1988
DOI: 10.1111/j.1151-2916.1988.tb05893.x
|View full text |Cite
|
Sign up to set email alerts
|

Phase Equilibrium and Martensitic Transformation in Lanthana‐Doped Zirconia

Abstract: The system Zr02-La203 has been studied in the 0 to 15 mol% La203 range using X-ray diffraction and thermal analysis. Tho kinds of diagrams were elaborated: First is a phase equilibrium diagram where the eutectoid decomposition of ZrOz,,,(T) -+ Zr02,..(M) + Py,, occurs at 1100°C and 0.75 mol% La203 (Py is the pyrochlore compound ZrzLaz07). The maximum solubility of La203 in ZrOz,..(M) is 0.5 mol% at room temperature. Second, a nonequilibrium diagram is determined showing the correlations between grain size, La2… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
19
0

Year Published

1989
1989
2016
2016

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 57 publications
(20 citation statements)
references
References 17 publications
1
19
0
Order By: Relevance
“…The calculated data on invariant reactions are presented in Table 3. The calculations agree with experimental phase equilibria [21,[39][40][41]. The detailed comparison of the calculated phase diagrams with the experimental data is given elsewhere [42].…”
Section: Binary Systemsmentioning
confidence: 71%
“…The calculated data on invariant reactions are presented in Table 3. The calculations agree with experimental phase equilibria [21,[39][40][41]. The detailed comparison of the calculated phase diagrams with the experimental data is given elsewhere [42].…”
Section: Binary Systemsmentioning
confidence: 71%
“…These results are consistent with the www.particle-journal.com www.MaterialsViews.com fi ndings of Bastide et al for La-doped bulk zirconia, for which both a stabilization of the tetragonal phase with increasing La content and the formation of a pyrochlore phase after heating to 1200 °C were documented. [ 21 ] Furthermore, the appearance of the pyrochlore phase coincided with the observed increase in particle disintegration at high dopant concentrations. This fi nding can possibly be attributed to a mismatch in thermal expansion coeffi cient between La 2 Zr 2 O 7 (9.1-9.7 × 10 −6 K −1 ) and ZrO 2 /YSZ (10.3 × 10 −6 K −1 , 10.5-11.5 × 10 −6 K −1 ).…”
Section: Stability Of La-doped Microparticlesmentioning
confidence: 86%
“…The diffraction refl exes for La 2 Zr 2 O 7 were no longer observed after reheating (see Supporting Information Figure S20), suggesting redissolution of the La 2 Zr 2 O 7 into the monoclinic phase. The La concentrations for the particles (3% and less) are borderline with the range for solid solubility in monoclinic zirconia, as given by the phase diagrams for the La 2 O 3 -ZrO 2 system, [22][23][24] but are higher than maximum solubility of 1% La reported by Bastide et al [ 21 ] Lastly, after heating at 1500 °C, all samples were fully sintered and had lost their spherical shape, as shown in the Supporting Information ( Figure S4). …”
Section: Stability Of La-doped Microparticlesmentioning
confidence: 93%
See 1 more Smart Citation
“…This is due to the large solubility of Mn in YSZ (∼5 cat.-% in 8YSZ at 1,000°C in air and ∼8 cat.-% at 1,000°C and P(O 2 ) = 10 0 Pa) [16]. Due to small solubility of La and Sr in YSZ (<2 cat.% La and ∼0 cat.% Sr at temperature below 1,500°C) [17][18][19][20][21][22][23][24][25], the diffusion of La and Sr from LSM into YSZ and the corresponding influence on the interface stability is quite limited. It is however a different situation for the Mn diffusion, due to relatively high solubility of Mn in YSZ and its dependence on P(O 2 ).…”
Section: Stability Of the Lsm-ysz Interface Under Different P(o 2 )mentioning
confidence: 99%