Grain Boundary Sliding in Aluminum Nano-Bi-Crystals Deformed at Room Temperature
Room‐temperature uniaxial compressions of 900‐nm‐diameter aluminum bi‐crystals, each containing a high‐angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite...
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| Published in | Small (Weinheim an der Bergstrasse, Germany) Vol. 10; no. 1; pp. 100 - 108 |
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| Language | English |
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WILEY-VCH Verlag
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| Abstract | Room‐temperature uniaxial compressions of 900‐nm‐diameter aluminum bi‐crystals, each containing a high‐angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of ∼176 MPa followed by gradual softening and a plateau centered around ∼125 MPa. An energetics‐based physical model, which may explain observed room‐temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano‐plasticity and defect microstructure evolution.
Bi‐crystalline Al nanopillars containing a single high‐angle grain boundary with a plane normal inclined at 24° to the loading direction are subject to room‐temperature uniaxial compression and reveal frictional sliding along the boundary plane to be the dominant deformation mechanism. An energetics‐based physical model, which may explain observed room‐temperature grain boundary sliding, is presented, and observations are discussed within the framework of crystalline nano‐plasticity and defect microstructure evolution. |
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| AbstractList | Room-temperature uniaxial compressions of 900-nm-diameter aluminum bi-crystals, each containing a high-angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of ~ 176 MPa followed by gradual softening and a plateau centered around ~ 125 MPa. An energetics-based physical model, which may explain observed room-temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano-plasticity and defect microstructure evolution. Room‐temperature uniaxial compressions of 900‐nm‐diameter aluminum bi‐crystals, each containing a high‐angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of ∼176 MPa followed by gradual softening and a plateau centered around ∼125 MPa. An energetics‐based physical model, which may explain observed room‐temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano‐plasticity and defect microstructure evolution. Bi‐crystalline Al nanopillars containing a single high‐angle grain boundary with a plane normal inclined at 24° to the loading direction are subject to room‐temperature uniaxial compression and reveal frictional sliding along the boundary plane to be the dominant deformation mechanism. An energetics‐based physical model, which may explain observed room‐temperature grain boundary sliding, is presented, and observations are discussed within the framework of crystalline nano‐plasticity and defect microstructure evolution. Room-temperature uniaxial compressions of 900-nm-diameter aluminum bi-crystals, each containing a high-angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of ~ 176 MPa followed by gradual softening and a plateau centered around ~ 125 MPa. An energetics-based physical model, which may explain observed room-temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano-plasticity and defect microstructure evolution.Room-temperature uniaxial compressions of 900-nm-diameter aluminum bi-crystals, each containing a high-angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of ~ 176 MPa followed by gradual softening and a plateau centered around ~ 125 MPa. An energetics-based physical model, which may explain observed room-temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano-plasticity and defect microstructure evolution. Room-temperature uniaxial compressions of 900-nm-diameter aluminum bi-crystals, each containing a high-angle grain boundary with a plane normal inclined at 24 degree to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of 176 MPa followed by gradual softening and a plateau centered around 125 MPa. An energetics-based physical model, which may explain observed room-temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano-plasticity and defect microstructure evolution. Bi-crystalline Al nanopillars containing a single high-angle grain boundary with a plane normal inclined at 24 degree to the loading direction are subject to room-temperature uniaxial compression and reveal frictional sliding along the boundary plane to be the dominant deformation mechanism. An energetics-based physical model, which may explain observed room-temperature grain boundary sliding, is presented, and observations are discussed within the framework of crystalline nano-plasticity and defect microstructure evolution. Room-temperature uniaxial compressions of 900-nm-diameter aluminum bi-crystals, each containing a high-angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of 176 MPa followed by gradual softening and a plateau centered around 125 MPa. An energetics-based physical model, which may explain observed room-temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano-plasticity and defect microstructure evolution. [PUBLICATION ABSTRACT] Room‐temperature uniaxial compressions of 900‐nm‐diameter aluminum bi‐crystals, each containing a high‐angle grain boundary with a plane normal inclined at 24° to the loading direction, revealed frictional sliding along the boundary plane to be the dominant deformation mechanism. The top crystallite sheared off as a single unit in the course of compression instead of crystallographic slip and extensive dislocation activity, as would be expected. Compressive stress strain data of deforming nano bicrystals was continuous, in contrast to single crystalline nano structures that show a stochastic stress strain signature, and displayed a peak in stress at the elastic limit of ∼176 MPa followed by gradual softening and a plateau centered around ∼125 MPa. An energetics‐based physical model, which may explain observed room‐temperature grain boundary sliding, in presented, and observations are discussed within the framework of crystalline nano‐plasticity and defect microstructure evolution. |
| Author | Jang, Dongchan Weinberger, Christopher R. Greer, Julia R. Aitken, Zachary H. |
| Author_xml | – sequence: 1 givenname: Zachary H. surname: Aitken fullname: Aitken, Zachary H. email: zaitken@caltech.edu organization: Division of Engineering and Applied Science, California Institute of Technology, 1200 E. California Blvd, Pasadena, CA 91125, USA – sequence: 2 givenname: Dongchan surname: Jang fullname: Jang, Dongchan organization: Division of Engineering and Applied Science, California Institute of Technology, 1200 E. California Blvd, Pasadena, CA 91125, USA – sequence: 3 givenname: Christopher R. surname: Weinberger fullname: Weinberger, Christopher R. organization: Sandia National Laboratories, P.O. Box 5800, MS1411, Albuquerque, NM 87185-1411, USA – sequence: 4 givenname: Julia R. surname: Greer fullname: Greer, Julia R. organization: Division of Engineering and Applied Science, California Institute of Technology, 1200 E. California Blvd, Pasadena, CA 91125, USA |
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| Keywords | bicrystals aluminum nanopillar grain boundary mechanical properties |
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| Snippet | Room‐temperature uniaxial compressions of 900‐nm‐diameter aluminum bi‐crystals, each containing a high‐angle grain boundary with a plane normal inclined at 24°... Room-temperature uniaxial compressions of 900-nm-diameter aluminum bi-crystals, each containing a high-angle grain boundary with a plane normal inclined at 24°... Room-temperature uniaxial compressions of 900-nm-diameter aluminum bi-crystals, each containing a high-angle grain boundary with a plane normal inclined at 24... |
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| SubjectTerms | Aluminum bicrystals grain boundary mechanical properties nanopillar Nanotechnology |
| Title | Grain Boundary Sliding in Aluminum Nano-Bi-Crystals Deformed at Room Temperature |
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