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1.
《稀有金属》2016,(7)
Zr-4合金广泛用作大多数压水堆和反应堆的燃料包壳材料,因此针对其焊接的研究有非常重要的现实意义。论文采用数值模拟方式研究Zr-4合金电子束焊接的瞬态过程,采用双椭球热源模型,结合接触及辐射等边界条件,采用变密度六面体网格,耦合温度场和应力场,建立了Zr-4合金管电子束焊接的有限元瞬态数学模型,采用自适应时间步,计算了Zr-4合金管真空电子束焊接的三维瞬态温度场和应力场。数值模拟结果表明:在电子束功率相对较小的条件下,焊缝深宽比较小,采用双椭球热源模型进行数值模拟,所获熔池形状与实验所得焊缝成形吻合良好,证明了该数学模型的合理性,从而可为制定实际焊接工艺提供理论指导。在所设定的计算条件下,筒盖和筒体均变形均匀,主要表现形式为沿径向突出,且筒盖变形大于筒体,和实际焊接现象基本一致;焊后最大整体变形约0.02 mm。 相似文献
2.
对铝合金5A06简体纵缝进行激光深熔焊接。建立了该条件下的焊接热源模型,热源模型由沿激光入射方向的旋转高斯体热源构成。使用该热源模型和ANSYS有限元分析软件对前述的试验进行了数值模拟。为制定和优化焊接工艺提供必要的参考。 相似文献
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《粉末冶金材料科学与工程》2015,(4)
选择双椭球热源模型对M42高速钢/X32弹簧钢双金属带锯的电子束焊接的温度场进行Ansys数值模拟,确定焊接的最佳工艺参数,并进行焊接试验,利用扫描电镜观察M42/X32接头的微观组织。结果表明,最佳焊接工艺为焊接电压U=140 k V,焊接电子束电流Ib=20 m A,焊接速度v=2 m/min。在此工艺条件下进行电子束焊接实验,焊缝宽度实验值和计算值的相对误差为-3%~1.5%,二者吻合较好,验证了双椭球热源模型在电子束焊接温度场模拟中的适用性。M42/X32接头的焊缝中心为等轴晶和柱状晶的典型铸态组织;M42熔合区(FZ)组织为马氏体和M2C型碳化物,M42热影响区(HAZ)组织为马氏体、残余奥氏体及碳化物。X32熔合区(FZ)由类马氏体层和马氏体组织组成,X32热影响区(HAZ)组织为马氏体、残余奥氏体以及M23C6。 相似文献
5.
根据电子束焊接焊缝形貌特征及其深宽比大等特点,选用复合热源作为热源模型.通过线性插值等方式估计材料热力学参数随温度变化,模拟Ti基非晶合金电子束焊接温度场.模拟结果与实际焊缝取得良好的吻合,验证了热源模型的准确性.获得一定变量参数下电子束焊接钛基非晶合金温度场及热循环曲线.在温度场的基础上再进行焊接应力场的模拟,获得残余应力分布曲线.实验验证整个焊件没有晶化相析出,验证了该焊接工艺的可行性. 相似文献
6.
针对过去采用弹塑性体邓肯应力-应变模型确定矿山废石场散体的弹性模理(E)及泊松比(μ)的计算过程繁琐、计算公式复杂,提出了改进的计算模型。新模型将原来确定模型参数的5个关系式减少到2个,使计算公式和计算过程简化。 相似文献
7.
将螺旋埋管等效为三维螺旋线热源,考虑螺旋埋管能源桩的传热过程,运用格林函数和第一型曲线进行积分,推导给出了考虑时间、空间位置、埋管参数和岩土体热物理性质4参数的螺旋埋管能源桩的温度场解析解,建立高精度三维螺旋埋管能源桩的传热模型。并通过在数值模拟软件中建立螺旋埋管能源桩三维模型,依据边界条件,求解得出三维螺旋埋管能源桩温度场数值解。对比结果表明:所建立的能源桩三维螺旋线热源模型具有很高的解析精度。最后,基于解析模型讨论了螺旋埋管能源桩换热温度场的空间分布和时间效应。 相似文献
8.
模拟了04Cr13Ni5Mo超级马氏体不锈钢不同焊接热循环条件下热影响区组织,进行了焊条电弧焊接及焊后热处理试验,分析了焊接热模拟试样及焊条电弧焊接头的微观组织、力学性能.焊接热模拟试验结果表明,模拟热影响区的组织主要为低碳板条马氏体,其硬度较母材有较大提高,冲击韧性有所下降;模拟单道焊或多道焊时,不同的冷却速度及层间热处理对模拟热影响区的硬度及冲击韧性影响不大,600℃焊后回火热处理可以明显软化模拟热影响区组织,并让其冲击韧性恢复到较高水平.焊条电弧焊接结果表明,采用04Cr13Ni5MoRe型焊条及配套的焊后热处理工艺,可以获得良好综合力学性能的焊接接头. 相似文献
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采用激光-电弧复合焊,激光前置焊接海工钢AH36薄板。利用高速摄像分析熔滴过渡特征与影响因素。运用计算流体力学体积分数法建立固液气三相流体动力学模型。采用高斯面热源、高斯旋转体热源和双椭球热源表征复合焊热源。数值模型考虑了表面张力、电磁力、浮力、反冲压力、蒸发冷凝、蒸发换热等多种物理场的耦合作用。对熔滴过渡冲击及其对熔池形貌、流动与温度的影响进行研究。结果表明,熔滴冲击熔池可促进熔池流动与传热。熔滴过渡受电磁力与蒸气反冲压力抑制,致使大熔滴出现。适当增加激光功率可降低熔滴表面张力,增加熔滴过渡频率,减小熔滴尺寸。激光功率过大或光丝间距过小时,出现熔滴破裂与飞溅。 相似文献
11.
An analytical solution for the temperature-rise distribution in arc welding of short workpieces is developed based on the
classical Jaeger’s moving heat-source theory to predict the transient thermal response. It, thus, complements the pioneering
work of Rosenthal and his colleagues (and others who extended that work), which addresses quasi-stationary moving heat-source
problems. The arc beam is considered as a moving plane (disc) heat source with a pseudo-Gaussian distribution of heat intensity,
based on the work of Goldak et al. It is a general solution (both transient and quasi-steady state) in that it can determine the temperature-rise distribution
in and around the arc beam heat source, as well as the width and depth of the melt pool (MP) and the heat-affected zone (HAZ)
in welding short lengths, where quasi-stationary conditions may not have been established. A comparative study is made of
the analytical approach of the transient analysis presented here with the finite-element modeling of arc welding by Tekriwal
and Mazumder. The analytical model developed can determine the time required for reaching quasi-steady state and solve the
equation for the temperature distribution, be it transient or quasi-steady state. It can also calculate the temperature on
the surface as well as with respect to the depth at all points, including those very close to the heat source. While some
agreement was found between the results of the analytical work and those of the finite-element method (FEM) model, there were
differences identified due to differences in the methods of approach, the selection of the boundary conditions, the need to
consider image heat sources, and the effect of variable thermal properties with temperature. The analysis presented here is
exact, and the solution can be obtained quickly and in an inexpensive way compared to the FEM. The analysis also facilitates
optimization of process parameters for good welding practice. 相似文献
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A new finite element model for welding heat sources 总被引:34,自引:0,他引:34
John Goldak Aditya Chakravarti Malcolm Bibby 《Metallurgical and Materials Transactions B》1984,15(2):299-305
A mathematical model for weld heat sources based on a Gaussian distribution of power density in space is presented. In particular
a double ellipsoidal geometry is proposed so that the size and shape of the heat source can be easily changed to model both
the shallow penetration arc welding processes and the deeper penetration laser and electron beam processes. In addition, it
has the versatility and flexibility to handle non-axisymmetric cases such as strip electrodes or dissimilar metal joining.
Previous models assumed circular or spherical symmetry. The computations are performed with ASGARD, a nonlinear transient
finite element (FEM) heat flow program developed for the thermal stress analysis of welds.* Computed temperature distributions
for submerged arc welds in thick workpieces are compared to the measured values reported by Christensen1 and the FEM calculated values (surface heat source model) of Krutz and Segerlind.2 In addition the computed thermal history of deep penetration electron beam welds are compared to measured values reported
by Chong.3 The agreement between the computed and measured values is shown to be excellent. 相似文献
14.
Numerical analysis of metal transfer in gas metal arc welding under modified pulsed current conditions 总被引:2,自引:0,他引:2
A method has been proposed to pulsate current in gas metal arc welding (GMAW) to achieve a specific type of desirable and
repeatable metal transfer mode, i.e., one drop per pulse (ODPP) mode. This method uses a peak current lower than the transition current to prevent accidental
detachment and takes advantage of the downward momentum of the droplet oscillation to enhance the detachment. A numerical
model with advanced computational fluid dynamics (CFD) techniques, such as a two-step projection method, volume of fluid (VOF)
method, and continuum surface force (CSF) model, was used to carry out the simulation for the metal transfer process. The
Gauss-type current density distribution was assumed as the boundary condition for the calculation of the electromagnetic force.
The calculations were conducted to demonstrate the effectiveness of the proposed method in achieving the desired metal transfer
process in comparison with conventional pulsed current GMAW. Also, the critical conditions for effective use of this proposed
method were identified by the numerical simulation. Comparison showed good agreement between calculation and experimental
results. 相似文献
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16.
Numerical analysis of metal transfer in gas metal arc welding 总被引:1,自引:0,他引:1
The present article describes a numerical procedure to simulate metal transfer and the model will be used to analyze the transport
processes involved in gas metal arc welding (GMAW). Advanced Computational fluid dynamics (CFD) techniques used in this model
include a two-step projection method for solving the incompressible fluid flow; a volume of fluid (VOF) method for capturing
free surface; and a continuum surface force (CSF) model for calculating surface tension. The electromagnetic force due to
the welding current is estimated by assuming several different types of current density distribution on the free surface of
the drop. The simulations based on the assumption of Gaussian current density distribution show that the transition from globular
to spray transfer mode occurs over a narrow current range and the size of detached drops is nonuniform in this transition
zone. The analysis of the calculation results gives a better understanding of this physical procedure. Comparisons between
calculated results and experimental results are presented. It is found that the results computed from the Gaussian assumption
agree well with those observed in experiments. 相似文献
17.
分析50MN挤压机张力柱的断裂原因,介绍采用埋弧自动焊焊接修复大型工件的工艺过程、焊接采取的措施,以及焊接修复后张力柱的强度校核。 相似文献
18.
This article is Part II of a two-part series on the thermal analysis of the arc welding process. In Part I, general solutions
for the temperature rise distribution in arc welding of short workpieces were developed based on Jaeger’s classical moving
heat source theory for a plane disc heat source with a pseudo-Gaussian distribution of heat intensity and constant values
of thermophysical properties at one temperature (400 °C). This was extended in this investigation (Part II) to consider different
thermophysical properties at different temperatures (from room temperature (25 °C) to 1300 °C) for a mild steel work material.
The objective is to develop a rationale for the selection of an appropriate temperature for the choice of the thermophysical
properties for the thermal analysis of arc welding. Since the quality of the weld for a given work material depends both on
the thermodynamic and kinetic considerations, namely, the maximum temperatures and the temperature gradients (cooling rates)
in appropriate sections of the welded part including the weld bead and the heat-affected zone (HAZ), they were determined
in this investigation. The main output parameters from a thermal point of view are the widths and the depths of the melt pool
(MP) and the HAZ at the weld joint. Although the length of the weld pool is also a consideration, if the entire length participates
in the welding process, which is generally the case, then this is not such an important consideration. It is found that for
welds produced in a conductive mode only (i.e., not considering the case of deep penetrating welds produced with keyhole mode), the values of the widths and the depths
of the MP and the HAZs are nearly the same (within 10 to 20 pct), irrespective of the values of thermal properties for temperatures
in the range of 400 °C to 1300 °C. Hence, the emphasis on the need to consider variable thermal properties with temperature
in welding appears to be somewhat exaggerated. Also, based on the thermal analysis of the welding process, it appears that
the room-temperature thermophysical properties may not be appropriate, as rightly pointed out by other researchers. The thermal
history and the cooling rates were also determined analytically for arc welding of long workpieces, where quasi-steady-state
conditions are established and the boundary effects can be ignored, as well as short workpieces, where transient conditions
prevail and boundary effects need to be considered. This information can then be used in the appropriate time-temperature-transformation
(TTT) diagram for a given steel work material to investigate the nature of the metallurgical transformation and the resulting
microstructure in the welding process both in the weld bead and in the adjacent HAZs on either side. 相似文献
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20.
A finite-element (FE) simulation process integrating three dimensional (3D) with two-dimensional (2D) models is introduced
to investigate the residual stress of a thick plate with 50-mm thickness welded by an electron beam. A combined heat source
is developed by superimposing a conical volume heat source and a uniform surface heat source to simulate the temperature field
of the 2D model with a fine mesh, and then the optimal heat source parameters are employed by the elongated heat source for
the 3D simulation without trial simulations. The welding residual stress also is investigated with emphasis on the through-thickness
stress for the thick plate. Results show that the agreement between simulation and experiment is good with a reasonable degree
of accuracy in respect to the residual stress on the top surface and the weld profile. The through-thickness residual stress
of the thick plate induced by electron beam welding is distinctly different from that of the arc welding presented in the
references. 相似文献