TY - JOUR
T1 - Diffusionless Tetragonal–Cubic Transformation Temperature in Zirconia–Ceria Solid Solutions
AU - Yashima, Masatomo
AU - Morimoto, Kenji
AU - Ishizawa, Nobuo
AU - Yoshimura, Masahiro
PY - 1993/11
Y1 - 1993/11
N2 - Diffusionless tetragonal (t′) cubic (c′) phase transformation in 65‐mol%‐CeO2‐ZrO2 was investigated around the c′‐t′ equilibrium temperature T0c′‐t′ using powder X‐ray diffraction, where c′ was defined as a tetragonal or cubic phase with an axial ratio of unity. The {400} peak profile of t′‐ZrO2 broadened at 860° and 900°C. This indicated that the t′‐ZrO2 transformed partially into c′‐ZrO2. The {400} peak profile of c′‐ZrO2 also broadened at 860° and 900°C, which indicated that the c′‐ZrO2 partially transformed to t′‐ZrO2. The finish point of t′→c′ transformation Tft′→c′ was investigated by annealing the t′‐ZrO2 containing 30–65 mol% CeO2 at various temperatures. The T′ft′→c′ line existed in the vicinity of the cubic solubility limit within the t + c two‐phase region. This Tft′→c′ location, which should have been located in the vicinity of T0c′‐t′ could not be explained by a simple regular solution model. However, it was described successfully by a thermodynamic model based on Landau's phenomenologic theory.
AB - Diffusionless tetragonal (t′) cubic (c′) phase transformation in 65‐mol%‐CeO2‐ZrO2 was investigated around the c′‐t′ equilibrium temperature T0c′‐t′ using powder X‐ray diffraction, where c′ was defined as a tetragonal or cubic phase with an axial ratio of unity. The {400} peak profile of t′‐ZrO2 broadened at 860° and 900°C. This indicated that the t′‐ZrO2 transformed partially into c′‐ZrO2. The {400} peak profile of c′‐ZrO2 also broadened at 860° and 900°C, which indicated that the c′‐ZrO2 partially transformed to t′‐ZrO2. The finish point of t′→c′ transformation Tft′→c′ was investigated by annealing the t′‐ZrO2 containing 30–65 mol% CeO2 at various temperatures. The T′ft′→c′ line existed in the vicinity of the cubic solubility limit within the t + c two‐phase region. This Tft′→c′ location, which should have been located in the vicinity of T0c′‐t′ could not be explained by a simple regular solution model. However, it was described successfully by a thermodynamic model based on Landau's phenomenologic theory.
UR - https://www.scopus.com/pages/publications/0027870763
UR - https://www.scopus.com/pages/publications/0027870763#tab=citedBy
U2 - 10.1111/j.1151-2916.1993.tb04028.x
DO - 10.1111/j.1151-2916.1993.tb04028.x
M3 - Article
AN - SCOPUS:0027870763
SN - 0002-7820
VL - 76
SP - 2865
EP - 2868
JO - Journal of the American Ceramic Society
JF - Journal of the American Ceramic Society
IS - 11
ER -