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 JF - Key Engineering Materials 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 - Artinov, Antoni A1 - Karkhin, Victor T1 - Геометрические различия между кратером шва и сварочной ванной T1 - Geometric differences between end crater and weld pool JF - Наука и техника JF - Welding and diagnostics 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 -