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1.
Abstract

An autogenous gas tungsten arc closure weld was developed for the US Department of Energy's primary container for the storage of plutonium bearing materials. The occurrence of porosity at the tie-in point of the closure weld was investigated. The primary cause of the porosity was linked to the geometry at the root of the closure weld joint. The present paper describes the mechanistic model that was developed to describe and predict the porosity.  相似文献   

2.
Abstract

A seam tracking method is presented based on the estimation of weld position during the gas tungsten arc welding process. Kalman filtering of the weld pool images from a visual sensor is applied to compute recursively the solution to the weld position equations which are established based on an estimation of the centroid position of the weld pool images. This centroid, the position of which corresponds with the weld position, is extracted as the measurement eigenvector. The evolution of the weld position data from the weld pool images can be described through an appropriate process model, so that the weld position can be detected by applying a Kalman filter. This allows adjustment of the welding torch position in real time, which may significantly reduce processing time and promote seam tracking accuracy. Simulations and actual welding experiments have demonstrated the effectiveness of the proposed algorithm in the presence of weld pool image noise and have demonstrated the robustness of weld position detection for seam tracking.  相似文献   

3.
Abstract

Manufacturers use different, proprietary pulse current programming algorithms in their synergic 'one knob control' pulsed gas metal arc welding (GMAW-P) power supplies. Since the different pulse waveforms produced by these supplies can produce somewhat different welding characteristics, inconsistent results can be obtained when transferring welding procedures between different GMAW-P power supplies. A primary objective of this work was to characterise the differences in welding heat input and weld bead shape that could be produced by the pulsed current waveforms from four different commercial supplies. To eliminate the affects of subtle differences in electrical characteristics and to ensure that the exact shape of all waveforms was fully known, the comparison was also done by simulating the waveforms generated by three of the four power supplies on the fourth supply, which was equipped with waveform programming capability. Then, the four waveforms were used to create 'bead on plate' welds over a range of wire feed speed settings, and corresponding heat inputs were calculated from current and voltage samples recorded by a computer data acquisition system during welding. Welds were also done at the same wire feed speed setting using a constant voltage supply. All welds were then cross-sectioned for penetration and dilution measurements. In general, all of the waveforms produced good metal transfer and weld quality. However, the heat input and beads shapes varied noticeably. The heat inputs for the four pulse waveforms and constant voltage welds differed by as much as 150 J mm?1 (17% of the maximum heat input) at the highest wire feed speed of 212 mm s?1. The weld penetration differed by 1 mm (22% of the maximum penetration) at a wire feed speed of 169 mm s?1 and the dilution differed a maximum value of 6.5% dilution (22% of the maximum dilution) at a wire feed speed of 169 mm s?1 .  相似文献   

4.
Abstract

The weld expulsion is prone to occur and severely affects the nugget quality when the initial gap between dual phase (DP) steel sheets exist in resistance spot welding (RSW). To investigate the effect of initial gap on weld expulsion, a finite element model was developed to analyse the weld nugget formation process with different initial gaps for DP steels. An estimation method of expulsion occurrence based on the ratio of the nugget radius Rn and the contact radius Rc between sheets was proposed to get the critical initial gap without expulsion. The simulation and experimental results showed that the weld expulsion would not happen until the gap spacing reaches the critical value. The critical initial gap of DP steel is much smaller than that of low carbon steel. For both DP steel and low carbon steel, the critical initial gap would increase with the thickening of the steel sheet.  相似文献   

5.
采用Cu68.5Ni15.7Sn9.3P6.5(质量分数,%)四元合金非晶薄带钎料真空钎焊紫铜,通过金相分析、电子探针以及X射线衍射物相分析方法对钎缝组织致密性进行了研究.结果表明,影响钎焊接头致密性的主要因素是焊缝中的气孔,钎焊中气孔的形成主要是由于P元素的汽化产生.对比非晶钎料和晶态钎料钎焊接头对气孔的敏感性可以看出,非晶钎料钎焊接头对气孔更为敏感,从空位和原子振动理论分析得出非晶钎料中气孔敏感主要是由非晶钎料元素的活度较大所致.  相似文献   

6.
Abstract

Although numerical calculations of heat transfer and fluid flow can provide detailed insights into welding processes and welded materials, these calculations are complex and unsuitable in situations where rapid calculations are needed. A recourse is to train and validate a neural network, using results from a well tested heat and fluid flow model to significantly expedite calculations and ensure that the computed results conform to the basic laws of conservation of mass, momentum and energy. Seven feedforward neural networks were developed for gas metal arc (GMA) fillet welding, one each for predicting penetration, leg length, throat, weld pool length, cooling time between 800°C and 500°C, maximum velocity and peak temperature in the weld pool. Each model considered 22 inputs that included all the welding variables, such as current, voltage, welding speed, wire radius, wire feed rate, arc efficiency, arc radius, power distribution, and material properties such as thermal conductivity, specific heat and temperature coefficient of surface tension. The weights in the neural network models were calculated using the conjugate gradient (CG) method and by a hybrid optimisation scheme involving the CG method and a genetic algorithm (GA). The neural network produced by the hybrid optimisation model produced better results than the networks based on the CG method with various sets of randomised initial weights. The CG method alone was unable to find the best optimal weights for achieving low errors. The hybrid optimisation scheme helped in finding optimal weights through a global search, as evidenced by good agreement between all the outputs from the neural networks and the corresponding results from the heat and fluid flow model.  相似文献   

7.
An amorphous Ti-37.5Zr-15Cu-15Ni (wt.%) ribbon fabricated by vacuum arc remelting and rapid solidification was used as filler metal to vacuum braze TiAl alloy (Ti-45Al-2Mn-2Nb-1B (at.%)). The effects of brazing temperature and time on the microstructure and strength of the joints were investigated in details. The typical brazed joint major consisted of three zones and the brazed joints mainly consisted of α2-Ti3Al phase, α-Ti phase and (Ti, Zr)2(Cu, Ni) phase. When the brazing temperature varied from 910 °C to 1010 °C for 30 min, the tensile strength of the joint first increased and then decreased. With increasing the brazing time, the tensile strength of the joint increased. The maximum room temperature tensile strength was 468 MPa when the specimen was brazed at 930 °C for 60 min. All the fracture surfaces assumed typical brittle cleavage fracture characteristic. The fracture path varied with the brazing parameter and cracks preferred to initiate at (Ti, Zr)2(Cu, Ni) phase and propagation path were mainly determined by the content and distribution of α-Ti phase and (Ti, Zr)2(Cu, Ni) phase.  相似文献   

8.
针对Si3N4陶瓷的高温活性钎焊要求,设计了高温Ti-Zr-Ni-Cu非晶钎料成分,并采用单辊急冷法成功制备了Ti-Zr-Ni-Cu非晶钎料.对比分析了相同成分的Ti-Zr-Ni-Cu非晶和晶态钎料在Si3N4陶瓷表面的润湿情况.结果表明:在低真空条件下,晶态钎料能够润湿Si3N4陶瓷,非晶钎料却因完全氧化而失效.在5×10-3Pa高真空条件下,非晶钎料的润湿性优于晶态钎料,在研究的Ti-Zr-Ni-Cu非晶钎料中,Ti40Zr25Ni15Cu20非晶钎料对Si3N4陶瓷的润湿性最佳.  相似文献   

9.
针对Ag-Cu-Ge系钎料难以加工成薄片的难题,利用电磁粉末压制结合液相烧结的成形工艺制备了钎料薄片,探究了不同压制电压及烧结温度对钎料薄片致密度和组织结构的影响,选用优化工艺下的钎料薄片对铜板进行焊接实验。实验结果表明:压坯致密度随着压制电压的提高而显著提升,当压制电压为2800 V时,压坯致密度达到最大值88.62%,而电压升高到3000 V时,锗粉颗粒内部开始产生裂纹甚至破裂;250℃烧结温度下烧结体出现了弹性后效现象,当烧结温度升高到400℃时,烧结体致密度增长率达到最大值2.63%,若温度继续升高,烧结体晶粒则出现粗化现象;最终当焊接温度为600℃时,焊缝组织均匀,与母材形成了较好的冶金结合,表现出良好的焊接性能,说明了该成形工艺用于制备钎料薄片的可行性。  相似文献   

10.
分别采用AgCu共晶钎料和AgCu共晶钎料中添加30%(质量分数)Zn的AgCuZn钎料在TiC金属陶瓷表面进行润湿试验.结果表明,Zn元素的添加显著改善了钎料在TiC金属陶瓷表面的润湿性;AgCu钎料润湿TiC金属陶瓷时,从近钎料外表面到钎料/陶瓷界面,组织依次为Ag(s.s)+Cu(s.s)/(Cu,Ni)+Ag(s.s)/TiC金属陶瓷+Ag(s.s)+Cu(s.s)/TiC金属陶瓷;而采用AgCuZn钎料润湿TiC金属陶瓷后,从近钎料外表面到钎料/陶瓷界面,组织依次为Ag(s.s)+Cu(s.s)+(Cu,Ni)/Ag(s.s)+Cu(s.s)/(Cu,Ni)/TiC金属陶瓷+Ag(s.s)+Cu(s.s)/TiC金属陶瓷.Zn元素在真空中挥发促进了界面处Ni原子的溶解和扩散,使钎料在陶瓷表面的润湿角由120.6°减小到33.9°.  相似文献   

11.
晶化温度对非晶态Cr-Fe-C合金镀层的影响   总被引:1,自引:0,他引:1  
采用三价铬电镀液,在4Cr10Si2Mo钢工件表面电沉积非晶态Cr-Fe-C合金镀层.通过改变络合剂的含量、电流密度和电镀时间,在阴极上沉积了不同厚度的非晶态Cr-Fe-C层.用扫描电子显微镜和光学显微镜、X射线衍射仪、能谱仪测定、显微硬度计研究了从三价铬镀液中电沉积Cr-Fe-C镀层的工艺以及镀层的形貌、结构与性能.结果表明,利用该工艺获得了厚度为30 μm、27 wt%Fe的非晶态Cr-Fe-C合金镀层.该镀层耐蚀性较好,经600℃×1 h晶化处理后硬度最高可达1 800 HV0.05.  相似文献   

12.
本文采用聚氨酯抛光盘和绒布抛光垫对铜衬底进行超精密抛光工艺研究,对铜衬底的表面粗糙度、材料去除率以及铜衬底表面组织结构变化过程进行了研究,并讨论了铜衬底在超精密抛光时,不同抛光条件对其表面粗糙度和材料去除率的影响,以及抛光压力对铜衬底的表面形成过程的影响。结果表明,采用聚氨酯抛光盘和绒布抛光垫可以消除划痕,抛光后的铜衬底表面粗糙度可达Ra6 nm。  相似文献   

13.
采用高速摄影对超声波辅助钎焊镁合金过程熔态钎料的填缝行为进行了实时观察,并研究了不等间隙中钎料的填缝行为及接头性能.结果表明,超声波在钎焊固/液界面传播对钎料填缝行为有显著的影响.钎料在平行于超声波能量传播方向上填缝,填缝长度和超声时间的动力学曲线呈直线型.超声时间相同时,预留间隙越大,钎料的填缝速度越低.在大间隙端加钎料,随超声时间增加,填缝长度减小,钎缝致密性较好;小间隙端加钎料,随超声时间增加,填缝长度先增大后减小,整个钎缝均存在缺陷.认为钎料在不等间隙的流动行为受超声诱导填缝和毛细填缝共同作用的影响.  相似文献   

14.
通过热物理模拟试验,系统地研究了主要热力参数(变形温度、变形速率、变形程度)与流动应力间的数值关系,采用正交设计原理,科学地分析并回归出GH44合金的本构方程,定性地探讨热力参数对GH44合金成形性能的影响规律,为GH44合金的热变形数值模拟和热力参数的合理制定与控制提供了依据。  相似文献   

15.
为获得最佳设计方案,设计两种实验方案,通过改变工艺参数对铜钛合金复合材料进行激光金属沉积。从显微组织演变、硬度和力学性能三方面对所沉积的复合材料进行表征。结果表明:复合材料的显微组织由一次、二次和三次枝晶臂,针状组织和α+β共晶组织组成。两种实验方案结果表明,在激光功率为1200 W、扫描速率为1.2 m/min的条件下得到的样品E具有最高的硬度,其值为HV (190±42),但由于其脆性,因此出现一些横间裂纹;而在激光功率为1200 W、扫描速率为0.3 m/min条件下得到的样品B无裂纹产生,且其显微组织良好并含有较多的枝晶。得到的铜复合材料的应变硬化系数为3.35。  相似文献   

16.
Alumina dispersion strengthened copper(ADSC) alloy was produced by internal oxidation. The hardness, ultimate tensile strength and electrical conductivity measurements and microstructure observation on the produced 0.12?SC (0.24% Al2O3, mass fraction) and 0.25% ADSC (0.50% Al2O3) subjected to different annealing treatments were conducted. The results show that the microstructure of the produced ADSC is characterized by an uniform distribution of nano-Al2O3 particles in Cu-matrix; the particles range in size from 20 to 50 nm with an interparticle spacing of 30 - 100 nm. The produced 0.12% ADSC can maintain more than 87% hardness retention after 900℃, 1 h annealing treatment; the recrystallization can be largely retarded and is not fully completed even after annealing at 1 000℃ for 1 h, followed by cold deformation of 84% ; local grain growth can be observed after 1 050℃ ,1 h annealing treatment. The results also show that increasing either the alumina content or cold deformation degree increases the hardness of the produced ADSC.  相似文献   

17.
采用超音速火焰喷涂技术在0Cr13Ni5Mo不锈钢基体上制备了铁基非晶涂层,研究了500%~800℃不同温度热处理对涂层的相组成和摩擦磨损性能的影响.从涂层的显微硬度分析、相组成分析、晶粒大小分析、以及摩擦磨损试验分析表明:随着热处理温度升高涂层的相结构及性能发生变化,在600℃时,涂层中析出大量的纳米硬质相,涂层的显微硬度和耐磨损性能也随之大幅提高;涂层的显微硬度在600℃时达到最大,耐磨性能在750℃时最好.  相似文献   

18.
The experimental investigation of different tran sition metals was carried out in the diffusion bonding joints of Cu alloys (CuAlBe) to stainless stee l (1Cr18Ni9Ti). The microstructure of the joint was analyzed with microscopic examination, SEM, EPMA and X-ray diffraction. Following conclusions have been draw n: (1) The joint strength with the Ni interlayer was higher than that with Cu in terlayer when the welding parameters were same;(2)When Ni interlayer was thinner ,Al could interact with Ni and Fe,and the intermetallic compounds,such as Fe3A letc,were formed in the interface,which decreased the strength of the joints;(3 ) When the bonding temperature was higher,because of the diffusion of Cu in Ni being faster than Ni in Cu,a Kirkendall effect was produced,which also decreased the strength of the joints.  相似文献   

19.
将铸态CuSn10P1铜合金先预退火处理,随后采用冷轧等温处理应变诱导熔化激活法(CRITSIMA)制备成半固态坯料。采用金相显微镜、配置能谱仪的扫描电子显微镜、X射线衍射仪、电子探针和布氏硬度计,研究预退火温度对半固态铜合金坯料的组织演变及力学性能的影响。结果表明:随着预退火温度升高,半固态铜合金坯料的平均晶粒尺寸增加,晶粒形状因子和液相率均降低;随着预退火温度升高,α-Cu相中固溶更多的Sn元素,减弱了Sn元素偏析,晶间脆硬相δ相含量减少,布氏硬度逐渐减小。在半固态铜合金坯料中检测到新相Cu13.7Sn的存在,这与晶间Sn元素的高度偏析有关。600 ℃预退火2 h制备的半固态铜合金坯料显微组织晶粒均匀细小,力学性能较好,其平均晶粒尺寸为68.34μm、晶粒形状因子为0.78、α-Cu基体中Sn元素固溶度为4.21wt%,布氏硬度为128 HBW。  相似文献   

20.
基于耦合外应力及交变温度场的微观相场动力学模型,以镍基合金为对象,研究了在沉淀过程中结构相的生长取向及合金元素分配。结果表明:交变温度场不能改变合金的生长取向及结构相的析出顺序。交变温度场条件下,合金Al含量较高时,L1_2相先析出;V含量较高时,DO_(22)相先析出;拉应力作用时,L1_2及DO_(22)结构相垂直于应力方向生长。[001]方向拉应力下、L1_2相先析出时,DO_(22)相在[100]取向上的生长受到促进;当在[100]方向拉应力下、DO_(22)相先析出时,L1_2相在[001]取向上的生长受到促进。随着交变高温温度的降低,L1_2相体积分数随温度的波动幅度显著降低而DO_(22)相的变化则相对较小。  相似文献   

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