Developing new high-entropy rare-earth zirconate (HE-RE2Zr2O7) ceramics with low thermal conductivity is essential for thermal barrier coating materials. In this work, the average atomic spacings, interatomic forces, and average atomic masses of 16 rare-earth elements occupying the A site of the cubic A2B2O7 crystal structure were calculated by density functional theory. These three physical qualities, as vectors, characterise the corresponding rare-earth elements. The distance between the two vectors quantitatively describes the difference between two rare-earth elements. For greater difference between two rare-earth elements, the disorder degree of HE-RE2Zr2O7 is higher, and therefore the thermal conductivity is lower. From theoretical calculation, the thermal conductivity of the ceramics gradually increases in the order (Sc0.2Y0.2La0.2Ho0.2Yb0.2)2Zr2O7, (Sc0.2Ce0.2Nd0.2Eu0.2Gd0.2)2Zr2O7, (Sc0.2Y0.2Tm0.2Yb0.2Lu0.2)2Zr2O7, and (Sc0.2Er0.2Tm0.2Yb0.2Lu0.2)2Zr2O7. Using the solution precursor plasma spray method and pressureless sintering method, four types of HE-RE2Zr2O7 powder and bulk samples were prepared. The samples all showed a single defective fluorite structure with uniform distribution of the elements and a stable phase structure. The thermal conductivities of the sintered HE-RE2Zr2O7 bulk samples were in the range 1.30–1.45 W·m−1·K−1 at 1400 °C, and their differences were consistent with the theoretical calculation results. Among the ceramics, (Sc0.2Y0.2La0.2Ho0.2Yb0.2)2Zr2O7 showed the lowest thermal conductivity (1.30 W∙m−1∙K−1, 1400 °C), highest thermal expansion coefficient (10.19 × 10−6 K−1, 200–1400 °C), highest fracture toughness (1.69 ± 0.28 MPa∙m1/2), and smallest brittleness index (3.03·μm−1/2). Therefore, (Sc0.2Y0.2La0.2Ho0.2Yb0.2)2Zr2O7 is considered to be an ideal candidate material for next-generation thermal barrier coating applications.
7 August 2018 in Journal of Thermal Spray Technology
Lanthanum-cerium oxide (La2Ce2O7, LC) thermal barrier coatings (TBCs) were prepared by atmospheric plasma spraying (APS). The actual composition of the as-sprayed coating is La2Ce1.66O4.32, due to the volatilization of CeO2 phase during the spray process. A little decomposition of the LC coating takes place after annealing at 1400¡䟦or 240h. The thermal conductivity of bulk LC material is about 0.51W/(m¡¤K) at 1000¡䪠which is one fourth of that of typical bulk YSZ. The coefficient of thermal expansion (CTE) of the LC coating ranges from 10¡�0-6K-1 to 13¡�0-6K-1 at the temperature from 450¡䟴o 1100¡䪠which is relatively higher than that of the YSZ coating. Dilatometric measurements show that there is slight shrinkage in the coating till 1250¡䪠however, a remarkable sintering process happens cluring holding period at 1250¡䬠A spallation of the LC TBC occurs after 60 cycles at 1100¡䟢y typical delaminating cracking within the LC topcoat.
In this work, LaPO4:Ce, Tb phosphors were prepared by firing a LaPO4:Ce, Tb precipitate using an ionic-liquid-driven supported liquid membrane system. The entire system consisted of three parts: a mixed rare earth ion supply phase, a phosphate supply phase, and an ionic-liquid-driven supporting liquid membrane phase. This method showed the advantages of a high flux, high efficiency, and more controllable reaction process. The release rate of PO43− from the liquid film under different types of ionic liquid, the ratio of the rare earth ions in the precursor mixture, and the structure, morphology, and photoluminescence properties of LaPO4:Ce, Tb were investigated by inductively coupled plasma-atomic emission spectroscopy, X-ray diffraction, Raman spectra, scanning electron microscopy, and photoluminescence emission spectra methods. The results showed that a pure phase of lanthanum orthophosphate with a monoclinic structure can be formed. Due to differences in the anions in the rare earth supply phase, the prepared phosphors showed micro-spherical (when using rare earth sulfate as the raw material) and nanoscale stone-shape (when using rare earth nitrate as the raw material) morphologies. Moreover, the phosphors prepared by this method had good luminescent properties, reaching a maximum emission intensity under 277 nm excitation with a predominant green emission at 543 nm which corresponded to the 5D4-7F5 transition of Tb3+.