TY - JOUR
T1 - Oxygen potential of solid solution EuyU1-yO2+x
AU - Fujino, Takeo
AU - Sato, Nobuaki
AU - Yamada, Kohta
AU - Nakama, Shohei
AU - Fukuda, Kousaku
AU - Serizawa, Hiroyuki
AU - Shiratori, Tetsuo
N1 - Copyright:
Copyright 2018 Elsevier B.V., All rights reserved.
PY - 1999/2
Y1 - 1999/2
N2 - The oxygen potential, ΔḠO2, of EuyU1-yO2+x solid solution was measured as a function of x value for y = 0.05 and 0.1 at 1000, 1100 and 1200°C using an electrobalance. With the addition of europium, a significant increase in ΔḠO2 was observed in the hypostoichiometric region, but its effect was almost the same for y = 0.05 and 0.1 in the hyperstoichiometric region. The O/M (M=Eu + U) ratio, which yields the steepest change of ΔḠO2, decreased with decreasing temperature in the range ca.1000-1400°C for y = 0.1, although this effect was not seen for y = 0.05. The temperature dependence of this decrease seemed to be enhanced as the y value increased. Both the partial molar entropy and enthalpy of oxygen (ΔS̄O2 and ΔH̄O2) for y = 0.1 solid solution showed sharp large peaks at O/M ratios slightly less than 2. Such peaks emerge as a result of the above decrease of the O/M ratio for steepest change of ΔḠO2, with decreasing temperature.
AB - The oxygen potential, ΔḠO2, of EuyU1-yO2+x solid solution was measured as a function of x value for y = 0.05 and 0.1 at 1000, 1100 and 1200°C using an electrobalance. With the addition of europium, a significant increase in ΔḠO2 was observed in the hypostoichiometric region, but its effect was almost the same for y = 0.05 and 0.1 in the hyperstoichiometric region. The O/M (M=Eu + U) ratio, which yields the steepest change of ΔḠO2, decreased with decreasing temperature in the range ca.1000-1400°C for y = 0.1, although this effect was not seen for y = 0.05. The temperature dependence of this decrease seemed to be enhanced as the y value increased. Both the partial molar entropy and enthalpy of oxygen (ΔS̄O2 and ΔH̄O2) for y = 0.1 solid solution showed sharp large peaks at O/M ratios slightly less than 2. Such peaks emerge as a result of the above decrease of the O/M ratio for steepest change of ΔḠO2, with decreasing temperature.
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U2 - 10.1016/S0022-3115(98)00502-9
DO - 10.1016/S0022-3115(98)00502-9
M3 - Article
AN - SCOPUS:0033079447
SN - 0022-3115
VL - 265
SP - 154
EP - 160
JO - Journal of Nuclear Materials
JF - Journal of Nuclear Materials
IS - 1-2
ER -