Yb3+ doping effects on thermal conductivity and thermal expansion of yttrium aluminium garnet. Issue 12 (September 2016)

• Record Type: Journal Article
• Authors: Wang, Jing; Xu, Fang; Wheatley, R.J.; Neate, Nigel; Hou, Xianghui
• Is Part Of: Ceramics international. Volume 42:Issue 12(2016)
• Page Start: 14228
• Page End: 14235
• Publication Date: 2016-09
• Subjects: Thermal barrier coating -- Yttrium aluminium garnet -- Thermal conductivity -- Coefficient of thermal expansion; Ceramics -- Periodicals; Céramique industrielle -- Périodiques; Ceramics; Periodicals; Electronic journals; 666
• DOI: 10.1016/j.ceramint.2016.06.034
• Languages: English
• ISSNs: 0272-8842

Abstract

Abstract: Yttrium Aluminium Garnet (YAG) is an attractive candidate as thermal barrier material used for turbine blade in aero engines, due to its relatively low thermal conductivity, low oxygen diffusivity and good phase stability at high temperature. YAG has a complex crystal structure, in which Y 3+ ions locate in dodecahedron and Al 3+ ions in octahedron and tetrahedron. Replacing the host cations with rare earth elements can cause the structure change which influences the thermal properties of YAG. Because the space inside the octahedron is relatively small, Yb 3+ ions which have the smallest ionic radial size in the lanthanide series, have been selected and attempted to be doped on dodecahedral and octahedral sites to investigate the effects on thermal conductivity and thermal expansion. The variation of lattice constant indicates that Yb 3+ ions are located on the dodecahedron or octahedron. In addition, when Yb 3+ ions replace Al 3+ ions on octahedral sites, the thermal conductivity at room temperature is dramatically reduced and the coefficient of thermal expansion is over 10×10 −6 K −1 at high temperature, which results from the expansion of octahedron due to the much larger radius of Yb 3+ ion compared with the host cation (Al 3+ ion). On the contrary, replacing Y 3+ ions with Yb 3+ ions in dodecahedron, the thermal conductivity also gradually reduces to the similar value but the coefficient of thermal expansion is getting smaller, due to the relatively small ionic radius of Yb 3+ causing the contraction of the dodecahedron. Therefore, a dopant with much larger radius would be preferred in both dodecahedron and octahedron to significant reduce thermal conductivity as well as increase coefficient of thermal expansion of YAG, by introducing large radial difference between the dopant and the host cations.