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首页> 外文期刊>Metallurgical and Materials Transactions, A. Physical Metallurgy and Materials Science >The Effects of Process Variables on Pulsed Nd: YAG Laser Spot Welds: Part II.AA 1100 Aluminum and Comparison to AISI 409 Stainless Steel
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The Effects of Process Variables on Pulsed Nd: YAG Laser Spot Welds: Part II.AA 1100 Aluminum and Comparison to AISI 409 Stainless Steel

机译:工艺变量对脉冲Nd:YAG激光点焊的影响:第二部分.AA 1100铝和与AISI 409不锈钢的比较

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摘要

In this two-part article ,the weldabilities of AA1100 aluminum and AISI 409 stainless steel by the pulsed Nd :YAG laser welding process have been examined experimentallyand compared .The effects of laser pulse time and power density onlaser spot weld characteristics ,such as welddiameter ,penetration ,melt area ,melting ratio ,porosity ,andsurface catering ,have been studied and explained qualitatively inrelation to material-dependent variables such as absorptivity andthermophysical properties .The weldability of AISI 409 stainlesssteel was reported in Part I of this article .In the present article ,theweldability of AA 1100 aluminum is reported and compared tothat of AISI 409 stainless steel .Weld pool shapes in aluminumwere found to be influenced by the mean power density of the laserbeam and the laser pulse time .Both conduction-mode andkeyhole-mode welding were observed in aluminum .Unlikestainless steel ,however ,drilling was not observed .Conduction-mode welds were produced in aluminum at power densitiesranging from 3.2 to 10GW/m2 .The power density required formelting aluminum was approximately 4.5 times greater thanstainless steel .The initial transient in weld pool development inaluminum occurred within 2 ms ,and the aspect ratios (depth/width)of the steady-state conduction-mode pools were approximately0.2.These values are about half those observed in stainlesssteel .The transition from conduction- to keyhole-mode weldingoccurred in aluminum at a power density of about10GW/m2 ,compared to about 4GW/m2 for stainless steel .Welddefects such as porosity and cratering were observed in bothaluminum and stainless steel spot welds .In both materials ,therewas an increased propensity for large occluded vapor pores nearthe root of keyhole-mode welds with increasing power density .Inaluminum ,pores were observed close to the fusionboundary .These could be eliminated by surface milling andvacuum annealing the specimens ,suggesting that such pored weredue to hydrogen .Finally ,excellent agreement was obtainedbetween experimental data from both alloys and an existinganalytical model for conduction-mode laser spot welding .Twonondimensional parameters ,the Fourier number and anondimensional incident heat flux parameter ,were derived andshown to completely characterize weld pool development inconduction-mode welds made in both materials.
机译:在这一由两部分组成的文章中,对Nd:YAG脉冲激光焊接工艺对AA1100铝和AISI 409不锈钢的可焊性进行了实验研究,并进行了比较。激光脉冲时间和功率密度对激光点焊特性(例如焊缝直径,已经研究并定性地解释了熔深,熔体面积,熔解率,孔隙率和表面适应性与材料相关变量(例如吸收率和热物理性能)的关系。本文第一部分报道了AISI 409不锈钢的可焊接性。报道了AA 1100铝的可焊接性,并将其与AISI 409不锈钢进行了比较。发现铝的熔池形状受激光束的平均功率密度和激光脉冲时间的影响。观察到导电模式和锁孔模式焊接在铝中。与不锈钢不同,但是未观察到钻孔。铝的功率密度范围为3.2至10GW / m2。熔化铝所需的功率密度约为不锈钢的4.5倍。铝的熔池发展的初始瞬变发生在2 ms内,并且稳定的长宽比(深度/宽度)态导通模式池约为0.2。这些值是不锈钢中观察到的值的一半。铝在功率密度约为10GW / m2时发生了从导通模式到锁孔模式焊接的转变,而不锈钢的功率密度约为4GW / m2在铝和不锈钢点焊中都观察到了诸如气孔和缩孔的焊接缺陷。在两种材料中,键孔型焊缝根部附近的大闭塞气孔的功率都随着功率密度的增加而增加。铝,观察到的孔接近这些可以通过表面铣削和真空退火样品消除,这表明这种孔是由于氢引起的。最后,在两种合金的实验数据与现有的传导模式激光点焊分析模型之间取得了很好的一致性。推导并显示了二维参数,傅立叶数和非三维入射热通量参数,从而完全表征了传导模式焊缝的熔池发展。在两种材料中。

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