direction (arbitrary)]. The sides are impenetrable to simulate grain boundaries, and the top and bottom faces are attractive to represent free surfaces.

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    Fig. 4.

    Thickness effect obtained by DDD calculations for different thicknesses (h = 0.2, 0.4, 0.6, and 1 μm) considering a freestanding columnar grain. The error bars represent the statistical scatter of different runs at the end of the simulation for each sample. (a) Source density = 2.4 × 104 per cm. (b) Source density = 0.8 × 104 per cm.

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    Fig. 5.

    Final dislocation configurations for an applied strain of 0.8% [top view (Left), 3D view (Right)]. (a) 0.2-μm sample. (b) 0.6-μm sample. (c) 1-μm sample.

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    Fig. 6.

    Flow stress (defined as the stress corresponding to 0.2% permanent deformation upon elastic unloading) as a function of film thickness inverse.

Data supplements

  • Espinosa et al. 10.1073/pnas.0508572102.

    Supporting Movies

    Files in this Data Supplement:

    Supporting Movie 1
    Supporting Movie 2
    Supporting Movie 3
    Supporting Movie 4
    Supporting Movie 5




    Supporting Movie 1

    Movie 1. Microstructure evolution recorded by optical imaging.





    Supporting Movie 2

    Movie 2. Local strain fields obtained by digital image correlation.





    Supporting Movie 3

    Movie 3. Discrete dislocation plasticity simulation of the 0.2-μm-thick sample.





    Supporting Movie 4

    Movie 4. Discrete dislocation plasticity simulation of the 0.6-μm-thick sample.





    Supporting Movie 5

    Movie 5. Discrete dislocation plasticity simulation of the 1 μm-thick sample.

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An interpretation of size-scale plasticity in geometrically confined systems
H. D. Espinosa, S. Berbenni, M. Panico, K. W. Schwarz
Proceedings of the National Academy of Sciences Nov 2005, 102 (47) 16933-16938; DOI: 10.1073/pnas.0508572102

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An interpretation of size-scale plasticity in geometrically confined systems
H. D. Espinosa, S. Berbenni, M. Panico, K. W. Schwarz
Proceedings of the National Academy of Sciences Nov 2005, 102 (47) 16933-16938; DOI: 10.1073/pnas.0508572102
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Proceedings of the National Academy of Sciences of the United States of America: 102 (47)
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