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  • In nanocrystalline materials the grain boundaries must be considered as regions of finite thickness with properties different from the crystalline bulk material present in the crystallite cores. Thus, dense (i.e. pore-free) single-phase nanocrystalline materials can be considered as quasi-two-phase systems whose effective properties can be calculated when quantitative thickness information is available and the property value of the grain boundary phase can be reliably estimated. Similarly, dense two-phase nanocomposites may be considered as quasi-three-phase systems and their effective properties can be predicted using an analogous phase mixture modeling approach. In this contribution this is done for the thermal conductivity of alumina-zirconia nanocomposites. A two-stage homogenization procedure is applied, consisting of a first step in which the alumina-zirconia composite is treated as a symmetric-cell material, and a second step in which the highly disordered grain boundary phase is treated as a m
  • In nanocrystalline materials the grain boundaries must be considered as regions of finite thickness with properties different from the crystalline bulk material present in the crystallite cores. Thus, dense (i.e. pore-free) single-phase nanocrystalline materials can be considered as quasi-two-phase systems whose effective properties can be calculated when quantitative thickness information is available and the property value of the grain boundary phase can be reliably estimated. Similarly, dense two-phase nanocomposites may be considered as quasi-three-phase systems and their effective properties can be predicted using an analogous phase mixture modeling approach. In this contribution this is done for the thermal conductivity of alumina-zirconia nanocomposites. A two-stage homogenization procedure is applied, consisting of a first step in which the alumina-zirconia composite is treated as a symmetric-cell material, and a second step in which the highly disordered grain boundary phase is treated as a m (en)
Title
  • Thermal Conductivity of Ceramic Nanocomposites - the Phase Mixture Modeling Approach
  • Thermal Conductivity of Ceramic Nanocomposites - the Phase Mixture Modeling Approach (en)
skos:prefLabel
  • Thermal Conductivity of Ceramic Nanocomposites - the Phase Mixture Modeling Approach
  • Thermal Conductivity of Ceramic Nanocomposites - the Phase Mixture Modeling Approach (en)
skos:notation
  • RIV/60461373:22310/10:00022970!RIV11-MSM-22310___
http://linked.open...avai/riv/aktivita
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  • P(IAA401250703), S, Z(MSM6046137302)
http://linked.open...iv/cisloPeriodika
  • 71
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  • 292704
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  • RIV/60461373:22310/10:00022970
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  • Thermal conductivity; nanocrystalline ceramics; grain boundaries; phase-mixture models; sigmoidal average; symmetric-cell materials; core-shell microstructure; Wiener bounds; Hashin-Shtrikman bounds; Beran bounds; alumina; zirconia; composites. (en)
http://linked.open.../riv/klicoveSlovo
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  • CH - Švýcarská konfederace
http://linked.open...ontrolniKodProRIV
  • [67F3E98E5804]
http://linked.open...i/riv/nazevZdroje
  • Advances in Science and Technology
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http://linked.open...vavai/riv/projekt
http://linked.open...UplatneniVysledku
http://linked.open...v/svazekPeriodika
  • 2010
http://linked.open...iv/tvurceVysledku
  • Pabst, Willi
  • Hostaša, Jan
http://linked.open...n/vavai/riv/zamer
issn
  • 1662-0356
number of pages
http://localhost/t...ganizacniJednotka
  • 22310
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