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1.
《Ceramics International》2022,48(17):24888-24897
In the furnace cycle test, the growth of oxide film leads to the propagation and coalescence of multiple cracks near the interface, which should be responsible for the spallation of thermal barrier coatings (TBCs). A TBC model with real interface morphology is created, and the near-interface large pore is retained. The purpose of this work is to clarify the mechanism of TBC spallation caused by successive initiation, propagation, and linkage of cracks near the interface during thermal cycle. The dynamic growth of thermally grown oxide (TGO) is carried out by applying a stress-free strain. The crack nucleation and arbitrary path propagation in YSZ and TGO are simulated by the extended finite element method (XFEM). The debonding along the YSZ/TGO/BC interface is evaluated using a surface-based cohesive behavior. The large-scale pore in YSZ near the interface can initiate a new crack. The ceramic crack can propagate to the YSZ/TGO interface, which will accelerate the interfacial damage and debonding. For the TGO/BC interface, the normal compressive stress and small shear stress at the valley hinder the further crack propagation. The growth of YSZ crack and the formation of through-TGO crack are the main causes of TBC delamination. The accelerated BC oxidation increases the lateral growth strain of TGO, which will promote crack propagation and coalescence. The optimization design proposed in this work can provide another option for developing TBC with high durability. 相似文献
2.
Thermal barrier coatings (TBCs) produced by electron beam physical vapor deposition (EB-PVD) or plasma spray (PS) usually suffer from molten calcium-magnesium-alumino-silicate (CMAS) attack. In this study, columnar structured YSZ coatings were fabricated by plasma spray physical vapor deposition (PS-PVD). The coatings were CMAS-infiltrated at 1250?°C for short terms (1, 5, 30?min). The wetting and spreading dynamics of CMAS melt on the coating surface was in-situ investigated using a heating microscope. The results indicate that the spreading evolution of CMAS melt can be described in terms of two stages with varied time intervals and spreading velocities. Besides, the PS-PVD columnar coating (~100?μm thick) was fully penetrated by CMAS melt within 1?min. After the CMAS attack for 30?min, the original feathered-YSZ grains (tetragonal phase) in both PS-PVD and EB-PVD coatings were replaced by globular shaped monoclinic ZrO2 grains in the interaction regions. 相似文献
3.
Lanthanum doped nickel and YSZ composite anode (LaNi–YSZ) exhibited a greatly reduced polarization resistance and high performance for electrochemical oxidation of hydrogen and methane, which resulted from a fine anode structure with a high dispersion of nickel catalyst and a high catalytic activity towards methane. 相似文献
4.
秀卢瑟福背散射-沟道技术(RBS-C)和X射线衍射技术(XRD)研究了Pt和注入YSZ(Y2O3稳定的ZrO2)后产生的损伤和退火过程中损伤的恢复及注入Pt的晶化,RBS-C分析表明YSZ室温下的存在较强自退火效应,XRD分析结果示出硫以铂的晶化产生很大影响。 相似文献
5.
6.
Characterization of YSZ solid oxide fuel cells electrolyte deposited by atmospheric plasma spraying and low pressure plasma spraying 总被引:1,自引:0,他引:1
C. Zhang H. L. Liao W. Y. Li G. Zhang C. Coddet C. Zhang C. J. Li C. X. Li X. J. Ning 《Journal of Thermal Spray Technology》2006,15(4):598-603
Yttria doped zirconia has been widely used as electrolyte materials for solid oxide fuel cells (SOFC). Plasma spraying is
a cost-effective process to deposit YSZ electrolyte. In this study, the 8 mol% Y2O3 stabilized ZrO2 (YSZ) layer was deposited by low pressure plasma spraying (LPPS) and atmospheric plasma spraying (APS) with fused-crushed
and agglomerated powders to examine the effect of spray method and particle size on the electrical conductivity and gas permeability
of YSZ coating. The microstructure of YSZ coating was characterized by scanning electron microscopy and x-ray diffraction
analysis. The results showed that the gas permeability was significantly influenced by powder structure. The gas permeability
of YSZ coating deposited by fused-crushed powder is one order lower in magnitude than that by agglomerated powder. Moreover,
the gas permeability of YSZ deposited by LPPS is lower than that of APS YSZ. The electrical conductivity of the deposits through
thickness direction was measured by potentiostat/galvanostat based on three-electrode assembly approach. The electrical conductivity
of YSZ coating deposited by low pressure plasma spraying with fused-crushed powder of small particle size was 0.043 S cm−1 at 100 °C, which is about 20% higher than that of atmospheric plasma spraying YSZ with the same powder.
This article was originally published inBuilding on 100 Years of Success, Proceedings of the 2006 International Thermal Spray Conference (Seattle, WA), May 15–18, 2006, B.R. Marple, M.M. Hyland, Y.-Ch. Lau, R.S. Lima, and J. Voyer, Ed., ASM International, Materials
Park, OH, 2006. 相似文献
7.
氧化物掺杂YSZ热障涂层的最新研究进展 总被引:1,自引:0,他引:1
随着先进航空发动机涡轮叶片热障涂层服役温度、服役寿命以及隔热性能的不断提升,研制温度高、使用寿命长和隔热性能优异的热障涂层材料,已成为国际高温防护涂层领域的研究热点。氧化物掺杂YSZ涂层因其良好的热学性能,成为最有可能替代YSZ涂层在航空发动机热端部件表面获得应用的热障涂层材料。综述了氧化物掺杂YSZ热障涂层研究取得的成果和存在的问题,重点阐述了不同氧化物掺杂对YSZ涂层性能的影响机理,并简述了目前国内外对该类涂层相关制备技术的研究进展。提出未来关于热障涂层的研究,应在进一步优化设计多元氧化物掺杂改性YSZ涂层的基础上,结合计算模拟,对多元氧化物掺杂的耦合作用机制进行深入剖析,同时结合新一代高温合金的性质,发展高温合金-粘结层-陶瓷层相匹配的新型热障涂层体系,从热力学-动力学两个方面考察其使役行为和失效机制,最终促进该类涂层的实际应用。 相似文献
8.
TiAl合金具有低密度、高比强度的优异性能,是一种潜在的航空发动机用结构材料。TiAl合金的服役温度范围为700~900℃,在其表面制备高温热防护涂层可以进一步提高服役温度。本研究采用等离子喷涂技术在TiAl合金表面制备了新型TiAlCrY/YSZ涂层,并与传统的NiCrAlY/YSZ热障涂层进行高温长时间服役性能对比研究。结果发现, TiAlCrY/YSZ涂层在1100℃空气环境中服役300 h保持完好,表现出良好的高温性能,而NiCrAlY/YSZ涂层在1100℃的服役寿命不足100 h。显微分析结果表明, TiAlCrY黏结层表面会形成一层连续且致密的TGO,其主要成分为Al2O3,与YSZ涂层的界面兼容性良好。并且TGO在1100℃空气环境中服役300 h后,厚度仍<8μm。以上研究表明,与传统NiCrAlY/YSZ热障涂层相比, TiAlCrY/YSZ更适合作为TiAl合金表面的高温热防护涂层。 相似文献
9.
10.
A physical model describing the I(V) characteristics of planar limiting current oxygen sensors based in an ion-conducting electrolyte is presented. The model focuses on the minimization of the electrochemical potential and the diffusion across a porous layer covering the measuring electrode. The proposed model describes three key phenomena in the response of the sensors: the influence of the polarization resistance on the slope of I(V), the linearity between the limiting current and the diffusivity of the porous layer and a low non-zero current at zero polarization. 相似文献