Pure zirconium dioxide undergoes a phase transformation from monoclinic to tetragonal and then to cubic, according to the scheme: monoclinic tetragonal cubic melt Obtaining stable sintered zirconia ceramic products is difficult because of the large volume change accompanying the transition from tetragonal to monoclinic. Stabilization of the cubic polymorph of zirconia over wider range of temperatures is accomplished by substitution of some of the Zr4+ ions in the crystal lattice with slightly larger ions, e.g., those of Y3+. The resulting doped zirconia materials are termed stabilized zirconias. Materials related to YSZ include calcia-, magnesia-, ceria- or alumina-stabilized zirconias, or partially stabilized zirconias. 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. Commonly used abbreviations in conjunction with yttria-stabilized zirconia are:
* 8YDZ - 8-9 mol% Y2O3-doped ZrO2: owing the fact that the material is not completely stabilized and decomposes at high application temperatures, see paragraph next paragraphs)
By the addition of yttria to pure zirconia Y3+ ions replace Zr4+ on the cationic sublattice. Thereby, oxygen vacancies are generated due to charge neutrality: with , meaning two Y3+ ions generate one vacancy on the anionic sublattice. This facilitates moderate conductivity of yttrium stabilized zirconia for O2− ions at elevated and high temperature. This ability to conduct O2− ions makes yttria-stabilized zirconia well suited for application as solid electrolyte 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. Unfortunately, 8-9 mol% YSZ also turned out to be situated in the 2-phase field 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. The microstructural and chemical changes on the nm-scale are accompanied by the drastic decrease of the oxygen-ion conductivity of 8YSZ of about 40% at 950 °C within 2500 hrs. Traces of impurities like Ni, dissolved in the 8YSZ, e.g., due to fuel-cell fabrication, can have a severe impact on the decomposition rate such that the degradation of conductivity even becomes problematic at low operation temperatures in the range of 500-700 °C. Nowadays, more complex ceramics like co-doped Zirconia are in use as solid electrolytes.
As an electroceramic due to its ion-conducting properties.
Used in the production of a solid oxide fuel cell. YSZ is used as the solid electrolyte, which enables oxygen ion conduction while blocking electronic conduction. In order to achieve sufficient ion conduction, an SOFC with a YSZ electrolyte must be operated at high temperatures. While it is advantageous that YSZ retains mechanical robustness at those temperatures, the high temperature necessary is often a disadvantage of SOFCs. The high density of YSZ is also necessary in order to physically separate the gaseous fuel from oxygen, or else the electrochemical system would produce no electrical power.
For its hardness and optical properties in monocrystal form, it is used as jewelry.
As a material for non-metallic knife blades, produced by Boker and Kyocera companies.
In water-based pastes for do-it-yourself ceramics and cements. These contain microscopic YSZ milled fibers or sub-micrometer particles, often with potassium silicate and zirconium acetate binders. The cementation occurs on removal of water. The resulting ceramic material is suitable for very high temperature applications.
YSZ doped with rare-earth materials can act as a thermographic phosphor and a luminescent material.
Historically used for glowing rods in Nernst lamps.
