首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到19条相似文献,搜索用时 187 毫秒
1.
目的 采用数值模拟方法代替传统测量方法,以准确模拟不锈钢薄壁管件焊接接头残余应力分布规律及预热温度对焊接残余应力的影响规律。方法 采用TIG焊接方法对304不锈钢进行圆管纵缝焊接试验,以最优焊接工艺参数为基础,基于ABAQUS有限元仿真软件,采用热力完全耦合模型,在DFLUX子程序中运用Fortran语言对模型进行汇编以完成ABAQUS的二次开发,模拟薄壁管件纵缝焊接热力耦合过程,并在模拟结果上添加预热温度为150 ℃的预热工艺。结果 304不锈钢薄壁管件焊接过程中会产生较大的残余应力,局部区域接近管材的屈服应力。纵向残余应力趋于焊缝中心方向由压应力转化为拉应力,焊缝中心横向应力承受压应力,并且随着向焊缝两侧移动,横向残余应力值逐渐趋近于0。焊缝厚度方向上的径向应力值变化幅度较小。预热可以有效降低不同方向上的焊接残余应力,其中对纵向残余应力的改善最为明显。结论 数值模拟方法能够准确计算出不锈钢薄壁管件焊接接头残余应力分布,预热处理能够有效降低接头残余应力。  相似文献   

2.
本文采用数值模拟的方法,对船体结构的某一环形拘束焊缝进行焊接残余应力的模拟计算.同时采用压痕式应力测试仪,对实际船体结构进行测试,并与模拟结果相对比验证.结果表明,模拟结果与实测结果测得的焊接残余应力分布规律基本一致,环形拘束焊缝纵向残余应力大于横向残余应力,最大焊接残余应力位于靠近热影响区的直线段焊缝近表面处.  相似文献   

3.
赵秋  吴冲 《工程力学》2012,29(10):170-176
基于焊接残余应力数值模拟方法, 分析了U 肋加劲板各组成板件的板宽、板厚对焊接残余应力分布的影响, 揭示了U 肋与母板残余应力合力的分配规律, 提出了针对不同构造尺寸的U 肋加劲板焊接残余应力分布简化计算方法。研究结果表明:各组成板件的板宽变化对焊接残余拉应力的分布影响较小, 但对焊接残余压应力的大小影响较大;U 肋与母板的板厚比对U 肋与母板残余应力的分配比例影响较大。U 肋加劲板受压承载力计算时, 焊接残余应力分布可以采用简化方法计算, 其结果与根据数值模拟得到的焊接残余应力分布计算的结果基本一致。  相似文献   

4.
为研究铝合金中厚板-节点套接头在多层多道焊后的残余应力和变形分布,本文基于ABAQUS软件建立了该接头三维有限元模型,采用双椭球热源、生死单元法以及顺序耦合法,对6061-T6铝合金中厚板-节点套多层多道焊进行数值模拟,并分析了接头的温度场,以及在夹具约束下的焊接残余应力及变形的分布情况。研究结果表明:数值模拟与实际接头的熔池形状吻合度较高;摆动焊接过程中温度曲线呈多峰结构;焊件的升温速率明显大于冷却速率,且冷却速率随时间逐渐减小;焊接残余应力主要集中在焊缝及夹具区域,且小于6061-T6铝合金在室温下的屈服强度;接头的最大横向残余应力为129.9 MPa,中厚板上的横向残余应力大于节点套上的横向残余应力;接头的最大纵向残余应力为132.9 MPa,沿焊接方向,焊缝处的纵向残余应力呈山峰状分布;该接头在Y轴方向上的变形最大,为1.494 mm,该接头的最终变形结果为上凸变形。  相似文献   

5.
采用组合热源模型对Al-Li合金电子束焊接温度场分布进行数值模拟分析,通过热-力耦合,模拟计算得到接头区域的残余应力分布.结果表明,Al-Li合金电子束焊接温度场沿焊接方向呈椭圆形分布,电子束热源中心的温度最高,其附近区域的等温线分布密集,随着与热源中心的距离增大,等温线分布逐渐稀疏,焊缝区存在较大的温度梯度,较好地模拟出了电子束焊缝的钉形分布特征.接头的残余应力分布模拟结果显示,残余应力主要集中于焊缝区,由于修饰焊的热作用,焊缝上部具有相对较大的应力值.利用模拟计算得到的结果进行焊接工艺及参数优化,焊接工艺试验表明,试验焊缝形貌与模拟熔池形貌相吻合,进一步验证了模拟计算结果的可靠性.  相似文献   

6.
为了研究圆钢管加工方法诱导的纵向残余应力分布规律,该文采用盲孔法对截面规格为 φ325×8的5组15个不同强度、不同加工方法的圆钢管试件进行了测量。基于测量数据,得到了试件截面残余应力分布和拉、压残余应力的数值大小,研究了埋弧焊、高频焊和热轧三种不同加工方法对残余应力分布的影响。试验结果表明,埋弧焊对圆钢管截面纵向残余应力的影响强于高频焊,高强度焊接圆钢管的残余应力分布比较均匀,且焊缝区最大残余拉应力分布在焊缝两侧各40 mm区域内;普通强度钢管截面的最大纵向残余压应力为0.35σy,而Q690高强钢焊接圆钢管截面的最大纵向残余压应力为0.21σy,同中点截面的纵向残余应力峰值相比,起焊点和落焊点截面处的纵向残余应力峰值偏小。不同于焊接圆钢管,热轧无缝圆钢管同一截面内外表面的最大纵向残余应力数值大小相同,符号相反,其最大值为0.15σy。  相似文献   

7.
使用压痕法对两副对接试板进行了表面焊接残余应力测试,并通过焊接有限元仿真获得了对接试板焊接残余应力分布规律,对比分析了表面残余应力实测和数值模拟结果。分析结果表明,焊接残余应力数值仿真结果和压痕法实测结果趋势一致,数值相差不大,残余拉应力峰值实测为599 MPa,仿真结果为597 MPa,表明数值模拟方法可预测焊接残余应力;焊缝及热影响区最大纵向残余应力属于拉应力,而最大横向残余应力为压应力,横向残余应力峰值低于纵向残余应力峰值;等效应力(Mises应力)峰值792 MPa,高于试板材料在常温下的初始屈服强度,表明该材料具有明显的加工硬化现象。  相似文献   

8.
U肋加劲板焊接残余应力数值模拟分析   总被引:5,自引:0,他引:5  
赵秋  吴冲 《工程力学》2012,29(8):262-268
通过数值模拟和实验方法对U 肋加劲板焊接残余应力进行了估算和分析,建立了三维热弹塑性有限元模型,采用生死单元法模拟焊缝填充和焊接热输入过程,实现了整个焊接过程中的动态应力和变形变化,得到了U肋加劲板的焊接温度场和应力场,分析了U 肋加劲板的焊接残余应力分布,并与残余应力测试试验结果比较.结果显示:U 肋加劲板近焊缝区残余拉应力达到材料屈服强度,母板远离焊缝区残余压应力平均值约为材料屈服强度的0.2 倍,其分布趋势与实验测试得到的残余应力分布比较接近,证明了所采用的焊接数值模拟方法的正确性.  相似文献   

9.
目的 研究激光+GMAW复合焊中不同激光功率参数对铝合金T型接头残余应力的影响,从而提高焊接性能。方法 分别考虑了热弹塑性理论、传热学以及T型接头几何特性,建立了铝合金T型接头激光+电弧复合焊残余应力的数值分析模型。采用双椭球体热源模型表征电弧热输入与熔滴晗,采用锥体热源模型对激光深熔焊进行描述。基于所建立的T型接头模型,使用ANSYS有限元软件对12 mm厚铝合金激光+ GMAW焊T型接头残余应力进行模拟计算,并研究其分布特征;使用X射线衍射法对T型接头处的残余应力进行测量从而对所建模型的准确性进行验证。同时,对比了不同激光功率下铝合金T型接头对残余应力的影响规律。结果 当激光功率分别为2、3、4、5 kW时,铝合金T型接头路径L3上的纵向残余应力最大值分别为270、263、258、251 MPa,米塞斯-等效应力最大值分别为265、261、257、250 MPa。结论 后焊的焊缝A对焊缝B有明显的热处理作用,使应力明显降低;在T型接头焊缝及近缝区,横向残余应力和厚度方向残余应力峰值均比纵向残余应力峰值小,且随着激光功率的增大,焊缝及近缝区拉应力峰值不断减小。  相似文献   

10.
考虑相变的铝合金管焊接残余应力数值模拟   总被引:1,自引:0,他引:1  
以铝合金薄壁管的对接接头为研究对象,根据实际情况建立了其热-冶金-力学耦合的三维有限元模型,运用SY-SWELD软件在考虑相变情况下对其焊接过程温度场与轴向和环向残余应力分布进行数值计算与分析,与实验结果进行对比验证了该模型的准确性。此外,还分析了铝合金管半径变化对残余应力分布的影响规律。结果表明:相变对轴向最大拉应力与环向最大拉应力和压应力都有明显的影响,且考虑相变能更准确地模拟轴向和环向残余应力;在考虑相变情况下,焊接残余应力随半径的增大而增加;并且在不同的半径条件下,距焊缝中心不同距离上的应力分布有着一致的变化趋势。  相似文献   

11.
目的 研究平板对接电子束焊接过程中Ti2AlNb合金接头的残余应力及变形规律。方法 采用高斯圆柱体和高斯面组合热源模型模拟了6.6 mm厚的Ti2AlNb合金平板对接电子束焊过程,对比研究了高焊速高束流和低焊速低束流2种工艺参数下焊接接头的残余应力和变形分布规律,并用小孔法测量了焊缝中心及距焊缝中心10 mm位置的残余应力值。结果 在高焊速高束流参数下,获得了熔池体积小、熔池宽度窄(为3.62 mm)、深宽比高的焊缝;在该参数下焊缝横截面上的高应力集中区(应力在900 MPa以上)尺寸较小,其宽度仅为低焊速低束流参数下的89%;同时,在高焊速高束流参数下,焊缝法向变形最大值为0.79 mm,低于低焊速低束流参数下的0.82 mm;模拟计算所得残余应力与实测值的误差在5.64%以内。结论 高束流高焊速工艺具有热输入小、热量集中、加工效率高的特点,有助于获得高应力集中区域小、深宽比高、变形小的焊缝,比低束流低焊速工艺更具优势。  相似文献   

12.
为研究焊接工艺参数对Q345钢平板焊接残余应力的影响,对采用药芯焊丝半自动焊接后的8 mm厚平板焊缝结构进行仿真模拟,在经验数值范围内设置不同的焊接工艺参数值,分析平板在横向和厚度方向的焊接残余应力分布情况。研究结果表明:横向的最大焊接残余应力分布在热影响区,且随着焊接速度的增大和焊接层间温度的降低而降低;沿厚度方向的最大焊接残余应力为115.92 MPa,位于平板中间层,随着焊接速度的增大而先减小后增大;平板焊接在横向的残余应力远大于厚度方向的应力。根据焊接残余应力的变化情况,运用二元回归分析法对横向和厚度方向的最大焊接残余应力进行函数拟合与检验,并开展多因素拟合模型的分析,得到焊接速度和焊接层间温度对焊接残余应力的综合影响规律。通过研究残余应力的变化趋势可选定焊接残余应力最小时的工艺参数范围,实现焊接工艺参数优化。  相似文献   

13.
目的 揭示焊接参数对TC4薄板焊接过程中温度场、位移场及应力场的影响规律。方法 基于有限元(FEM)模拟方法,运用Fortran语言对焊接热源及焊接参数进行定义,以模拟不同焊接参数下TC4薄板的TIG对接焊过程。结果 在稳弧阶段,温度场为一组以焊接方向为长轴的椭圆,且存在温度梯度,随着焊接速度的增大,温度场峰值、温度场温度梯度、熔池宽度和熔池体积逐渐减小,而焊接效率和焊接电流对温度场的影响与焊接速度刚好相反;随着焊接速度的增大,薄板最大变形量逐渐减小,焊接角变形及挠度变形逐渐得到改善,而焊接效率和焊接电流对位移场的影响与焊接速度刚好相反。在稳弧阶段,焊缝位置的残余应力为拉应力,两侧为压应力,随着焊接速度和焊接电流的增大,纵向残余拉应力逐渐增大,焊缝处高应力集中区的宽度逐渐减小,而焊接效率对应力场的影响与焊接速度刚好相反。在高焊接速度、中等焊接效率、低焊接电流参数条件下,可获得熔池体积小及熔池宽度窄的焊缝,有利于减小焊后残余应力与变形。结论 上述研究结果可为TC4薄板的焊接过程提供一定的理论指导。  相似文献   

14.
卓子超  张庆亚  王江超 《工程力学》2020,37(11):238-247
船舶钢结构皆采用焊接方法建造而成,在实际工况及环境载荷作用下,焊接接头的力学性能及其断裂强度,直接影响船舶整体结构的强度和寿命。该文针对常用的船板钢材料(Q345和Q690),首先对母材进行单向拉伸试验,获得其各自的应力-应变曲线,进而评估其断裂性能;基于Gurson-Tvergaard-Needleman (GTN)损伤模型,通过程序代码的调试和一系列的数值模拟分析,提出了母材本构关系的表达函数及最优GTN模型参数,且与实测的应力-应变曲线高度吻合。同时,针对满足焊接规范要求的船板钢对接焊接头,进行了单向拉伸试验获得其应力-应变曲线;考虑焊缝微观缺陷以及焊接残余应力的影响,提出修正GTN损伤模型中的初始空穴体积分数f0和材料的幂函数塑性强化参数,预测焊接接头的断裂强度,且与试验测量数据吻合一致。  相似文献   

15.
In the present test the fatigue crack growth rate in the parent plate, weld and cross-bond regions was measured and the results were correlated with the stress intensity range ΔK and the effective stress intensity range ΔKeff. It is indicated that the welding residual stresses strongly affect the crack growth rate. For the weld metal and cross-bond compact tension specimens in which crack growth is along the weld line the fatigue crack growth rate increases as the crack grows. However, for the T compact tension specimen in which crack growth is perpendicular to the weld line at a constant value of applied ΔK the crack growth rate initially decreases as the crack grows. Particularly, at a low constant value of applied ΔK the crack growth rate obviously decreases and the crack fails to grow after short crack growth. When the crack grows to intersect the welded zone, the fatigue crack growth rate gradually increases as the crack grows further. It is clear that the effect of welding residual stresses on the crack growth rate is related to the position of the crack and its orientation with respect to the weld line. Finally, the models of welding residual stress redistribution in the compact tension specimens with the growing crack and its influence on the fatigue crack closure are discussed. It appears that for a butt-welded joint one of the crack closure mechanisms may be considered by the bend or rotation deformation of crack faces due to the welding residual stress redistribution as the fatigue crack grows in the welded joint.  相似文献   

16.
This paper investigates distortions and residual stresses induced in butt joint of thin plates using Metal Inert Gas welding. A moving distributed heat source model based on Goldak’s double-ellipsoid heat flux distribution is implemented in Finite Element (FE) simulation of the welding process. Thermo-elastic–plastic FE methods are applied to modelling thermal and mechanical behaviour of the welded plate during the welding process. Prediction of temperature variations, fusion zone and heat affected zone as well as longitudinal and transverse shrinkage, angular distortion, and residual stress is obtained. FE analysis results of welding distortions are compared with existing experimental and empirical predictions. The welding speed and plate thickness are shown to have considerable effects on welding distortions and residual stresses.  相似文献   

17.
Surface residual stress evaluation for double-electrode welding was studied. The stresses were monitored after each operational step: positioning, implementing of constraints, welding and constraints removal. The measurements were performed at the deposited metal, heat affected zone, base metal close to the weld joint and along the plate using the X-ray diffraction method. It was observed differences in the stress evaluations for double-electrode welding which resulted in lower bending distortions and higher values of surface residual stresses, compared with single-electrode welding. This behavior is associated with the stress distribution just after the welding processes in both heat affected zone and base metal close to the fillet for double-electrode welding. The main results from the laboratorial tests indicated lower values of the bending distortions for double-electrode welding compared with the single-electrode. In relation to the residual stress, the double-electrode welding generated, in general, higher stress values in both longitudinal and transversal directions.  相似文献   

18.
The influence of the friction-stir welding process on microstructure and mechanical properties of API 5L X80 skelp was investigated. Friction-stir welds were produced using welding parameters optimized to promote weld toughness. The solid-state welding process produced microstructures that significantly varied from those observed in the base metal, namely the redistribution and resizing of Martensite–Austenite constituent in the heat-affected zone and stir zone regions of the welds. Mechanical properties of the welds and base metal were evaluated with uniaxial tension testing and microhardness testing revealing overmatching welds and a hard zone within the weld stir zone. Residual stresses were determined in several directions with respect to the joint revealing that stress in the longitudinal direction is highest, yet well below material yield strength. Fatigue-crack propagation behavior was characterized in the different weld regions and base metal by testing with the compact tension specimen configuration showing that welds have impeded fatigue-crack growth compared to the base metal mostly due to welding-induced residual stress fields interacting with the crack.  相似文献   

19.
Residual stresses in a structure are generated as a result of the various fabrication and welding processes used to make the component. Being able to quantify these residual stresses is a key step in determining the continuing integrity of a structure in service. In this work, the residual stresses around a high strength, quenched and tempered steel T-butt web to curved plate weld have been measured using neutron strain scanning. The results show that the residual stresses near the weld were dominated by the welding residual stresses, while the stresses further from the weld were dominated by the bending residual stresses. The results suggest that the combination of welding-induced residual stress and significant pre-welding residual stress, as in the case of a thick bent section of plate can significantly alter the residual stress profile from that in a flat plate.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号