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  1. National Taiwan Ocean University Research Hub
  2. 電機資訊學院
  3. 光電與材料科技學系
請用此 Handle URI 來引用此文件: http://scholars.ntou.edu.tw/handle/123456789/4706
DC 欄位值語言
dc.contributor.authorTai-Jung Wuen_US
dc.contributor.authorChien-Chun Liaoen_US
dc.contributor.authorTai-Cheng Chenen_US
dc.contributor.authorRen-Kae Shiueen_US
dc.contributor.authorLeu-Wen Tsayen_US
dc.date.accessioned2020-11-19T02:23:45Z-
dc.date.available2020-11-19T02:23:45Z-
dc.date.issued2019-12-
dc.identifier.urihttp://scholars.ntou.edu.tw/handle/123456789/4706-
dc.description.abstractT92 steel tubes have been widely applied in advanced supercritical boilers to replace Gr.91 tubes. Simulated samples with microstructures similar to those present in the heat-affected zone (HAZ) of a T92 steel weld were subjected to short-term creep tests in the study. T92 steel tubes were normalized at either 1213 K (L) or 1333 K (H) for 1 h, followed by tempering (T) at 1033 K for 2 h. After the normalizing and tempering treatments, the HT samples comprised finer precipitates but in greater numbers along the prior austenite grain boundaries (PAGBs) and martensite lath boundaries, as compared with those of the LT samples. The HAZ microstructures in the T92 steel welds were simulated by using an infrared heating system, which included over-tempering (OT, below AC1) and partial transformation (PT, slightly below AC3) zones. Martensite laths in the OT sample were more likely to be replaced by numerous cellular structures or subgrains together with spherodized carbides mainly located at the lath and austenite grain boundaries. Furthermore, coarser but fewer carbides were found along the refined lath and grain boundaries in the PT samples, in comparison with other samples in each group. Short-term creep tests showed that the PT samples were more likely to fracture than other samples in each group. Moreover, under the same testing conditions, the microstructures of T92 steel were more stable and resistant to degradation than those of T91 steel after welding or loading at elevated temperatures. Such events were responsible for higher creep resistance of the simulated T92 samples than that of the simulated T91 samples under the same creep-rupture conditions.en_US
dc.language.isoenen_US
dc.relation.ispartofMetalsen_US
dc.subjectT92en_US
dc.subjectthermal simulationen_US
dc.subjectheat-affected zoneen_US
dc.subjectcreepen_US
dc.titleMicrostructural Evolution and Short-Term Creep Rupture of the Simulated HAZ in T92 Steel Normalized at Different Temperaturesen_US
dc.typejournal articleen_US
dc.identifier.doi10.3390/met9121310-
dc.identifier.isiWOS:000506637800070-
dc.relation.journalvolume9en_US
dc.relation.journalissue12en_US
dc.relation.pages1310en_US
item.openairetypejournal article-
item.fulltextno fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_6501-
item.grantfulltextnone-
item.cerifentitytypePublications-
item.languageiso639-1en-
crisitem.author.deptCollege of Electrical Engineering and Computer Science-
crisitem.author.deptDepartment of Optoelectronics and Materials Technology-
crisitem.author.deptNational Taiwan Ocean University,NTOU-
crisitem.author.deptCenter of Excellence for Ocean Engineering-
crisitem.author.orcid0000-0003-1644-9745-
crisitem.author.parentorgNational Taiwan Ocean University,NTOU-
crisitem.author.parentorgCollege of Electrical Engineering and Computer Science-
crisitem.author.parentorgNational Taiwan Ocean University,NTOU-
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