Yttria-stabilized zirconia

Yttria-stabilized zirconia (YSZ) is a ceramic in which the crystal structure of zirconium dioxide is made stable at room temperature by an addition of yttrium oxide. These oxides are commonly called "zirconia" (ZrO2) and "yttria" (Y2O3), hence the name.

Stabilization

Pure zirconium dioxide undergoes a phase transformation from monoclinic (stable at the room temperature) to tetragonal (at about 1173 °C) and then to cubic (at about 2370 °C), according to the scheme:

monoclinic (1173 °C) tetragonal (2370 °C) cubic (2690 °C) melt

Obtaining stable sintered zirconia ceramic products is difficult because of the large volume change accompanying the transition from tetragonal to monoclinic (about 9%). Stabilization of the cubic polymorph of zirconia over wider range of temperatures is accomplished by substitution of some of the Zr4+ ions (ionic radius of 0.82 Å, too small for ideal lattice of fluorite characteristic for the tetragonal zirconia) in the crystal lattice with slightly larger ions, e.g., those of Y3+ (ionic radius of 0.96 Å). The resulting doped zirconia materials are termed stabilized zirconias.[1]

Materials related to YSZ include calcia-, magnesia-, ceria- or alumina-stabilized zirconias, or partially stabilized zirconias (PSZ). Hafnia stabilized Zirconia is also known.

Although 8-9 mol% YSZ is known to not be completely stabilized in the pure cubic YSZ phase up to temperatures above 1000 °C (Ref.[2] and publications therein), commonly used abbreviations in conjunction with yttra-stabilized zirconia are:

Thermal expansion coefficient

The thermal expansion coefficients depends on the modification of zirconia as follows:

Ionic conductivity of YSZ and its degradation

By the addition of yttria to pure zirconia (e.g., fully stabilized YSZ) Y3+ ions replace Zr4+ on the cationic sublattice. Thereby, oxygen vacancies are generated due to charge neutrality:[6]

with ,

meaning two Y3+ ions generate one vacancy on the anionic sublattice. This facilitates moderate conductivity of yttrium stabilized zirconia for O2− ions (and thus electrical conductivity) at elevated and high temperature. This ability to conduct O2− ions makes yttria-stabilized zirconia well suited for application as solid electrolye in solid oxide fuel cells.

For low dopant concentrations, the ionic conductivity of the stabilized zirconias increases with increasing Y2O3 content. It has a maximum around 8-9 mol% almost independent of the temperature (800-1200 °C).[1][2] Unfortunately, 8-9 mol% YSZ (8YSZ, 8YDZ) also turned out to be situated in the 2-phase field (c+t) of the YSZ phase diagram at these temperatures, which causes the material's decomposition into Y-enriched and depleted regions on the nm-scale and, consequently, the electrical degradation during operation.[3] The microstructural and chemical changes on the nm-scale are accompanied by the drastic decrease of the oxygen-ion conductivity of 8YSZ (degradation of 8YSZ) of about 40% at 950 °C within 2500 hrs.[4] Traces of impurities like Ni, dissolved in the 8YSZ ,e.g., due to fuel-cell fabrication, can have a severe impact on the decompositon rate (acceleration of inherent decomposition of the 8YSZ by orders of magnitude) such that the degradation of conductivity even becomes problematic at low operation temperatures in the range of 500-700 °C.[7]

Nowadays, more complex ceramics like co-doped Zirconia (e.g., with Scandia, ...) are in use as solid electrolytes.

Applications

Multiple metal-free dental crowns

YSZ has a number of applications:

See also

References

  1. 1 2 H. Yanagida, K. Koumoto, M. Miyayama, "The Chemistry of Ceramics", John Wiley & Sons, 1996. ISBN 0 471 95627 9.
  2. 1 2 3 Butz, Benjamin (2011). Yttria-doped zirconia as solid electrolyte for fuel-cell applications : Fundamental aspects. Südwestdt. Verl. für Hochschulschr. ISBN 978-3-8381-1775-1.
  3. 1 2 Butz, B.; Schneider, R.; Gerthsen, D.; Schowalter, M.; Rosenauer, A. (2009-10-01). "Decomposition of 8.5 mol.% Y2O3-doped zirconia and its contribution to the degradation of ionic conductivity". Acta Materialia. 57 (18): 5480–5490. doi:10.1016/j.actamat.2009.07.045.
  4. 1 2 Butz, B.; Kruse, P.; Störmer, H.; Gerthsen, D.; Müller, A.; Weber, A.; Ivers-Tiffée, E. (2006-12-01). "Correlation between microstructure and degradation in conductivity for cubic Y2O3-doped ZrO2". Solid State Ionics. 177 (37–38): 3275–3284. doi:10.1016/j.ssi.2006.09.003.
  5. 1 2 3 Matweb: CeramTec 848 Zirconia (ZrO2) & Zirconium Oxide, Zirconia, ZrO2
  6. Hund, F (1951). "Anomale Mischkristalle im System ZrO2–Y2O3. Kristallbau der Nernst-Stifte.". Zeitschrift für Elektrochemie und Angewandte Physikalische Chemie. 55: 363–366.
  7. Butz, B.; Lefarth, A.; Störmer, H.; Utz, A.; Ivers-Tiffée, E.; Gerthsen, D. (2012-04-25). "Accelerated degradation of 8.5 mol% Y2O3-doped zirconia by dissolved Ni". Solid State Ionics. 214: 37–44. doi:10.1016/j.ssi.2012.02.023.
  8. Minh, N.Q. (1993). "Ceramic Fuel-Cells". Journal of the American Ceramic Society. 76 (3): 563–588. doi:10.1111/j.1151-2916.1993.tb03645.x.
  9. De Guire, Eileen (2003). "Solid Oxide Fuel Cells". CSA.
  10. American Ceramic Society (29 May 2009). Progress in Thermal Barrier Coatings. John Wiley and Sons. pp. 139–. ISBN 978-0-470-40838-4. Retrieved 23 October 2011.
  11. http://www.diamond-fo.com/en/products_catalogue_details.asp?section=2&group=e2000&source=Assemblies&family=10101

Further reading

This article is issued from Wikipedia - version of the 12/4/2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.