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1.
TIG熔修后T形接头的焊接残余应力及消除   总被引:1,自引:0,他引:1       下载免费PDF全文
用红外热成像仪测量了P355NL1钢T形接头在焊接过程中的温度场分布,得到焊接过程的温度循环曲线,并且与有限元方法模拟的温度场结果吻合,验证模拟计算的准确性;使用盲孔法,测量了T形板焊接MAG焊后、TIG熔修后以及热处理后的残余应力;采用间接法利用温度场计算结果计算了T形接头试板焊接残余应力场,模拟结果与实际测量的残余应力趋势相符.结果表明,TIG熔修能一定程度的降低焊缝中心的残余应力,但增大了熔修区域的残余应力;而通过整体热处理能有效地消除熔修带来的大部分残余应力,但仍有部分残余应力存在.  相似文献   

2.
《塑性工程学报》2016,(3):178-182
以长轴薄壁连接杆为研究对象,采用MARC有限元软件对连接杆的焊接过程进行数值模拟,分析不同焊接热输入对温度场、残余应力及变形的影响规律。结果表明,焊接热输入由5 600J·mm-1减小到2 800J·mm-1,残余应力及变形均显著增加,纵向残余应力增加17%,横向残余应力增加33.9%,变形量增加63.5%。焊接实验结果与模拟结果吻合,验证了模拟结果的准确性,对焊接变形的预测及控制具有重要意义。  相似文献   

3.
借助有限元分析手段对板材的焊接过程进行模拟,得到焊接变形和应力分布情况。基于白光三维扫描仪和DIC两种测量手段,分别验证焊后变形趋势和变形量,同时采用盲孔法测量残余应力分布结果,计算结果与实验结果吻合较好,证明有限元模型的正确性和有效性。结果表明,白光三维扫描法对焊后整体变形趋势进行了定性分析,DIC对焊后局部变形进行了定量分析,应力模拟结果基与实际应力分布测量结果基本吻合,对现场结构件变形预测和残余应力分布趋势分析有重要指导意义。  相似文献   

4.
王浩  李莉 《电焊机》2016,(10):90-95
为研究焊接顺序对T型接头角焊缝残余变形的影响,对平对接接头的焊接过程进行数值模拟和焊接实验,验证焊接模拟的合理性;建立T型接头双面角焊缝的有限元模型,采用生死单元技术和热结构耦合的方法对T型接头焊接过程中的温度场和应力场进行数值模拟,分析4种焊接顺序对其残余变形的影响。结果表明,模拟结果与残余应力测试结果吻合良好,说明焊接模拟过程合理有效。T型接头在焊后发生了挠曲变形,焊接顺序2的残余变形最小,变形量为0.61 mm,采用从两侧向中间的焊接顺序能够减小T型接头的残余变形。  相似文献   

5.
采用大型通用有限元软件对TRT焊接机壳进行焊接过程的模拟。利用有限元软件中的单元生死技术和热-结构耦合技术,成功的预测了TRT机壳焊后残余应力及变形,并通过焊后残余应力测试试验验证对比。结果表明,有限元模拟机壳在焊接过程中,焊缝附近残余应力较大,局部达到其屈服强度;远离焊缝处的壳体上应力较小,均处于弹性变形。进行"盲孔法"测量残余应力,试验测量的残余应力跟模拟所得残余应力分布趋势相同,峰值应力出现的点基本重合。由于机壳实际焊接中施加的约束较多,应力得不到释放,导致试验数值略高于模拟数据。  相似文献   

6.
焊后热处理对P92钢管道焊接残余应力场的影响   总被引:5,自引:3,他引:2       下载免费PDF全文
采用红外热成像仪测量了P92钢管道在焊接过程中的温度场分布,由此获得P92钢焊接过程的温度循环曲线;采用有限元方法模拟了P92钢管道多层多道焊的整个焊接过程,获得焊接温度场分布,与P92钢焊接温度场实测结果吻合良好,验证了模拟计算的准确性;采用间接法,利用温度场结果计算了P92钢管道环焊缝焊接形成的残余应力场,并重点分析了焊后热处理前后的焊接残余应力变化情况.结果表明,焊后热处理对P92钢管道焊接残余应力具有明显的消除作用,但不能完全消除,焊缝中依然存在较大的拉伸残余应力.  相似文献   

7.
低碳钢薄板单道堆焊焊接变形的数值模拟   总被引:2,自引:1,他引:1       下载免费PDF全文
周一俊  邓德安  冯可  毕涛 《焊接学报》2013,(12):101-104
基于ABAQUS有限元分析软件,开发了考虑移动热源、材料非线性和几何非线性的热-弹-塑性有限元计算方法.利用所开发的数值方法对薄板单道堆焊时的焊接残余应力和变形进行了模拟.同时采用试验方法测量了薄板接头的焊接变形和残余应力.通过对比数值模拟结果和试验结果,验证了所开发方法的有效性.在同时考虑几何非线性与材料非线性的情况下,有限元计算得到的焊接变形结果与实测值一致;计算得到的焊接残余应力也与实测值比较吻合.此外利用数值模拟方法详细研究了薄板焊接变形的特点和残余应力的分布特征.  相似文献   

8.
以DP980高强钢板带材为例,研究其激光拼焊过程中的残余应力、焊接变形与焊接工艺参数的关系,用热-力耦合的方法模拟带钢激光焊接过程,通过试验验证了模型的可信度.最后设置不同工况,分析焊接工艺参数对其残余应力及变形的影响.结果 表明:焊接残余应力与变形随着焊接速度的增大有减小的趋势,焊接速度在2.0~3.0 m/min时...  相似文献   

9.
焊接的非平衡加热、冷却过程导致产生焊接应力与变形,而焊接残余变形是影响结构设计完整性、制造工艺合理性和结构使用可靠性的关键因素.本文基于"局部-整体"映射法.模拟了局部模型为T形接头角焊缝的局部塑性应变,并把结果用于薄壁箱形梁的焊接装配变形数值仿真,同时对不同焊接顺序产生的残余变形情况进行了分析和探讨,并将预测结果与焊接工艺试验结果进行了对比验证,二者吻合很好,从而为研究焊接顺序对大型焊接结构变形的影响提供了一种方法.  相似文献   

10.
沟槽蒙皮结构激光焊接应力和变形的数值模拟   总被引:3,自引:2,他引:1       下载免费PDF全文
利用有限元分析软件MARC对"沟槽-蒙皮"结构的激光焊接过程进行三维数值模拟,涉及了激光焊接复合热源模型的确定,热力学边界条件的简化,数值模拟温度场的验证,以及残余变形和应力分布结果的分析和讨论.研究了结构上规则排列的多道焊缝的施焊顺序对焊接残余应力和变形的影响.结果表明,不同焊接顺序所产生的变形态相同,变形量有区别,而残余应力的分布则不同,以由外向中的对称顺序进行焊接时,结构的焊后残余变形最小,残余应力的分布比较均匀,峰值最小.  相似文献   

11.
In as-welded state, each region of 2219 aluminum alloy TIG-welded joint shows diff erent microstructure and microhardness due to the diff erent welding heat cycles and the resulting evolution of second phases. After the post-weld heat treatment, both the amount and the size of the eutectic structure or θ phases decreased. Correspondingly, both the Cu content in α-Al matrix and the microhardness increased to a similar level in each region of the joint, and the tensile strength of the entire joint was greatly improved. Post-weld heat treatment played the role of solid solution strengthening and aging strengthening. After the post-weld heat treatment, the weld performance became similar to other regions, but weld reinforcements lost their reinforcing eff ect on the weld and their existence was more of an adverse eff ect. The joint without weld reinforcements after the post-weld heat treatment had the optimal tensile properties, and the specimens randomly crack in the weld zone.  相似文献   

12.
After nearly two years' tense construction, the first phase of industrialized base of Shenyang Research Institute of Foundry (SRIF), located at the Tiexi Casting and Forging Industrial Park in the west of Tiexi District, has now been completed and formally put into operation.  相似文献   

13.
吴玉梅  熊晓云  靳蓉  孙敬民  杨林  罗晓星 《金属学报》2005,10(10):1100-1103
目的: 观察本实验室合成的一种治疗阿尔茨海默氏症(AD)的药物(1-二甲基磷酰基-2, 2, 2 -三氯)-乙基-1-醇烟酸醋(NMF),对体外培养的皮层神经细胞活性的影响以及对海人藻酸(KA)所致的神经损伤的保护作用。方法: 采用体外培养皮层神经元的方法,解剖分离 15 d胚胎小鼠皮层神经细胞, 接种于 96孔板,48 h 后加药并培养 72 h,以 MIT 法 观察 NMF 对小鼠皮层神经细胞活性的影响;同时将接种于 24 孔板的细胞预先给予 NMF,d 3 时加或不加KA处理后,以台盼蓝染色鉴别并计数死、活细胞,可得出细胞的存活率。结果: NMF 明显促进胎鼠皮层神经元活性,其中 NMF1、0. 1、10nmol·L-1促进神经元活性增殖率分别高达 34.7%、37.4%、36. 7%, NMF 明显促进正常胎鼠皮层神经元存活卒,与对照组比较,10nmol·L-1 NMF 对皮层神经元的存活率分别提高 39.3%、73.5%。 NMF能显著 对抗 KA 所致的神经元损伤,与 KA 损伤组相比, NMF0.1、10、10nmol·L-1对损伤皮层神经元的保护率分别为 77.30%、80.10%、84.15%。结论: NMF 明 显促进胎鼠皮层神经元的洁性、提高正常皮层神经元,的存活卒,并能有效地保护KA所致的神经元损伤,提示 NMF 是一种很有潜力的治疗 AD 的药物。  相似文献   

14.
The motion of melt droplets in spray degassing process was analyzed theoretically. The height of the treatment tank in spray degassing process could be determined by the results of theoretical calculation of motion of melt droplets. To know whether the melt droplets would solidify during spraying process, the balance temperature of melt droplets was also theoretically analyzed. Then proof experiments for theoretical results about temperature of melt droplets were carried. In comparison, the experimental results were nearly similar to the calculation results.  相似文献   

15.
On the basis of the single-particle framework, a new theory on inclusion growth in metallurgical melts is developed to study the kinetics of inclusion growth on account of reaction and collision. The studies show that the early growth of inclusion depends on reaction growth and Brawnian motion collision, and where the former is decisive, the late growth depends on turbulence collision and Stokes' collision, and where the former is dominant; collision growth is very quick during the smelting process, lessened in the refining process, but nearly negligible in the continuous casting process.  相似文献   

16.
Coherent second phase often exhibits anisotropic morphology with specifi c orientations with respect to both the second and the matrix phases. As a key feature of microstructure, the morphology of the coherent particles is essential for understanding the second-phase strengthening eff ect in various industrial alloys. This letter reports anisotropic growth of coherent ferrite from austenite matrix in pure iron based on molecular dynamics simulation. We found that the ferrite grain tends to grow into an elongated plate-like shape, independent of its initial confi guration. The fi nal shape of the ferrite is closely related to the misfi t between the two phases, with the longest direction and the broad facet of the plate being, respectively, consistent with the best matching direction and the best matching plane calculated via the Burgers vector content(BVC) method. The strain energy calculation in the framework of Eshelby's inclusion theory verifi es that the simulated orientation of the coherent ferrite is energetically favorable. It is anticipated that the BVC method will be applicable in analysis of anisotropic growth and morphology of coherent second phase in other phase transformation systems.  相似文献   

17.
An approach based on film buckling under simple uniaxial tensile testing was utilized in this paper to quantitatively estimate the interfacial energy of the nanostructured multilayer films(NMFs) adherent to flexible substrates. The interfacial energies of polyimide-supported NMFs are determined to be *5.0 J/m2 for Cu/Cr, *4.1 J/m2 for Cu/Ta,*2.8 J/m2 for Cu/Mo, *1.1 J/m2 for Cu/Nb, and *1.2 J/m2 for Cu/Zr NMFs. Furthermore, a linear relationship between the adhesion energy and the interfacial shear strength is clearly demonstrated for the Cu-based NMFs, which is highly indicative of the applicability and reliability of the modified models.  相似文献   

18.
A 17 vol% SiCp/Al–Mg–Si–Cu composite plate with a thickness of 3 mm was successfully friction stir welded(FSWed) at a very high welding speed of 2000 mm/min for the first time. Microstructural observation indicated that the coarsening of the precipitates was greatly inhibited in the heat-affected zone of the FSW joint at high welding speed, due to the significantly reduced peak temperature and duration at high temperature. Therefore, prominent enhancement of the hardness was achieved at the lowest hardness zone of the FSW joint at this high welding speed, which was similar to that of the nugget zone. Furthermore, the ultimate tensile strength of the joint was as high as 369 MPa, which was much higher than that obtained at low welding speed of 100 mm/min(298 MPa). This study provides an effective method to weld aluminum matrix composite with superior quality and high welding efficiency.  相似文献   

19.
On the basis of energy and shape method for the determination of the valence bond (VB) structures of crystal, the valence bond structure of titanium is redetermined at room temperature and calculated in the whole temperature range of 0-1943K. The outer shell electronic distribution of Ti is e_c~(2.9907) · (s_c~(0.4980) d_c~(2.4927)) ef1.0093 in crystal. The temperature dependences of the VB structures of hcp and bcc phases are the same. The VB structures of hcp and bcc phases monotonically increase or decrease with the increase in temperature, but show discontinuous changes at the phase-transformation temperature 1155K.  相似文献   

20.
The Lanthanum-doped bismuth ferrite–lead titanate compositions of 0.5(Bi LaxFe1-xO3)–0.5(Pb Ti O3)(x = 0.05,0.10,0.15,0.20)(BLxF1-x-PT) were prepared by mixed oxide method.Structural characterization was performed by X-ray diffraction and shows a tetragonal structure at room temperature.The lattice parameter c/a ratio decreases with increasing of La(x = 0.05–0.20) concentration of the composites.The effect of charge carrier/ion hopping mechanism,conductivity,relaxation process and impedance parameters was studied using an impedance analyzer in a wide frequency range(102–106Hz) at different temperatures.The nature of Nyquist plot confirms the presence of bulk effects only,and non-Debye type of relaxation processes occurs in the composites.The electrical modulus exhibits an important role of the hopping mechanism in the electrical transport process of the materials.The ac conductivity and dc conductivity of the materials were studied,and the activation energy found to be 0.81,0.77,0.76 and 0.74 e V for all compositions of x = 0.05–0.20 at different temperatures(200–300 °C).  相似文献   

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