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Interfacial delamination mechanism of thermal barrier coatings with real microstructure considering gradient thermal and growth strains based on the fracture phase field
被引:0
作者:
Xiao, Y. Q.
[1
,2
]
Liu, Z. Y.
[3
]
Zhu, W.
[4
]
Peng, X. M.
[1
,2
]
机构:
[1] Hunan Inst Engn, Dept Mech Engn, Hunan Prov Key Lab Vehicle Power & Transmiss Syst, Xiangtan 411104, Peoples R China
[2] Hunan Inst Engn, Hunan Prov Engn Lab Wind Power Operat Maintenance, Xiangtan 411104, Peoples R China
[3] Cent South Univ Forestry & Technol, Sch Mat Sci & Engn, Changsha 410004, Hunan, Peoples R China
[4] Xiangtan Univ, Sch Mat Sci & Engn, Key Lab Low Dimens Mat & Applicat Technol, Minist Educ, Xiangtan 411105, Hunan, Peoples R China
基金:
中国国家自然科学基金;
关键词:
Thermal barrier coatings;
Delamination mechanism;
Thermally grown oxide;
Real microstructure;
Phase field method;
RESIDUAL-STRESS;
TGO GROWTH;
EB-PVD;
BEHAVIOR;
CRACKING;
SYSTEMS;
OXIDE;
EVOLUTION;
D O I:
10.1016/j.matchar.2024.114014
中图分类号:
T [工业技术];
学科分类号:
08 ;
摘要:
The interface of atmospheric plasma spray (APS) thermal barrier coatings (TBCs) is highly irregular and rough, while their microstructure is porous and extremely uneven. This complexity leads to intricate patterns during the growth of thermally grown oxide (TGO), the distribution and evolution of the generated stress, as well as the initiation and expansion of cracks. Along these lines, in this work, a phase-field theory considering both the thermal gradient strain and TGO growth was established to thoroughly investigate the interface oxidation cracking in TBCs. More specifically, a two-dimensional geometric model of APS TBCs was established, incorporating real interface morphology and microstructure. Numerical simulations and experiments were also conducted to study the temperature and stress distribution, as well as the underlying mechanism of interface cracking during the service of TBCs. The results indicated that at high temperatures, the bottom temperature of the top coating (TC) layer with a porosity of 3.1% and a thickness of 200 mu m was approximately 5 degrees C lower than that of the TC layer without porosity. Compared to the ideal model without pores, the model considering the real microstructure, with the presence of microcracks in the TC, makes it easier for the normal stress in the TGO at the peak region to be released. The inter-lamella cracks (Type A) in the TC near the peaks initiated earliest, followed by the creation of inter-lamella cracks at other locations, accompanied by the appearance of lamella-fracture cracks (Type B), inter-lamella to interfacial cracks (Type C), inter-lamella to TGO cracks (Type D), and internal TGO cracks (Type E). The coalescence of all these types of cracks will ultimately lead to coating failure.
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