Investigations into the slip behavior of zirconium diboride

The slip systems in ZrB2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a dislocation density of approximately 1013 m−2. The structure of the dislocations as well as the low density is in agreement with a ceramic that is hard...

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Published inJournal of materials research Vol. 31; no. 18; pp. 2749 - 2756
Main Authors Hunter, Brett, Yu, Xiao-Xiang, De Leon, Nicholas, Weinberger, Christopher, Fahrenholtz, William, Hilmas, Greg, Weaver, Mark L., Thompson, Gregory B.
Format Journal Article
LanguageEnglish
Published New York, USA Cambridge University Press 28.09.2016
Springer International Publishing
Springer Nature B.V
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Abstract The slip systems in ZrB2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a dislocation density of approximately 1013 m−2. The structure of the dislocations as well as the low density is in agreement with a ceramic that is hard and brittle and dislocation nucleation and motion is restricted. The low temperature slip systems were found to include c-prismatic slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {0001} \right]\left( {\bar 1010} \right)$ —and a-pyramidal slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {\bar 1101} \right)$ whereas the elevated temperature sample revealed a-basal slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {0001} \right)$ . Density functional theory Generalized Stacking Fault Energy curves for perfect slip were calculated and agreed well with geometric considerations for slip, including interplanar spacing and planar packing. Though basal slip has the lowest fault energy, the presence of the other dislocation types is suggestive that the activation barrier is not a hindrance for the temperatures studied and is likely activated to increase the number of plastic degrees of freedom.
AbstractList Abstract The slip systems in ZrB 2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a dislocation density of approximately 10 13 m −2 . The structure of the dislocations as well as the low density is in agreement with a ceramic that is hard and brittle and dislocation nucleation and motion is restricted. The low temperature slip systems were found to include c-prismatic slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {0001} \right]\left( {\bar 1010} \right)$ —and a-pyramidal slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {\bar 1101} \right)$ whereas the elevated temperature sample revealed a-basal slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {0001} \right)$ . Density functional theory Generalized Stacking Fault Energy curves for perfect slip were calculated and agreed well with geometric considerations for slip, including interplanar spacing and planar packing. Though basal slip has the lowest fault energy, the presence of the other dislocation types is suggestive that the activation barrier is not a hindrance for the temperatures studied and is likely activated to increase the number of plastic degrees of freedom.
The slip systems in ZrB 2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a dislocation density of approximately 10 13 m −2 . The structure of the dislocations as well as the low density is in agreement with a ceramic that is hard and brittle and dislocation nucleation and motion is restricted. The low temperature slip systems were found to include c-prismatic slip— 1 / 3 [ 0001 ] ( 1 ¯ 010 ) —and a-pyramidal slip— 1 / 3 [ 11 2 ¯ 0 ] ( 1 ¯ 101 ) whereas the elevated temperature sample revealed a-basal slip— 1 / 3 [ 11 2 ¯ 0 ] ( 0001 ) . Density functional theory Generalized Stacking Fault Energy curves for perfect slip were calculated and agreed well with geometric considerations for slip, including interplanar spacing and planar packing. Though basal slip has the lowest fault energy, the presence of the other dislocation types is suggestive that the activation barrier is not a hindrance for the temperatures studied and is likely activated to increase the number of plastic degrees of freedom.
The slip systems in ZrB2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a dislocation density of approximately 1013 m−2. The structure of the dislocations as well as the low density is in agreement with a ceramic that is hard and brittle and dislocation nucleation and motion is restricted. The low temperature slip systems were found to include c-prismatic slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {0001} \right]\left( {\bar 1010} \right)$ —and a-pyramidal slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {\bar 1101} \right)$ whereas the elevated temperature sample revealed a-basal slip— ${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {0001} \right)$ . Density functional theory Generalized Stacking Fault Energy curves for perfect slip were calculated and agreed well with geometric considerations for slip, including interplanar spacing and planar packing. Though basal slip has the lowest fault energy, the presence of the other dislocation types is suggestive that the activation barrier is not a hindrance for the temperatures studied and is likely activated to increase the number of plastic degrees of freedom.
The slip systems in ZrB2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a dislocation density of approximately 1013 m-2. The structure of the dislocations as well as the low density is in agreement with a ceramic that is hard and brittle and dislocation nucleation and motion is restricted. The low temperature slip systems were found to include c-prismatic slip-- [formula omitted: see PDF] --and a-pyramidal slip-- [formula omitted: see PDF] whereas the elevated temperature sample revealed a-basal slip-- [formula omitted: see PDF] . Density functional theory Generalized Stacking Fault Energy curves for perfect slip were calculated and agreed well with geometric considerations for slip, including interplanar spacing and planar packing. Though basal slip has the lowest fault energy, the presence of the other dislocation types is suggestive that the activation barrier is not a hindrance for the temperatures studied and is likely activated to increase the number of plastic degrees of freedom.
Author Hunter, Brett
Fahrenholtz, William
De Leon, Nicholas
Thompson, Gregory B.
Yu, Xiao-Xiang
Hilmas, Greg
Weinberger, Christopher
Weaver, Mark L.
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  givenname: Xiao-Xiang
  surname: Yu
  fullname: Yu, Xiao-Xiang
  organization: Department of Metallurgical & Materials Engineering, University of Alabama, Tuscaloosa, AL 35405
– sequence: 3
  givenname: Nicholas
  surname: De Leon
  fullname: De Leon, Nicholas
  organization: Department of Metallurgical & Materials Engineering, University of Alabama, Tuscaloosa, AL 35405
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  givenname: Christopher
  surname: Weinberger
  fullname: Weinberger, Christopher
  organization: † Department of Mechanical Engineering and Mechanics, Drexel University, Philadelphia, PA 19104
– sequence: 5
  givenname: William
  surname: Fahrenholtz
  fullname: Fahrenholtz, William
  organization: ‡ Department of Materials Science & Engineering, Missouri S&T, Rolla, MO 65401
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  organization: ‡ Department of Materials Science & Engineering, Missouri S&T, Rolla, MO 65401
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  givenname: Mark L.
  surname: Weaver
  fullname: Weaver, Mark L.
  organization: Department of Metallurgical & Materials Engineering, University of Alabama, Tuscaloosa, AL 35405
– sequence: 8
  givenname: Gregory B.
  surname: Thompson
  fullname: Thompson, Gregory B.
  email: gthompson@eng.ua.edu
  organization: Department of Metallurgical & Materials Engineering, University of Alabama, Tuscaloosa, AL 35405
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Snippet The slip systems in ZrB2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a...
The slip systems in ZrB 2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a...
Abstract The slip systems in ZrB 2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a...
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SubjectTerms Analysis
Applied and Technical Physics
Biomaterials
Ceramics
Chemistry
Deformation
Focus Section Article
Focus Section Articles
Focus Section: Reinventing Boron Chemistry and Materials for the 21st Century
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Inorganic Chemistry
Materials Engineering
Materials research
Materials Science
Nanotechnology
Oxidation
Scanning electron microscopy
Studies
Temperature
Title Investigations into the slip behavior of zirconium diboride
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