TY - JOUR
T1 - The brick layer model revisited
T2 - Introducing the nano-grain composite model
AU - Kidner, Neil J.
AU - Perry, Nicola H.
AU - Mason, Thomas O.
AU - Garboczi, Edward J.
PY - 2008/6
Y1 - 2008/6
N2 - Brick layer models (BLMs), although applicable at the microscale, are inappropriate for characterizing electroceramics at the nanoscale. A new construct, the nano-grain composite model (n-GCM), has been developed to model/analyze the AC-impedance response of equiaxed polycrystalline electroceramics. The procedure employs a set of equations, based on the Maxwell-Wagner/Hashin-Shtrikman effective medium model, to calculate local electrical properties (conductivity, dielectric constant) for both "phases" (grain core, grain boundary) from experimental AC-impedance spectra and also, for the first time, grain core volume fraction. The n-GCM method was tested on a model system (a 3D-BLM material) and demonstrated with a test case (nanograined yttria-stabilized zirconia). The method appears to be applicable only at nanograin sizes, i.e., 10-100 nm. Limitations of the method, in terms of grain size (10-100 nm) and experimental uncertainty, are also discussed.
AB - Brick layer models (BLMs), although applicable at the microscale, are inappropriate for characterizing electroceramics at the nanoscale. A new construct, the nano-grain composite model (n-GCM), has been developed to model/analyze the AC-impedance response of equiaxed polycrystalline electroceramics. The procedure employs a set of equations, based on the Maxwell-Wagner/Hashin-Shtrikman effective medium model, to calculate local electrical properties (conductivity, dielectric constant) for both "phases" (grain core, grain boundary) from experimental AC-impedance spectra and also, for the first time, grain core volume fraction. The n-GCM method was tested on a model system (a 3D-BLM material) and demonstrated with a test case (nanograined yttria-stabilized zirconia). The method appears to be applicable only at nanograin sizes, i.e., 10-100 nm. Limitations of the method, in terms of grain size (10-100 nm) and experimental uncertainty, are also discussed.
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U2 - 10.1111/j.1551-2916.2008.02445.x
DO - 10.1111/j.1551-2916.2008.02445.x
M3 - Article
AN - SCOPUS:44649176898
SN - 0002-7820
VL - 91
SP - 1733
EP - 1746
JO - Journal of the American Ceramic Society
JF - Journal of the American Ceramic Society
IS - 6
ER -