Strength Estimation and Residual Stress Analysis of Thermal Barrier Coatings by Synchrotron Radiations.
Strength Estimation and Residual Stress Analysis of Thermal Barrier Coatings by Synchrotron Radiations.
批准号:
13650078
负责人:
SUZUKI Kenji
金额:
$1.15万
依托单位:
依托单位国家:
日本
项目类别:
Grant-in-Aid for Scientific Research (C)
财政年份:
2001
资助国家:
日本
项目状态:
已结题
起止时间:
2001 至 2003
中文摘要
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英文摘要
As a bond coating, NiCoCrAlY was plasma sprayed oh the substrate of Ni super alloy and a top coating of the specimen was made by air-plasma spraying. High energy X-rays from a synchrotron source has a large penetration depth. A special furnace was made for the in-situ stress measurement in high temperature. This furnace was attached on a 4-circle goniometer at a beam line BL02B1 in SPring-8. Using high energy X-rays with 72keV, the internal stress of the bond coating was measured nondestructively through the top coating with the increase in temperature. At 1073 K or higher, the internal stress in the bond coat was released due to softening of the bond coat. The change of internal stresses in the bond coat with temperatures was explained by thermal mismatch of expansion between top and bond coats.A new hybrid method was proposed to evaluate a spalling stress. The in-plane stress in the thermal barrier coatin can be measured with laboratory X-rays, and the out-of-plane stress can be meas … More ured with high energy synchrotron X-rays. Combining these stresses obtained by the low and high energy X-rays, the distribution of the spalling stress was evaluated. To oxidize the specimen, the specimens were kept in air at 1373 K for 0,500,1000 and 2000h. The cross section of each oxidized specimen was observed with a scanning electron microscope. The thermally grown oxide(TGO) consists of the alumina layer and the composite oxide layer. The thickness of alumina layer stopped to increase after 500h exposure, while the thickness of the composite oxide layer incresed monotonically. The TGO grew at the convex part of the bond coating, and pushed up the top coating. As a result, the spalling crack was initiated near the convex part. The spalling stress for each oxidized specimen was estimated by the hybrid method using the stress data obtained by laboratory X-rays and high energy synchrotron X-rays. The top coating without the oxidization did not have the spalling stress. For the oxidized specimen, the spalling stress was small beneath the surface, and steeply increased near the interface between the top and the bond coating. The spalling stress near the interface was about 200 MPa. The distribution of the spalling stress for the case of the 1000h exposure was similar to that for the case of 500h. The TGO promotes the spallation of the top coating, and the distribution of the spalling stress corresponds to the observed position of spalling cracks. Less
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鈴木賢治: "高エネルギー放射光による遮熱コーティングのボンドコートの高温その場応力測定"材料. 52. 756-763 (2003)
Kenji Suzuki:“使用高能同步辐射的热障涂层粘合层的高温原位应力测量”材料 52. 756-763 (2003)。
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柳瀬悦也, 西尾光司, 楠見之博, 新井和夫, 鈴木賢治, 秋庭義明, 東海博央, 田中啓介: "放射光高エネルギX線を用いたショットピーニング処理した鉄鋼の残留応力分布の評価"材料. 51. 756-763 (2002)
Etsuya Yanase、Koji Nishio、Yukihiro Kusumi、Kazuo Arai、Kenji Suzuki、Yoshiaki Akiba、Hiroo Tokai、Keisuke Tanaka:“使用同步加速器高能 X 射线评估喷丸钢中的残余应力分布”材料。 763(2002)
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S.Machiya: "X-ray stress measurement and deformation behavior of zirconia thermal barrier coatings"Proceedings of ATEM'03. OS04W0430. 1-6 (2003)
S.Machiya:“氧化锆热障涂层的X射线应力测量和变形行为”ATEM03论文集。
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鈴木賢治, 田中啓介, 秋庭義明, 川村昌志, 西尾光司, 尾角英毅: "高エネルギーX線によるTBCの残留応用力分布解析"第38回X線材料強度に関するシンポジウム. 99-104 (2002)
Kenji Suzuki、Keisuke Tanaka、Yoshiaki Akiba、Masashi Kawamura、Koji Nishio、Hideki Ozuno:“高能 X 射线对 TBC 中残余作用力分布的分析”第 38 届 X 射线材料强度研讨会(2002 年)。
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田中啓介: "放射光高エネルギX線によるショットピーニング材の残留応力測定"第37回X線材料強度に関する講演論文集. 72-77 (2001)
Keisuke Tanaka:“使用同步加速器高能 X 射线测量喷丸材料中的残余应力”第 37 届 X 射线材料强度讲座论文集(2001 年)。
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