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[温度] 移动热源加载问题

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发表于 2011-4-25 18:50:16 | 显示全部楼层 |阅读模式 来自 江苏南京
我想做焊接过程的模拟,但是如何用ADINA加载移动热源呢,热流密度恒定,想参考primer例A58做,但是没有成功,请各位大侠帮忙,谢谢
发表于 2011-4-25 21:27:35 | 显示全部楼层 来自 江苏镇江
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我记得我有焊接的例子,哪天给你找找
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 楼主| 发表于 2011-4-26 08:03:18 | 显示全部楼层 来自 江苏南京
我整了好久了都没弄出来,抓狂阿,知识还是不够啊,谢谢 2# nickcoom
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 楼主| 发表于 2011-4-27 18:47:29 | 显示全部楼层 来自 江苏南京
我的邮箱[email=723783068@qq.com,麻烦您找到了发下723783068@qq.com,麻烦您找到了发下[b[/email]] 2# nickcoom
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发表于 2011-4-30 08:06:26 | 显示全部楼层 来自 湖北武汉
Thermo-mechanical Analysis of Electron Beam Welding Electron beam welding is a fusion welding process that utilizes the kinetic energy of a high-velocity electron beam, which upon impact on the workpiece heats it up due to conversion of its kinetic energy to thermal energy. In this Brief, we present the results of a numerical modeling of the electron beam welding process of two steel tubes with different diameters. The numerical results are also compared with the available experimental data (see Ref.). Figure 1 shows a representative specimen and a close-up of the welded region.



Figure 1  The welded specimen


One half of the finite element model used for modeling the welding process is depicted in Figure 2. The movement of the heat source was simulated by applying the heat source to only one prism element along the circumference of the welding zone in each instance. There are 72 prisms along the circumference, each corresponding to 5° rotation of the heat source. The heat flux was applied in pulses, with an idle time between each pulse, to model the actual experimental condition. Since the electron beam welding is usually performed in a vacuum, the convection coefficient was set to zero on the tube walls. Each of the welding pulses was discretized by 100 time steps. Temperature-dependent thermal properties were used for modeling the thermal behavior of the tubes. A temperature-dependent elasto-plastic material model, in which the yield stress and the strain hardening modulus are functions of temperature, was used in the stress analysis. The movie above shows the evolution of the temperature field along the welding path as the heat source moves along the circumference of the tubes.




Figure 2  One half of the finite element model used in the analyses


Figure 3 presents the temperature variation as a function of time, for the welding speed of 10 mm/s, for the points located on the same plane perpendicular to the tube axis but at different depth through the thickness. Figure 4 shows the temperature variation as a function of time for the points located at the same depth through the thickness but at different distances normal to the welding plane for the welding speed of 10 mm/s. Figure 5 shows the temperature variation as a function of time for a single point but for different welding speeds.

Figure 3 Time variation of temperature in the weld zone (10 mm/s speed of welding)




Figure 4 Time variation of temperature in the weld zone (10 mm/s speed of welding)




Figure 5 Time variation of temperature at a single point, for different welding speeds


Figure 6 depicts the snapshots of the temperature variation as well as the thermal stresses in the tubes resulting from the coupled thermo-mechanical analysis at different times during the pulse period. It can be seen that the lowest values of effective stress occur in the molten pool while the highest values of effective stress occur around the molten pool. Figure 7 presents a comparison between the numerical and experimental results. The isothermal lines obtained using the finite element method are superimposed on a picture of the welded region. A reasonable agreement is reported for the lower parts of the welded region. However, there is a discrepancy between the results for the upper portion. The main reason for the difference is that the specimen has undergone a secondary heat treatment to smooth out the weld face but this secondary heat treatment was not modeled in the numerical analysis.




Figure 6  Temperature field and effective stress band plots for (a) half of the pulse duration (b) end of the pulse (c) end of the idle period between pulses




Figure 7  Comparison between the temperature fields obtained using the FEA and experimental data


This study shows some of the capabilities of ADINA for solving industrial problems involving strong coupling between the thermal field and the mechanical deformations. For more information, please refer to our page on thermo-mechanical coupling capabilities of ADINA. Reference
  • P. Lacki, K. Adamus, "Numerical simulation of the electron beam welding process", Computers and Structures, 2011, in press.

Keywords:
Electron beam welding, thermo-mechanical coupling, residual stress, thermo elasto-plastic material, moving heat source
Courtesy of P. Lacki and K. Adamus (Czestochowa University of Technology, Poland)
4# dedi
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发表于 2011-5-4 09:17:37 | 显示全部楼层 来自 广西桂林
5# wry618
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发表于 2011-5-7 08:50:18 | 显示全部楼层 来自 大连理工大学
看到你的帖子,你应该是在ANSYS方面非常强大的一人,我现在属于初学者,刚自己写了一个小程序,我的初衷是高斯热源从Y轴中间最上方开始往下加载贯穿Y轴,按道理最高温度在最下面也应该有,但是却不是我预想的那样,附件里有最终求截图和命令流,望你能帮我看看,究竟是哪块出问题了,谢谢了

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发表于 2011-5-7 20:17:10 | 显示全部楼层 来自 北京
我记得苦苦视频里不是有个移动载荷的例子,这个与时间函数有关系,与施加载荷时的arrival time也有关系,自己琢磨下吧,呵呵。

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发表于 2011-5-8 08:11:44 | 显示全部楼层 来自 湖北武汉
关键我用的ADINA啊,ansys很久都没有用了( ⊙ o ⊙ )啊! 7# abcmn0233
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