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用波长为1.06μm的Nd:YAG激光器对厚度为0.08 mm的超薄不锈钢片进行激光密封焊接,通过调节脉冲激光的频率、脉宽、焊接速度、离焦量等工艺参数成功地对超薄不锈钢片进行了脉冲激光焊接。本文重点研究了焊接光斑重叠率对焊缝密封性的影响,并详细讨论了影响光斑重叠率的主要因素:脉冲频率、焊接速度、光斑大小之间的关系。 相似文献
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基于金属材料熔化、汽化界面二维扩展机制建立了脉冲激光的焊接模型。该模型是将激光作用区和脉冲作用时间分离为离散单元后计算焊缝断面形状的,提出以深熔小孔中的腔内光强动态再分布机理更精确地描述焊缝断面形状。腔内光强再分布机制主要考虑腔壁菲涅耳反射。光强叠加是基于与入射角无关的相干强度叠加。每次反射后的位置单元的确定采用光线追迹法。数值模型分别算出功率P、光斑尺寸α、吸收率α(材料一定,波长变化,吸收率亦改变)等参数变化所导致的液相线断面曲线的变化,并给出作用时间变化时,断面曲线的变化规律。计算结果表明,焊缝断面形状受脉冲功率、光斑直径、脉冲作用时间影响较大,这和实际的焊接情况吻合,同时,理论结果也可解释焊缝断面曲线走向突变现象。 相似文献
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对奥氏体不锈钢的焊接性进行了分析.针对容器制造的特点,制定了双人钨极氩弧焊打底、埋弧焊盖面的焊接工艺并用于产品的焊接,取得了良好效果. 相似文献
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针对不锈钢薄板的激光焊接进行了研究,分析了激光工艺参数对超薄不锈钢板焊接质量的影响。结果表明,对于不锈钢薄板激光焊接,脉冲工作电流和脉冲宽度对焊缝成形影响很大。在合适的工艺参数下,超薄不锈钢薄板焊缝成形良好,焊接接头基本与母材等强。 相似文献
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采用额定功率为5KW连续可调的CO2横流激光器,研究了激光的输出功率和焊接地2mm厚1r18Ni9Ti奥氏体不锈钢的力学性能指标(抗拉经度σb,屈服强度σ0.65)的影响规律;并且通过分析得到了激光焊接1Cr18Ni9Ti薄板的最佳工艺参数。 相似文献
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激光焊接锋利型小锯片配方的研制 总被引:3,自引:0,他引:3
激光焊接小锯片刀头是通过热压烧结而成,其刀头比以往整体的烧结的刀头致密,但锋利度不够,针对如何提高激光焊接小锯片的锋利性问题,本文主要研究了铁含量,添加元素成分以及金刚石品质,浓度,粒度等对锯片锋利度的影响。 相似文献
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铝合金脉冲激光焊接能够精准调节激光能量输入,广泛应用于动力电池与新能源汽车等精密加工领域。然而,铝合金自身高导热率和高反射率等固有属性,以及与高能量激光剧烈的相互耦合作用,对工艺参数优化和焊接质量控制带来挑战。以2 mm厚1060铝合金作为研究对象,主要分析了不同脉冲激光工艺参数(峰值功率、脉冲频率和焊接速度)对焊缝成形的影响规律;以工艺参数为多维输入变量,进一步构建了基于BP神经网络的熔池尺寸预测模型。结果表明:不同工艺参数均对焊缝熔深和熔宽有直接影响,需要确定一个合适的工艺窗口;同时构建模型的平均预测误差在10%以内,具有较高的预测精度。为铝合金脉冲激光焊接质量预测及工艺优化提供了可靠的实验和指导依据。 相似文献
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超薄不锈钢激光精密缝焊工艺 总被引:1,自引:0,他引:1
以304超薄不锈钢片作为试验材料,使用YAG激光嚣进行精密缝焊试验,详细研究了脉冲能量、脉冲宽度、脉冲频率及离焦量的变化对焊缝成形的影响.此外,对激光脉冲宽度及脉冲频率对焊缝宽度的影响作了深入研究.试验结果表明:焊接电流为78 A,频率为10Hz,脉冲宽度1 ms,正离焦量2mm时,可对0.15mm超薄304不镑钢实现精密缝焊,得到光滑美观的焊缝;随着电流及脉宽的增加,焊缝宽度增大,并出现飞溅,最后试样被氧化烧穿;随着脉冲频率升高,焊点重叠率增加,焊缝宽度增大,并且越来越光滑,但试样的下表面逐渐出现氧化;对于薄板材料的焊接,正离焦比负离焦易得到光滑美观的焊缝. 相似文献
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采用YLS-6000型激光焊接系统对304不锈钢进行穿透焊,研究激光功率和离焦量对T形接头焊缝成形、显微组织和显微硬度的影响。结果表明,随着激光功率的增加,焊缝的熔深、熔宽和搭接处焊缝宽度都增大;焊缝搭接处焊缝宽度在离焦量为-2 mm时达到最大,同时考虑深宽比,离焦量为0 mm时焊缝成形较好;焊缝区组织为以奥氏体柱状晶为基体,间隙中分布着网状δ铁素体;焊缝区硬度略低于母材,且随着激光功率的增加,焊缝区组织粗化,硬度降低。创新点:对不锈钢T形接头进行了激光穿透焊接,较为系统的分析了激光功率、离焦量等对焊缝成形的影响。综合考虑搭接处焊缝宽度和熔深,离焦量为0 mm时,焊缝成形最好。 相似文献
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超薄不锈钢片微激光焊接的焊缝成形 总被引:4,自引:0,他引:4
采用微型脉冲激光实现了0.2 mm厚321不锈钢片的对接焊,研究了脉冲频率、脉冲宽度和脉冲功率等工艺参数对焊缝成形的影响规律.结果表明,0.2 mm厚321不锈钢片的微激光对接焊容易在焊缝处产生烧穿,在收弧处形成较深的弧坑.在其它工艺参数固定不变时,减小脉冲频率和脉冲宽度均可以减少或避免焊缝的烧穿,改善焊缝成形;减小脉冲功率有利于避免焊缝收弧处较深弧坑的形成,但脉冲功率过小会导致未焊合.当脉冲功率分数为12%时,脉冲频率在较宽的范围内变化都能获得成形良好、无缺陷的焊接接头.焊缝组织由中心部位的等轴晶和边缘细小的柱状晶组成,在焊缝和母材的交界处几乎不存在焊接热影响区. 相似文献
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Katsutoshi Takano Norikiyo Koizumi Hisashi Serizawa Shuho Tsubota Yoshinobu Makino 《Welding International》2017,31(11):827-836
The radial stainless steel plates (RPs) used for Toroidal field (TF) coils in the International Thermonuclear Experimental Reactor (ITER) are 13 m long, 9 m wide and 10 cm thick, which are quite large. Even though they are very large structures, high manufacturing tolerances and high mechanical strength at 4 K are required. It is also required that each RP should be fabricated every three weeks. Therefore, the authors intend to develop efficient manufacturing methods for an ITER TF coil RP. Laser welding is then selected as a welding method for RP. Especially, the development of high technology laser welding is necessary to prevent hot cracking in the material used for the RP; namely, fully austenitic stainless steel with high nitrogen content. The authors carried out trial laser welding experiments aiming at its application to RP. As a result, it was effective to make the angle of back inclination of the weld head at a uniform welding speed. It also seemed that the sensitivity of hot cracking could be reduced by optimizing the chemical compositions of material used for RP. The base material and the welded joints satisfied mechanical properties in 4 K. The application of the laser welding technology to the fully austenitic stainless steel was therefore demonstrated. 相似文献
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Analysis on characteristics of laser induced plasma during laser welding of A304 stainless steel sheet 下载免费PDF全文
A group of the stainless steel laser welding was performed using continuous wave (CW) laser and pulsed laser. During the welding process the laser induced plasma behavior was recorded by high-speed video camera, while the plasma spectrum was acquired by the spectrometer. The plasma temperature was calculated based on the spectroscopic analysis of the optical emission and the results show that different output mode of laser source led to big difference of plasma temperature. The high-speed video images showed that the plasma was very steady and kept certain strength in CW laser welding, while the plasma erupted a little later after the laser peak arising during the pulsed laser welding. During a period of time about 2ms just after the laser peak arising during the pulsed laser welding, much more laser energy reached the workpiece. This made the workpiece fully penetrated with a lower average power. 相似文献