欢迎登录材料期刊网

材料期刊网

高级检索

The electron beam local post-weld heat treatment (EBLPWHT) is a rather new method that provides the advantages ofhigh precision, flexibility and efficiency, energy saving and higher productivity. This paper studies the effect of two post-weldheat treatment processes on the microstructure, mechanical properties and fracture toughness of an electron beam weldedjoints in 30CrMnSiNi2A steel. EBLPWHT, in a vacuum chamber, immediately after welding and a traditional furnace wholepost-weld heat treatment (FWPWHT) were compared. The experimental results show that, after EBLPWHT treatment, themain microstructure of weld was changed from coarse acicular martensite into lath martensite, HAZ was changed from lathmartensite, bainite into lower bainite, and base metal was changed from ferrite and pearlite into upper bainite and residualaustenite. The microstructures of different zones of joints in FWPWHT condition were tempered sorbite. The properties ofwelded joints can be improved by the EBLPWHT in some extent, and especially largely for the fracture toughness of weldedjoints. However the value of fracture toughness of base metal is comparatively low, so appropriate heat treatment parametersshould be explored in the future.

参考文献

[1] T. Sebastiano;N. Fabio;D. M. Marcello .Electron beam welding and post-weld treatments of steels[J].Journal of Materials Science Letters,1996(10):827-830.
[2] Wang Chienchun;Chang Yih .[J].Metallurgical and Materials Transactions A:Physical Metallurgy and Materials Science,1996,27A(10):3162.
[3] C C Huang;Y C Pan;T H Chuang .[J].Journal of Materials Engineering and Performance,1997,6(01):61.
[4] G Cam;S Erimm;C Yeni;M Kocak .[J].Welding Journal,1999,78(06):193s.
[5] BS7448(part1-Method for determination of KIC, critical CTOD and critical J values of metallic material[Z].,1993.
[6] BS7448(part2)-Method for determination of KIC, critical CTOD and critical J values of welds in metallic material[Z].,1997.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%