聚变堆用CLF-1 钢与316L 钢TIG 焊接接头组织与性能初步研究

对用W19123L 为焊丝的聚变堆用低活化CLF-1 钢与316L 钢的钨极氩弧焊(TIG)焊接接头金相组织及性能进行了初步研究。结果表明：焊接接头成型良好、无缺陷;金相组织表明焊接接头由CLF-1 侧(母材区、热影响区、熔合区)、过渡层、焊缝区、316L 侧(母材区、热影响区、熔合区)组成;室温拉伸试验结果优于母材的最低要求值;弯曲试验后的焊接接头内外表面完好,无裂纹产生,变形均匀;焊接接头冲击值成凹型分布,焊缝区冲击值最低,焊缝两侧热影响区冲击值次之,母材冲击值最高,316L 侧冲击值略高于CLF-1 侧,均满足焊接接头设计值;焊接接头上表面1.6mm 硬度波动较大,略高于1/2T 和下表面1.6mm 处,焊接接头1/2T 和下表面1.6mm 硬度分布较均匀,从CLF-1 侧到316L 侧有下降趋势。整体焊接性能基本稳定,满足异种钢焊接性能匹配要求。     

低活化马氏体钢热等静压焊接接头性能初步研究

研究了低活化马氏体钢(CLF-1)热等静压(HIP)焊接接头的性能,经980℃/1h/空冷+740℃/2h/空冷的性能热处理后,接头组织保持着CLF-1钢母材回火马氏体组织;常温拉伸性能与母材相当,断口为韧窝状且有第二相粒子产生,为塑性断裂且断于焊缝;常温冲击功最高为母材的26.2%。初步分析认为焊接表面制备状态、表面污染物、表面清洗状态、表面氧化膜都会影响基体原子充分扩散,导致界面扩散层不均匀,焊缝裂纹敏感性增强,冲击功低,且不稳定。     

用磁搅拌技术减轻和消除铍的焊接缺陷

在焊接时利用电磁搅拌技术可以起到细化晶粒，减轻或消除各种焊接缺陷的作用，有利于焊接接头质量的提高。电磁搅拌是在交变磁场的作用下产生的电磁力迫使焊缝熔池的液态金属改变原有运动模式和结晶状态，从而达到控制焊缝凝固组织、减少焊接缺陷的目的。电磁场与焊缝金属的相互作用有2个显著特点：使枝晶破碎、游离，加速枝状晶向等轴晶转变，扩大等轴晶的形成，使晶粒细化；促使焊缝气泡的分离与浮出，对减轻和消除焊接气孔有利。铍的熔焊由于结晶组织粗大和焊缝的高应力状态将导致焊缝开裂。采用高能束（激光）焊接，并且在进行铍的熔焊时加Al-si合金填充材料，再辅以合适的焊接工艺措施可以改善铍的焊接性能和防止铍的开裂。采用磁搅拌技术减轻和消除铍的焊接缺陷，需要在技术上考虑3方面的问题：（1）铍和Al-si合金填充材料都是非磁性材料，非磁性材料对电磁搅拌产生何种效果和影响。（2）与TIG（氩弧焊）焊接相比，激光焊接为无焊接电弧柔性载流导体，电磁场能否对激光焊接实现搅拌。（3）磁场应加在焊缝区域的什么位置才能使搅拌获得良好的效果。对于非磁性材料又无焊接电弧柔性载流导体的激光焊接，交变磁场式电磁搅拌装置显然对熔池起不到搅拌作用，焊缝的原有液态金属的运动规律不能被打乱，起不到细化晶粒和消除焊接缺陷的目的。     

低活化马氏体钢热等静压焊接接头性能初步研究

研究了低活化马氏体钢(CLF-1)热等静压(HIP)焊接接头的性能,经980℃/1h/空冷+740℃/2h/空冷的性能热处理后,接头组织保持着CLF-1钢母材回火马氏体组织;常温拉伸性能与母材相当,断口为韧窝状且有第二相粒子产生,为塑性断裂且断于焊缝;常温冲击功最高为母材的26.2%。初步分析认为焊接表面制备状态、表面污染物、表面清洗状态、表面氧化膜都会影响基体原子充分扩散,导致界面扩散层不均匀,焊缝裂纹敏感性增强,冲击功低,且不稳定。     

钨/低活化钢钎焊用铁基非晶钎料与接头微结构

为了连接W和CLF-1 RAFM钢,设计出由低活化元素组成的Fe-B-Si、Fe-B-Si-Sn、Fe-B-Si-Cr-(Sn)、Fe-B-Si-P-(Cr,Sn)、Fe-B-Si-Mn-(Ga,Sn)和Fe-B-Si-(Cr,Mn,Ga,Ta,Sn)系列Fe基非晶钎料,结合熔体快淬技术制备出非晶合金箔带,并对W/CLF-1 RAFM钢接头微结构进行了对比研究。采用X-射线衍射仪对箔带样品与焊缝进行了相鉴定;通过差热分析测量了非晶箔带的熔化温度和液相线温度;利用光学金相和电子探针分析了焊缝组织形貌和元素分布。结果表明,利用Fe-B-Si、Fe-B-Si-Cr和Fe-B-Si-Mn-Sn非晶钎料可获得结构完整的W/CLF-1钢接头;前两种钎料得到的焊缝组织基体相为α-Fe固溶体,而含Mn钎料形成的焊缝基体为马氏体组织;在高温钎焊过程中,这些Fe基非晶钎料中的高B含量促使FeWB、FeW2B2和Fe3B型金属间化合物在焊缝中形成,并有效地阻止了W元素向低活化钢基体长程扩散。所设计的低活化Fe基非晶钎料可用于W和低活化钢的连接和接头性能研究。     

人工吸收杂质诱导增透膜损伤阈值研究

为研究杂质大小对增透膜激光损伤阈值(LIDT)影响,利用光刻技术在熔石英基底表面设置厚度为100nm不同直径大小的柱状金属Al“杂质吸收点”,然后在此基础上沉积增透膜。通过Comsol模拟仿真了解损伤过程,并利用532nm纳秒激光器进行阈值测试,对实验数据与样品损伤形貌进行分析,结果表明杂质直径为50um、100um、200um、300um、400um的薄膜损伤阈值分别为18.93J/cm²,18.62J/cm²,17.11J/cm²,15.28J/cm²,13.47J/cm²,呈非线性下降,“杂质吸收点”吸收光能产生热量,传导于增透膜层后产生的轴向热应力超过了薄膜的拉伸强度是膜层损伤的主因。     

用能量平衡法确定激光焊接熔池尺寸

本文对前人提出的计算激光焊接深熔焊过程中熔池尺寸的方法进行了检验、改进与推广。从激光焊接过程中的能量平衡出发,预报了不同焊接工况下熔池的尺寸,并与实验数据进行了比较,得到了符合得比较好的结果。     

激光诱导金纳米棒图案化光纤SERS探针

研究了激光诱导沉积制备光纤表面增强拉曼散射(SERS)探针,并对探针的SERS性能进行检测。探讨光纤探针制备过程中金纳米棒溶液的浓度对探针灵敏度的影响。结果表明,将不同浓度的金纳米棒溶液进行激光诱导,在光纤端面会形成金纳米棒团簇和分散两种纳米结构。金纳米棒溶液的浓度、激光功率、诱导时间等因素都会对诱导沉积图案产生影响。实验利用功率为5 mW的激光进行诱导,在1.5×10^-9, 1.0×10^-9和7.5×10^-10 mol·L^-1的金纳米棒溶液中,经5 min沉积,制备出不同图案的光纤SERS探针。采用晶种法合成金纳米棒,用透射电子显微镜(TEM)观察金纳米棒形貌,并根据TEM图像分析计算了合成金纳米棒的长径比约为3.8。用扫描电子显微镜(SEM)观察金纳米棒的形貌以及激光诱导沉积后的纤维修饰端形貌,7.5×10^-10 mol·L^-1的金纳米棒溶液进行激光诱导,金纳米棒在光纤端面分布较为分散,而1.5×10^-9和1.0×10^-...     

高温合金活性剂激光微焊接接头的组织性能研究（英文）

采用配方均匀设计法,配制了SiO2-MnO2-CaO-TiO2-CaF2-NaF多组元活性剂,利用微型脉冲激光器对500μm厚GH4169高温合金进行了活性剂激光焊接试验。分析并讨论了焊接接头的显微组织和力学性能。试验结果表明,与传统激光焊相比,所配制的20种活性剂均增加了焊缝熔深,并且其中F12系混合活性剂增加熔深能力最为显著,使焊缝深宽比增加了159%,证明通过使用活性剂来增加微激光焊焊缝熔深,降低高温合金板激光焊接的成本是可行的。在活性剂作用下,焊缝显微组织仍由柱状晶和等轴晶组成,接头抗拉强度达到927 MPa,为母材强度的92.7%。     

高温合金活性剂激光微焊接接头的组织性能研究

采用配方均匀设计法,配制了SiO2-MnO2-CaO-TiO2-CaF2-NaF多组元活性剂,利用微型脉冲激光器对500 m厚GH4169高温合金进行了活性剂激光焊接试验。分析并讨论了焊接接头的显微组织和力学性能。试验结果表明,与传统激光焊相比,所配制的20种活性剂均增加了焊缝熔深,并且其中F12系混合活性剂增加熔深能力最为显著,使焊缝深宽比增加了159%,证明通过使用活性剂来增加微激光焊焊缝熔深,降低高温合金板激光焊接的成本是可行的。在活性剂作用下,焊缝显微组织仍由柱状晶和等轴晶组成,接头抗拉强度达到927 MPa,为母材强度的92.7%。     

�۱����CLF-1 ����316L ��TIG ���ӽ�ͷ��֯�����ܳ����о�

A preliminary study of microstructure and properties of the welded joint of low activation CLF-1 steel used for fusion reactor and 316L dissimilar metal by tungsten inert gas (TIG) welding using W19123L as filler material, has been performed. The welded joint forming is proved well and without defect. The welded joint consists of CLF-1 zone [base metal (BM), heat affected zone (HAZ), fusion zone (FZ)], inside layer (IL), weld zone (WZ), and 316L zone (BM, HAZ, FZ). Tensile strength of the joint is better than the base metal minimum value in room temperature. Both surfaces of welded joint are without crack and with deformation uniformity under the bending test. The distribution of impact value of the joint is concave-like and satisfies the designed values for the welded joint, the WZ’s value is the lowest, the HAZ’s of both WZ zones is the second, the BM’s was the best, and the 316L steel zone’s is slightly larger than the CLF-1 zone’s. The hardness values of the point under the 1.6mm top surface of welded joint have a larger fluctuation range, and is slightly higher than those of 1/2T and above down surface 1.6mm position. The hardness distribution of 1/2T and above the down surface 1.6mm position is roughly uniform, and has a downward trend from the CLF-1 zone to 316L zone. Welding properties generally has remained stable and satisfy the requirement of dissimilar steel welding performance matching.     

High-speed laser welding of plastic films

Laser welding of plastic materials has a large field of applications in the packaging industry provided that it can compete, in quality and productivity, with currently used industrial methods. Welding of white and transparent thin films of polypropylene and polyethylene of low and high density at high speeds of 20 m s⁻¹ using a CO₂ laser has been studied experimentally.‘ The weld process has been characterised by the specific energy required for each thickness, kind of plastic and the resistance of the weld seam. The influence of the dimensions of the laser beam spot on weld strength has also been analysed.     

Cutting and welding using a CO2 laser

Of all the types of lasers now available, the CO₂ laser is particularly suitable for materials working. It has a very high efficiency (15–20%) and a high out-put power (up to several kW). When the laser light is focused by means of a lens or a mirror, a c.w. power density of more than 10⁹ W cm^-2 can be attained. The laser need not be used in vacuum.

The CO₂ laser is a suitable cutting tool for numerous materials. These include metals such as titanium or steel; combustible materials such as paper, textiles and wood; and plastics. The CO₂ laser can also cut hard and brittle materials such as aluminum oxide and silicon carbide. If metals are cut in an oxidizing atmosphere, the cutting speed may be increased. The cutting width, however, is determined by the size of the laser spot. Another important field of application is the growth of single crystals.

Experiments are reported in which the CO₂ laser was used for welding steel, titanium, plastics, quartz, and glass. The advantages of the laser for this application are discussed. A comparative study of laser and electron beam techniques is included.     

Improvement of laser keyhole formation with the assistance of arc plasma in the hybrid welding process of magnesium alloy

In the previous work, low-power laser/arc hybrid welding technique is used to weld magnesium alloy and high-quality weld joints are obtained. In order to make clear the interactions between low-power laser pulse and arc plasma, the effect of arc plasma on laser pulse is studied in this article. The result shows that the penetration of low-power laser welding with the assistance of TIG arc is more than two times deeper than that of laser welding alone and laser welding transforms from thermal-conduction mode to keyhole mode. The plasma behaviors and spectra during the welding process are studied, and the transition mechanism of laser-welding mode is analyzed in detail. It is also found that with the assistance of arc plasma, the threshold value of average power density to form keyhole welding for YAG laser is only 3.3×10⁴ W/cm², and the average peak power density is 2.6×10⁵ W/cm² in the present experiment. Moreover, the distribution of energy density during laser pulse is modulated to improve the formation and stability of laser keyholes.     

Optimization of laser welding of DP/TRIP steel sheets using statistical approach

Generally, the quality of a weld joint is directly influenced by the welding input parameter settings. Selection of proper process parameters is important to obtain the desired weld bead profile and quality. In this research work, numerical and graphical optimization techniques of the CO₂ laser beam welding of dual phase (DP600)/transformation induced plasticity (TRIP700) steel sheets were carried out using response surface methodology (RSM) based on Box–Behnken design. The procedure was established to improve the weld quality, increase the productivity and minimize the total operation cost by considering the welding parameters range of laser power (2–2.2 kW), welding speed (40–50 mm/s) and focus position (?1 to 0 mm). It was found that, RSM can be considered as a powerful tool in experimental welding optimization, even when the experimenter does not have a model for the process. Strong, efficient and low cost weld joints could be achieved using the optimum welding conditions.     

Process Window for Nd:YAG Laser Welding of Super Duplex Stainless Steel

Super duplex stainless steel (SDSS), an advanced duplex stainless steel with higher alloying concentration, is employed widely in acidic atmospheres. In this study, we make an attempt to develop a process window for the pulsed mode Nd:YAG laser welding of SDSS, as reference maps, to identify the range of process parameters viz., laser power, welding speed, defocusing distance, and pulse frequency for obtaining a defect free full penetration welds. The eminence of the welds, based on the macrostructure, microstructure, and tensile strength, is reported. We obtain a complete penetration weld devoid of undercut, crating at the top and minimum heat affected zone (HAZ) with a overlapping factor of 80–90% and heat input at 100–200 J/mm. The experimental settings prevailing inside the preferred region of the process window exhibit a higher tensile strength as well.     

Analysis of a fibre laser welding case study, utilising a matrix flow chart

For fibre laser welding of an eccentric corner joint, the quality of the resulting weld cross section was studied with respect to the dependence on process parameters like lateral laser beam alignment, beam inclination, focal plane position or welding speed. The complex load situation of the support beamer was simplified to bending of one corner. Due to fatigue load, the weld properties causing the peak stress are essential, in particular the top and root shape of the weld cross section. For the parameters varied, the resulting shapes were categorized into different top and root classes, determined by certain key dimensions, considering also welding defects like undercuts. The shapes are boundary conditions for Finite Element Analysis of the joint under load for quantitative comparative analysis of the maximum stress. As two high strength steel grades were joined, the hardness transition across the weld was of interest, too. High speed imaging of the weld pool surface shape provided additional information on the relation between the parameter input and quality output. The different trends identified were discussed and guidelines were derived. As the systematic documentation of results is unsatisfactory in welding, a new method was developed and applied for the first time, called the Matrix Flow Chart. It enables an illustrative view on the resulting welding trends in a combined manner and is extendable by other researchers.     

Research on laser welding of high-strength galvanized automobile steel sheets

The paper presented some useful results of deep-penetration laser welding of high-strength galvanized steel sheets, which had been carried out by a self-made CO₂ laser unit with maximum power output of 1.5 kW. The workpieces of high-strength galvanized automobile steels with thickness of 1.5 mm were butt-welded with argon as the shielding gas. The effects of such factors as laser power, welding speed, focal position, shielding gas and zinc vaporization on the quality of welds are investigated. With the processing parameters optimized and the proper shielding gas used in both coaxial and side-blow direction, most of the defects, such as pores, cracks and softening in HAZ, can be avoided in laser welding joints. The microstructure, the hardness distribution and the elemental distribution in the welding joints can be changed due to laser heating and recrystallization. In order to determine the mechanical properties of the welding joints, the static tensile strength was tested. Experimental results indicated that both the strength and microhardness of welding joints were higher than those of the base metal. Consequently, the welding quality is reliable for manufacturing of automobile bodies.     

Analysis of droplet transfer mode and forming process of weld bead in CO2 laser–MAG hybrid welding process

In this paper, CO₂ laser–metal active gas (MAG) hybrid welding technique is used to weld high strength steel and the optimized process parameters are obtained. Using LD Pumped laser with an emission wavelength of 532 nm to overcome the strong interference from the welding arc, a computer-based system is developed to collect and visualize the waveforms of the electrical welding parameters and metal transfer processes in laser–MAG. The welding electric signals of hybrid welding processes are quantitatively described and analyzed using the ANALYSATOR HANNOVER. The effect of distance between laser and arc (D_LA) on weld bead geometry, forming process of weld shape, electric signals, arc characteristic and droplet transfer behavior is investigated. It is found that arc characteristic, droplet transfer mode and final weld bead geometry are strongly affected by the distance between laser and arc. The weld bead geometry is changed from “cocktail cup” to “cone-shaped” with the increasing D_LA. The droplet transfer mode is changed from globular transfer to projected transfer with the increasing D_LA. Projected transfer mode is an advantage for the stability of hybrid welding processes.