TY - GEN
T1 - Mechanical properties of La 0.6Sr 0.4Co 1-yFe yO 3-δ under various temperatures and oxygen partial pressures
AU - Kimura, Y.
AU - Kushi, T.
AU - Hashimoto, S.
AU - Watanabe, S.
AU - Amezawa, K.
AU - Kawada, T.
AU - Fukuda, Y.
AU - Unemoto, A.
AU - Sato, K.
AU - Yashiro, K.
AU - Mizusaki, J.
AU - Hashida, T.
PY - 2011
Y1 - 2011
N2 - Young's modulus, shear modulus, Poisson's ratio and internal friction of La 0.6Sr 0.4CoO 3-δ (LSC) and La 0.6Sr 0.4Co 0.2Fe 0.8O 3-δ (LSCF6428) were evaluated in the temperature range between 298 to 1173 K, and the oxygen partial pressure, P(O 2), range between 1 × 10 -1 to 1 × 10 -4 bar using the resonance method. The apparent Young's moduli of LSC and LSCF6428 first decreased with increasing temperature, and then drastically increased at intermediate temperatures. P(O 2) dependence of the Young's modulus of LSCF6428 showed different trends depending on temperature. At 873 K, the Young's modulus was almost independent of P(O 2), while it increased with decreasing P(O 2) at 973 K. At 1073 K, it increased down to 5 × 10 -3 bar and then decreased in further lower P(O 2). At 1173 K, it decreased with decreasing P(O 2). Such complicated temperature and P(O 2) dependences are considered as composite phenomena caused by the lattice expansion/shrinkage, the oxygen nonstoichiometry change, and the phase transition.
AB - Young's modulus, shear modulus, Poisson's ratio and internal friction of La 0.6Sr 0.4CoO 3-δ (LSC) and La 0.6Sr 0.4Co 0.2Fe 0.8O 3-δ (LSCF6428) were evaluated in the temperature range between 298 to 1173 K, and the oxygen partial pressure, P(O 2), range between 1 × 10 -1 to 1 × 10 -4 bar using the resonance method. The apparent Young's moduli of LSC and LSCF6428 first decreased with increasing temperature, and then drastically increased at intermediate temperatures. P(O 2) dependence of the Young's modulus of LSCF6428 showed different trends depending on temperature. At 873 K, the Young's modulus was almost independent of P(O 2), while it increased with decreasing P(O 2) at 973 K. At 1073 K, it increased down to 5 × 10 -3 bar and then decreased in further lower P(O 2). At 1173 K, it decreased with decreasing P(O 2). Such complicated temperature and P(O 2) dependences are considered as composite phenomena caused by the lattice expansion/shrinkage, the oxygen nonstoichiometry change, and the phase transition.
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U2 - 10.1149/1.3570240
DO - 10.1149/1.3570240
M3 - Conference contribution
AN - SCOPUS:84863155550
SN - 9781607682363
T3 - ECS Transactions
SP - 2429
EP - 2434
BT - Solid Oxide Fuel Cells 12, SOFC XII
T2 - 12th International Symposium on Solid Oxide Fuel Cells, SOFC-XII - 219th ECS Meeting
Y2 - 1 May 2011 through 6 May 2011
ER -