Abstract
The internal friction and creep deformation behavior of La0.8Ca0.2CoO3 and pure LaCoO3 mixed ionic electronic conducting perovskite ceramics have been studied by Dynamic Mechanical Analysis and uniaxial compression under constant applied load, respectively. It was found that both the internal friction and creep strain were almost an order of magnitude higher for Ca2+ doped LaCoO3 as compared to pure undoped LaCoO3. The difference in Ca2+ doped LaCoO3 behavior was attributed to the much higher concentration of point defects (e.g., oxygen vacancies) in the structure and their interaction with other mobile defects, such as ferroelastic domain/twin walls, stacking faults, dislocations, etc. Such interactions of numerous point defects with domain walls produce energetic barriers and slow down the movement of ferroelastic domain walls under applied stress. At the same time, the defects' interactions increase the internal friction resulting in a much higher creep strain of La0.8Ca0.2CoO3 as compared to pure LaCoO3, as the creep strain is determined by the distance between the domain wall and its equilibrium position at the onset of the creep process. Therefore, the high friction will result in the larger distance the wall has to move to reach the equilibrium which in turn results in higher creep strain. The expansion of LaCoO3 under constant applied compressive stress, named here as negative creep, was also discovered to occur during room temperature creep experiments.
Original language | English |
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Article number | 205103 |
Journal | Journal of Applied Physics |
Volume | 124 |
Issue number | 20 |
DOIs | |
State | Published - Nov 28 2018 |
Funding
This work was supported in part by the NSF Project No. CMMI-0968911, “Time Dependent Creep Deformation of Non Polar Mixed Conducting Ferroelastic Perovskites”. John Lloyd’s help with the DMA measurements of temperature and frequency dependent real and imaginary parts of elastic modulus of La0.8Ca0.2CoO3 and LaCoO3 perovskites during his stay at Oak Ridge National Laboratory in 2004 is acknowledged. The neutron diffraction experiment was carried out at the Spallation Neutron Source at Oak Ridge National Laboratory, which is one of the user facilities sponsored by the Scientific User Facilities Division, Office of Basic Energy Sciences, U.S. Department of Energy. The authors thank Mr. H. D. Skorpenske from SNS for the technical support of the neutron experiment. M.R. is thankful to the NSF Ceramics Program for supporting this study through Grant No. 1057155 awarded to Texas A&M University. S.P. acknowledges the support from the 2005 SURA-ORNL (the Southeastern Universities Research Association) Summer Cooperative Research Program scholarship and the thesis grant from Empa, Duebendorf, Switzerland for this work. Work at the Oak Ridge National Laboratory was sponsored by the U.S. Department of Energy, Office of Fossil Energy, Solid Oxide Fuel Cells Program, Core Technology Program at ORNL.
Funders | Funder number |
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Southeastern Universities Research Association | |
National Science Foundation | |
U.S. Department of Energy | 1057155 |
Office of Fossil Energy | |
Basic Energy Sciences | |
Texas A and M University |