TY - JOUR A1 - Artinov, Antoni A1 - Karkhin, Victor T1 - Геометрические различия между кратером шва и сварочной ванной T1 - Geometric differences between end crater and weld pool N2 - Приведено аналитическое решение задачи теплопроводности после прекращения действия подвижного источника теплоты для различных комбинаций источника и свариваемого тела. Показано, что после выключения источника возможно дополнительное плавление основного металла за счет перегретого жидкого металла сварочной ванны. Например, при лазерной сварке со сквозным проплавлением стальной пластины толщиной 2 мм длина кратера шва может быт на 19% больше установившейся длины сварочной ванны. Установлено, что центр кратера, в котором заканчивается затвердевание жидкого металла, смещен в сторону хвостовой части кратера относительно оси теплового источника в момент прекращения его действия. Скорость и направление кристаллизации металла сварочной ванны и кратера различны. N2 - A functional-analytical solution of the problem of heat conduction after the moment of switch-off of the moving heat source is presented. Different combinations of heat sources and heated bodies are considered. It is demonstrated that an additional melting of the base metal is possible after the switch-off due to the overheated weld pool metal. For example, in laser beam keyhole welding of a 2 mm thick steel plate, the crater can be 19% longer than the weld pool. It is found that the crater centre, where the solidification of the liquid metal ends, is displaced from the heat source axis at the moment of switch-off towards the weld pool tail. The rate and the direction of crystallization of the molten metal in the weld pool and the end crater differ significantly. KW - сварочная ванна KW - кратер шва KW - плавление, KW - кристаллизация, KW - температурное поле KW - функция теплонасыщения KW - Weld pool KW - End crater KW - Melting KW - Solidification KW - Temperature field KW - Heat saturation function PY - 2019 SN - 2071-5234 SP - 19 EP - 23 PB - National Agency for Control and Welding CY - Moscow AN - OPUS4-50289 LA - rus AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Ivanov, S. A1 - Vildanov, A. A1 - Golovin, P. A1 - Artinov, Antoni A1 - Karpov, I. T1 - Effect of Inter-Layer Dwell Time on Distortion and Residual Stresses of Laser Metal Deposited Wall N2 - The laser metal deposition is an advanced manufacturing technology enabling the production of large-sized parts and partially or completely elimination of machining and welding. The process is characterised by non-uniform local heating of the buildup leading to a stress distribution, which may exceed the yield strength of the material and leads to loss of dimensional accuracy. The interlayer dwell time has a strong influence on the temperature field. The effect of the interlayer dwell time on the distortion and the stress distribution during laser metal deposition of a single-pass wall on the edge of 2 mm thick plate was studied experimentally and numerically. The deposited material was IN625 and the substrate material was AISI 316. A decrease of the residual displacement, due to a uniform shrinkage after the deposition of the last layer and a lower level of the residual compressive longitudinal plastic strain, has been observed in the studies without dwell time. The peak increment of the free edge displacement corresponds to the first layer and hence the subsequent layers will be deposited on the already plastically deformed buildup. The tensile residual longitudinal stress near the top of the buildup and transverse stress near the edges of the buildup is higher than yield strength in the studies with dwell time. KW - Laser metal deposition KW - Distortion KW - Residual stresses KW - Temperature field KW - Simulation PY - 2019 DO - https://doi.org/10.4028/www.scientific.net/KEM.822.445 SN - 1662-9795 VL - 822 SP - 445 EP - 451 PB - Trans Tech Publications Ltd. AN - OPUS4-49113 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Thater, Raphael A1 - Perret, William A1 - Schwenk, Christopher A1 - Alber, U. A1 - Rethmeier, Michael T1 - Industrial application of welding temperature field and distortion visualization using FEA KW - Numerical welding simulation KW - Temperature field KW - Distortion KW - Industrial application KW - Automotive assembly PY - 2010 SN - 0387-4508 VL - 39 IS - 2 SP - 232 EP - 234 CY - Osaka, Japan AN - OPUS4-24354 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - CONF A1 - Perret, William A1 - Alber, U. A1 - Schwenk, Christopher A1 - Rethmeier, Michael ED - Wieland, H.-J. T1 - Efficient welding simulation of an automotive sheet metal assembly N2 - Fusion welding is widely used in the automotive industry to join metal structures. It is well-known that distortions and residual stresses occur during and after the welding process. Many procedures exist to decrease these negative heat effects of welding, but are often coupled with highly cost intensive experiments. The implementation of a welding Simulation tool to reduce this very expensive experimental procedures is therefore of high interest. Despite the fact that the automotive industry is a key sector for Simulation procedures, welding Simulation Software is nevertheless not yet widely implemented. This is mainly due to the complexity of the Simulation tools requiring expert users and the resulting high time to Solution. In this study, a new fast thermo-mechanical Simulation of a complex and large laser beam welded automotive sheet metal assembly with several non linear welds is simulated. Assumptions and simplifications of the complex physical welding phenomenon, which are made to keep the computational cost and the complexity of the Simulation in an industrial frame, are discussed. The calibration time of the phenomenological heat source model has been optimized with a very fast analytical thermal model and the resulting simulated temperature fields match perfectly with the measured ones. Additionally, the user experience and the time-to-solution are kept within a reasonable time frame for arr industrial environment. All Simulation results are validated with experimental results. T2 - SCT2011 - 3rd International conference on steels in cars and trucks CY - Salzburg, Austria DA - 05.06.2011 KW - Welding simulation KW - Temperature field KW - Laser beam welding KW - Fast calculation PY - 2011 SN - 978-3-514-00783-3 SP - 704 EP - 713 PB - Stahleisen AN - OPUS4-24088 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - GEN A1 - Schwenk, Christopher A1 - Rethmeier, Michael ED - Cerjak, H. ED - Enzinger, N. T1 - Structured approach for a transient 3D numerical welding simulation KW - Numerical welding simulation KW - Experimental validation KW - Temperature field KW - Welding distortion KW - Residual stress PY - 2010 SN - 978-3-85125-127-2 SP - 901 EP - 917 PB - Verlag der Technischen Universität Graz AN - OPUS4-23153 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - CONF A1 - Thater, Raphael A1 - Perret, William A1 - Schwenk, Christopher A1 - Alber, U. A1 - Rethmeier, Michael T1 - Industrial application of welding temperature field and distortion visualization using FEA N2 - The non-uniform heat input during the welding process leads to problematic permanent deformations of welded parts. The control of these welding distortions is, with the absence of the knowledge of the fundamental mechanisms responsible for these deformations, an extremely time and cost consuming iterative “trial-and-error” optimization process. The visualization of the involved physical phenomena, like temperature and distortions, .is an indispensable tool to clearly identify these mechanisms in order to adapt the welding parameters and clamping conditions target-oriented. Both experimental and virtual methods exist to obtain these physical data, however the possibilities to visualize them with experimental methods are laborious, expensive and limited in their application. Welding Simulation using finite element analysis (FEA) offers many benefits and has a great potential to reduce the experimental effort. Nevertheless, the industrial application of welding Simulation is not yet established widely because of reservations regarding the computation costs and the resulting accuracy for instance. In this paper, the results of a case study for a welding Simulation with an industrial background are presented. A welded assembly from the automotive industry has been investigated with numerical and experimental methods. A comparison between both methods demonstrates the Potentials of welding Simulation in terms of visualization. Furthermore, the numerical results reveal the possibilities of current resources. regarding calculation time and result accuracy of an industrial applied welding Simulation. T2 - VISUAL-JW 2010 - The international symposium on visualization in joining & welding science through advanced measurements and simulation CY - Osaka, Japan DA - 11.11.2010 KW - Numerical welding simulation KW - Temperature field KW - Distortion KW - Industrial application KW - Automotive assembly PY - 2010 VL - 1 IS - PT-31 SP - 245 EP - 246 AN - OPUS4-22721 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - CONF A1 - Perret, William A1 - Thater, R. A1 - Alber, U. A1 - Schwenk, Christopher A1 - Rethmeier, Michael T1 - Case study for welding simulation in the automotive industry T2 - INPRO - Intermediate meeting - IIW-Select committee "automotive and road transport" DA - 2010-04-21 KW - Welding simulation KW - Temperature field KW - Distortion KW - Automotive industry KW - Experimental validation PY - 2010 IS - IIW-Doc. No. SC-Auto-37-10 SP - 1 EP - 13 AN - OPUS4-22541 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Perret, William A1 - Schwenk, Christopher A1 - Rethmeier, Michael T1 - Comparison of analytical and numerical welding temperature field calculation N2 - Analytical and numerical methods are used to estimate the temperature field due to the heat effects of welding. Numerical techniques are more adapted for industrial complex applications where analytical solutions do not exist yet. However, computational time is much lower with analytical models and a combination of both methods is investigated. Therefore, the two approaches are introduced and confronted in this paper. The finite-element software Ansys has been used for numerical simulations and Scilab for analytical simulations. In order to get a similar result quality, both methods have to be analysed and compared with respect to boundary conditions. These configurations are presented in this paper. Before starting any analysis, the analytical and numerical models have to be comparable. For the numerical simulation, every in- or output is given in discrete form and, for the analytical simulation, in continuous form. Thus, an analysis of the energy input distribution in both models is compulsory to ensure that the same amount of energy is applied. After this first study, a comparison of the analytical and numerical temperature field simulation is done from a fix point source in an infinite volume in steady state to a moving point source in a finite dimension in a transient state. A good agreement between the analytical and the numerical simulation results is found. However, some techniques, like a consideration of an image heat source for the analytical model or the selection of boundary conditions for the numerical model, need to be taken into consideration when the degree of complexity of the study (finite dimension or cooling time) increases. The limit of the comparison is reached when the geometry becomes too complex and when the effect of variable thermal properties with temperature cannot be neglected. KW - Welding simulation KW - Temperature field KW - Analytical approach KW - Numerical approach KW - Heat conduction PY - 2010 DO - https://doi.org/10.1016/j.commatsci.2009.11.032 SN - 0927-0256 VL - 47 IS - 4 SP - 1005 EP - 1015 PB - Elsevier CY - Amsterdam AN - OPUS4-20887 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER -