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 - Artinov, Antoni A1 - Karkhin, Victor A1 - Bachmann, Marcel A1 - Khomich, Pavel A1 - Rethmeier, Michael T1 - МОДЕЛИРОВАНИЕ ГИДРОДИНАМИЧЕСКИХ И ТЕПЛОВЫХ ПРОЦЕССОВ ПРИ ЛАЗЕРНОЙ СВАРКЕ СО СКВОЗНЫМ ПРОПЛАВЛЕНИЕМ N2 - Разработана модель физических процессов при сварке плавлением на основе концепции эквивалентных источников теплоты. Модель включает в себя две части: термогидродинамику сварочной ванны и теплопроводность свариваемого тела вне ванны. В задаче термогидродинамики учитываются температурные зависимости свойств материала, форма парогазового канала, термокапиллярная и естественная конвекция, фазовые превращения и другие физические явления.Приведено решение задачи термогидродинамики методом конечных элементов на примере сварки стальной пластины толщиной 15 мм со сквозным проплавлением лазерным лучом (по технологии "замочная скважина"). Показано, что термокапиллярная конвекция жидкого металла является основной причиной сложной выпукло-вогнутой формы границы ванны с увеличенными размерами в приповерхностных областях. Получено удовлетворительное совпадение расчетных и экспериментальных размеров сварочной ванны. KW - ЛАЗЕРНАЯ СВАРКА KW - СВАРОЧНАЯ ВАННА KW - ЧИСЛЕННОЕ МОДЕЛИРОВАНИЕ KW - ГИДРОДИНАМИКА KW - КОНВЕКЦИЯ KW - ТЕПЛОПРОВОДНОСТЬ KW - ТЕМПЕРАТУРНОЕ ПОЛЕ KW - МЕТОД КОНЕЧНЫХ ЭЛЕМЕНТОВ PY - 2020 SN - 0491-6441 SP - 58 EP - 69 AN - OPUS4-50290 LA - rus AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - CONF A1 - Artinov, Antoni A1 - Bachmann, Marcel A1 - Karkhin, Victor A1 - Rethmeier, Michael ED - Sommertisch, C. ED - Enzinger, N. ED - Mayr, P. T1 - A novel approach for calculating the thermal cycle of a laser beam welding process using a stationary CFD model N2 - This work aims to find the thermal cycles during and after fusion welding through simulation by first calculating the resulting local temperature field in the quasi-stationary part of the process. Here complete-penetration keyhole laser beam welding with a laser power of 18 kW on a 15 mm thick slab of a low-alloyed steel at a welding speed of 2 m/min is considered. In order to physically depict the laser material interaction a multi-physics numerical model including the effects of phase transformation, thermo-capillary convection, natural convection and temperature-dependent material properties up to evaporation temperature is developed. It uses a fixed keyhole geometry with a right truncated circular cone shape to introduce the laser beam energy to the workpiece. In a subsequent study, the resulting local temperature field is then used as an equivalent heat source in order to predict the unsteady thermal cycle during and after fusion welding. The translational movement of the laser beam through the workpiece is represented by a moving mesh approach. For the simulation, stationary heat transfer and fluid dynamics are described by a system of strongly coupled partial differential equations. These are solved with the commercial finite element software COMSOL Multiphysics 5.0. The results of the numerical simulation are validated by experiments, where the weld bead shapes and the thermal cycles show good correlation. T2 - 12th International Seminar "Numerical Analysis of Weldability" CY - Graz, Austria DA - 24.09.2018 KW - Equivalent heat source KW - Process simulation KW - Laser beam welding KW - Transient heat transfer KW - Moving mesh PY - 2019 SN - 978-3-85125-616-1 VL - 12 SP - Chapt. VI, 694 EP - 710 PB - Verlag der Technischen Universität Graz AN - OPUS4-48817 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - CONF A1 - Karkhin, Victor A1 - Artinov, Antoni A1 - Khomich, P. A1 - Bachmann, Marcel A1 - Rethmeier, Michael T1 - Modelling of welding thermal cycles by boundary element method N2 - A numerical model for simulation of the steady-state thermal behaviour in keyhole mode welding has been developed. It is based on the equivalent heat source concept and consists of two parts: computational thermo-hydrodynamics and heat conduction. The solution of the thermo-hydrodynamics problem by the finite element method for a bounded domain results in a weld pool interface geometry being the input data for a subsequent heat conduction problem solved for a workpiece by a proposed boundary element method. The main physical phenomena, such as keyhole shape, thermo-capillary and natural convection and temperature-dependent material properties are taken into consideration. The developed technique is applied to complete-penetration keyhole laser beam welding of a 15 mm thick low-alloyed steel plate at a welding speed of 33 mm/s and a laser power of 18 kW. The fluid flow of the molten metal has a strong influence on the weld pool geometry. The thermo-capillary convection is responsible for an increase of the weld pool size near the plate surfaces and a bulge formation near the plate middle plane. The evaluated and experimental molten pool, cross-sectional weld dimensions and thermal cycles of the heat affected zone are in close agreement. T2 - Trends in Joining, BTU Cottbus CY - Cottbus, Germany DA - 14.11.2018 KW - Keyhole welding KW - Computational fluid dynamics KW - Boundary element method KW - Thermal cycles PY - 2018 AN - OPUS4-46606 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Karkhin, Victor A1 - Artinov, Antoni A1 - Bachmann, Marcel A1 - Rethmeier, Michael T1 - Simulation of solidification during laser welding of thin plates T1 - Моделирование процесса кристаллизации при лазерной сварке пластин малой толщины N2 - It is proposed to model the experimentally observed weld pool boundary with superellipses (Lamé curves) and to find the unknown parameters of the curves using optimization methods. It has been shown experimentally that during laser welding of austenitic stainless steel with a thickness of 2 mm at a speed of 20 mm/s, the rear weld pool part has a shape close to triangular which can be accurately approximated by a superellipse. Analytical dependences of the trajectory and growth rate of the crystal and its cross-sectional area on the geometry of the rear weld pool part are obtained. KW - Laser beam welding KW - Plane crystalization KW - Mathematical modeling KW - Superellipse KW - Thin steel plates PY - 2023 U6 - https://doi.org/10.34641/SP.2023.1061.4.033 VL - 4 SP - 28 EP - 33 AN - OPUS4-59649 LA - rus AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Artinov, Antoni A1 - Karkhin, Victor A1 - Bachmann, Marcel A1 - Rethmeier, Michael T1 - Simulation of solidification during keyhole laser welding of thick plates T1 - Моделирование процесса кристаллизациипри лазерной сварке со сквозным проплавлением пластин большой толщины N2 - A method of solving the thermo-fluid dynamics problem is presented, enabling the prediction of the shape and dimensions of the weld pool during keyhole laser welding of thick plates. It is shown that the rear weld pool boundary can be satisfactorily approximated by a set of superellipses (Lamé curves). The presence of a convex rear weld pool boundary in the mid-plane has been observed experimentally and reproduced numerically. It was shown that in this zone the concentration of liquating impurities increases and the local solidification temperature decreases, contributing to the susceptibility to hot cracking. KW - Laser beam welding KW - Three-dimensional crystallization KW - Mathematical modeling KW - Superellipse KW - Thick steel plates PY - 2024 U6 - https://doi.org/10.34641/SP.2023.1062.5.041 VL - 5 SP - 31 EP - 36 AN - OPUS4-59639 LA - rus AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER -