High pwder Nd-YAG laser welding of SiC particle reinforced aluminium alloy 2124

1998 ◽  
Vol 14 (9) ◽  
pp. 906-912 ◽  
Author(s):  
T. M. Yue ◽  
J. H. Du ◽  
H. C. Man
1998 ◽  
Vol 14 (9-10) ◽  
pp. 906-912 ◽  
Author(s):  
T. M. Yue ◽  
J. H. Du ◽  
H. C. Man

2003 ◽  
Vol 8 (4) ◽  
pp. 246-256 ◽  
Author(s):  
M. G. Deutsch ◽  
A. Punkari ◽  
D. C. Weckman ◽  
H. W. Kerr

2009 ◽  
Vol 23 (10) ◽  
pp. 753-762 ◽  
Author(s):  
Seiji Katayama ◽  
Satoshi Kawaguchi ◽  
Masami Mizutani ◽  
Yousuke Kawahito ◽  
Taishi Tarui

2018 ◽  
Vol 262 ◽  
pp. 411-421 ◽  
Author(s):  
Indhu R. ◽  
Soundarapandian S. ◽  
Vijayaraghavan L.

2009 ◽  
Vol 519 (1-2) ◽  
pp. 167-171 ◽  
Author(s):  
F. Malek Ghaini ◽  
M. Sheikhi ◽  
M.J. Torkamany ◽  
J. Sabbaghzadeh

2002 ◽  
Vol 396-402 ◽  
pp. 1691-1696 ◽  
Author(s):  
Reinhold Braun ◽  
Günther Roth ◽  
Johannes Arnold

2011 ◽  
Vol 287-290 ◽  
pp. 2401-2406 ◽  
Author(s):  
Ai Qin Duan ◽  
Shui Li Gong

In this paper, the keyhole of YAG laser welding 5A90 Al-Li alloy was observed and measured through the high speed camera. The characteristics of the keyhole and the effects of welding parameters were studied. The characteristics of the absorption of laser energy and the susceptivity for heat input in welding 5A90 were given. The results show that in this welding condition, the keyhole of laser welding 5A90 is nearly a taper and the highest temperature area is in the bottom. There are clear effects of heat input on the characteristics, especially the surface radius of keyhole and plasma/vapor in keyhole. Another phenomena is observed that sometime plasma/vapor could disappear in 0.3ms welding time, and this feature will be more remarkable as decrease of heat input. It shows that the absorption of energy is unsteady. It is known that when this instability reaches a certain value, an unsteady weld will be formed.


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