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采用超音速火焰喷涂+大气等离子喷涂工艺,在K403高温合金表面制备不同层厚比的NiCrAlY/纳米7YSZ热障涂层,研究了涂层厚度变化对热障涂层表面粗糙度、结合强度、热震性能和热循环寿命的影响规律.结果表明:当粘结层厚度一定时,随着陶瓷层厚度的增加,其表面粗糙度增加,涂层结合强度下降;当粘结层厚度为50 μm时,热障涂层的抗热震性能随陶瓷层厚度增加而降低,粘结层厚度提高至100 μm时,热障涂层的抗热震性能随陶瓷层厚度增加先提高,后降低,热障涂层在1100℃的热循环寿命测试结果也基本对应这一规律;当粘结层厚50μm且陶瓷层/粘结层的层厚比在(1~2)∶1的范围内,或者粘结层厚100 μm且陶瓷层/粘结层的层厚比在(2~2.5)∶1范围内时,热障涂层具有较优异的性能.

参考文献

[1] MEIER S M;GUPTA D K .The Evolution of Thermal Barrier Coatings in Gas Turbine Engine Applications[J].Transactions of the ASME,1994,116:250-257.
[2] Clarke DR. .Materials selection guidelines for low thermal conductivity thermal barrier coatings[J].Surface & Coatings Technology,2003(0):67-74.
[3] David R. Clarke;Simon R. Phillpot .Thermal barrier coating materials[J].Materials Today,2005(6):22-29.
[4] Nitin P. Padture;Maurice Gell;Eric H. Jordan .Thermal Barrier Coatings for Gas-Turbine Engine Applications[J].Science,2002(5566):280-284.
[5] MURPHYA K S;MORE K L;LANCE M J.As-deposited Mixed Zone in Thermally Grown Oxide Beneath a Thermal Barrier Coating[J].Surface and Coatings Technology,2001(146/147):152-161.
[6] P. Y. Hou .Segregation behavior at TGO/bondcoat interfaces[J].Journal of Materials Science,2009(7):1711-1725.
[7] Balint DS;Xu T;Hutchinson JW;Evans AG .Influence of bond coat thickness on the cyclic rumpling of thermally grown oxides[J].Acta materialia,2006(7):1815-1820.
[8] TAYLOR T A;APPLEBY D L;WEATHERILL A E.Plasma Sprayed Yttria Stabilized Zirconia Coatings:Structure Property Relationships[J].Surface and Coatings Technology,1990(43/44):470-480.
[9] Choi HM.;Choi WK.;Choi DG.;Choi SK.;Kim JC.;Park YK.;Kim GM.;Kang BS. .Effect of the thickness of plasma-sprayed coating on bond strength and thermal fatigue characteristics[J].Journal of Materials Science,1998(24):5895-5899.
[10] AHRENS M;LAMPENSCHERF S;VASSEN R et al.Sintering and Creep Processes in Plasma-sprayed Thermal Barrier Coatings[J].Journal of Thermal Spray Technology,2004,13(03):432-442.
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