Ingenieurwissenschaften und zugeordnete Tätigkeiten
Filtern
Dokumenttyp
- Zeitschriftenartikel (5)
- Beitrag zu einem Tagungsband (1)
- Dissertation (1)
- Vortrag (1)
Schlagworte
- Solidification (8) (entfernen)
Organisationseinheit der BAM
- 9 Komponentensicherheit (8) (entfernen)
Eingeladener Vortrag
- nein (1)
Laser beam welding is a widely used joining technique in many industrial applications. This is mainly due to its many unique advantages, especially compared to conventional arc welding processes. These advantages include, among others, highly concentrated energy deposition, low total heat input and a capacity to penetrate deep into the material while causing only small welding distortions.
However, at the same time, the small dimension of the laser spot, high solidification rates, and small dimensions of the weld pool itself can provoke issues regarding the assembly tolerances of the workpiece, the hot-cracking phenomena, as well as keyhole-induced bubbles escaping from the melt.
Weld pool shapes in laser beam welding are elongated at the external, free surfaces under the action of the main driving forces in the melt – such as recoil pressure and surface tension forces – while being shorter in the internal areas of the weld pool. This leads to a regular solidification sequence from the internal zones toward the free surfaces, e.g. from the bottom to the top in partial penetration welding. However, in recent studies reported in the literature and seen in the experimental and numerical investigations of BAM Bundesanstalt für Materialforschung und -prüfung in Berlin, it was found that an internal narrowing phenomenon can occur that is often accompanied by a distinct bulging of the weld bead in deeper zones.
As the internal behaviour of the melt during the process is hardly optically accessible, several numerical models and experimental techniques were established to visualise the mechanisms of the formation of the bulging and the narrowing phenomenon and to reveal the consequences on the solidification sequence, pore formation, and filler metal dilution.
This study presents mechanisms of the evolution of a narrowed region in the weld pool center during deep penetration laser beam welding. In numerous numerical studies presented in this study, it was also found that the local reduction of the weld pool size can cause detrimental effects on the melt flow behavior and the resulting properties of the welds. A particularly large influence of this effect was identified in three aspects. Firstly, the local variation of the solidification sequence of the weld pool causes an increase in the hot-cracking susceptibility due to a locally delayed solidification. Secondly, it was proven that a change in the local length and width of the weld pool is associated with an adverse impact on the potential flow routes of the molten material that induces stronger local variations of its solidification. Thus, the element mixing, e.g. during the welding with filler materials, is blocked. This leads to a non-homogeneous chemical composition of the final weld and can cause undesired effects on the final material properties. Finally, another observed effect is related to the reduced ability of process pores to reach the top surface. As this type of porosity is usually produced around the keyhole tip, the change of the fluid flow regime above this area plays a significant role in determining the final path of the pores until the premature solidification in the middle of the weld pool captures them. This study summarizes mainly numerical results which were supported by selected experimental validation results.
This study presents mechanisms of the evolution of a narrowed region in the weld pool center during deep penetration laser beam welding. In numerous numerical studies presented in this study, it was also found that the local reduction of the weld pool size can cause detrimental effects on the melt flow behavior and the resulting properties of the welds. A particularly large influence of this effect was identified in three aspects. First, the local variation of the solidification sequence of the weld pool causes an increase in the hotcracking susceptibility due to a locally delayed solidification. Second, it was proven that a change in the local length and width of the weld pool is associated with an adverse impact on the potential flow routes of the molten material that induces stronger local variations of its solidification. Thus, the element mixing, e.g., during the welding with filler materials, is blocked. This leads to a nonhomogeneous chemical composition of the final weld and can cause undesired effects on the final material properties. Finally, another observed effect is related to the reduced ability of process pores to reach the top surface. As this type of porosity is usually produced around the keyhole tip, the change of the fluid flow regime above this area plays a significant role in determining the final path of the pores until the premature solidification in the middle of the weld pool captures them. This study summarizes mainly numerical results that were supported by selected experimental validation results.
This study presents mechanisms of the evolution of a narrowed region in the weld pool center during deep penetration laser beam welding. In numerous numerical studies presented in this study, it was also found that the local reduction of the weld pool size can cause detrimental effects on the melt flow behavior and the resulting properties of the welds. A particularly large influence of this effect was identified in three aspects. First, the local variation of the solidification sequence of the weld pool causes an increase in the hot-cracking susceptibility due to a locally delayed solidification. Second, it was proven that a change in the local length and width of the weld pool is associated with an adverse impact on the potential flow routes of the molten material that induces stronger local variations of its solidification. Thus, the element mixing, e.g., during the welding with filler materials, is blocked. This leads to a non-homogeneous chemical composition of the final weld and can cause undesired effects on the final material properties. Finally, another observed effect is related to the reduced ability of process pores to reach the top surface. As this type of porosity is usually produced around the keyhole tip, the change of the fluid flow regime above this area plays a significant role in determining the final path of the pores until the premature solidification in the middle of the weld pool captures them. This study summarizes mainly numerical results that were supported by selected experimental validation results.
Zur Prüfung der Erstarrungsrissanfälligkeit von Werkstoffen existiert eine Vielzahl von Prüfverfahren, die jedoch oft nur in ihren Grundzügen standardisiert sind. Ein Beispiel ist der an der Bundesanstalt für Materialforschung und -prüfung entwickelte und angewendete Modifizierte Varestraint-/Transvarestraint-Test (MVT), der eine von vielen Umsetzungen des Varestraint-Verfahrensprinzips darstellt. Hierbei werden durch Biegung während des Schweißens gezielt Erstarrungsrisse erzeugt und anschließend lichtmikroskopisch vermessen. Die Ergebnisse von Varestraint-Prüfungen charakterisieren jedoch nicht allein das Werkstoffverhalten, sondern sind in hohem Maße von der Konstruktion der jeweiligen Prüfmaschine sowie den verwendeten Prüfparametern abhängig. Dies erschwert die Vergleichbarkeit von Ergebnissen, welche nicht unter exakt identischen Bedingungen ermittelt wurden, und kann darüber hinaus zu einer ungenauen oder unvollständigen Bewertung des Werkstoffverhaltens führen.
Die vorliegende Arbeit widmet sich zunächst der detaillierten Ausgestaltung der geometrischen Zusammenhänge rund um die Ausbreitung von Erstarrungsrissen während der Varestraint-Prüfung. Mit Blick auf Prokhorovs Technological Strength Theory und die sich daraus ergebenden erstarrungsrisskritischen Temperaturen wird anschließend eruiert, wie aus den Anfangs- und Endkoordinaten der entstandenen Risse auf das charakteristische Erstarrungsrissverhalten geschlossen werden kann. Die daraus entwickelte Bewertung der Rissanfälligkeit
ist weitestgehend von den Prüfparametern und weiteren verfahrensspezifischen Einflüssen entkoppelt, wodurch eine deutlich bessere Übertragbarkeit der Ergebnisse gewährleistet ist. Zur Erprobung der neu entwickelten Bewertungsansätze wurden zunächst MVT-Prüfungen an mehreren hochlegierten, martensitischen Schweißzusatzwerkstoffen, sowie am Nickelbasiswerkstoff Alloy 602 CA durchgeführt. So konnten einerseits verschiedene Legierungen hinsichtlich ihres Erstarrungsrissverhaltens charakterisiert und Empfehlungen für die schweißtechnische Fertigung generiert werden. Zum anderen dienten die Proben zur vollständigen Konzipierung, Entwicklung und Validierung einer digitalen Auswertemethodik.
Die eigens programmierte Software ermöglicht die schnelle und praxisgerechte Auswertung von MVT-Proben, und implementiert dabei zusätzlich die zuvor entwickelten, prozessunabhängigen Bewertungsansätze. Als Ergebnis konnten kritische Dehnraten identifiziert werden,ab deren Überschreitung die betrachteten Werkstoffe unter den verwendeten Prüfbedingungen gesteigerte Erstarrungsrissanfälligkeiten aufweisen. So ergibt sich ein direkter Zusammenhang zwischen MVT-Prüfergebnissen und der Technological Strength Theory
von Prokhorov. Die Bewertung des Werkstoffverhaltens anhand der kritischen Dehnraten erwies sich gegenüber den üblicherweise betrachteten Gesamtrisslängen als deutlich zuverlässiger.
Zusammenfassend konnte gezeigt werden, dass die digitale Auswertung eine sinnvolle Verbesserung der analogen Standardauswertung darstellt.
The geometrical characteristics of the weld end crater are commonly used as a means of validating numerical results in welding simulations.
In this paper, an analytical model is developed for calculating the cooling stage of the welding process after the moving energy source is turned off. Solutions for various combinations of heat sources and heated bodies are found. It is shown that after turning off the Energy source, additional melting of the base material in the longitudinal direction may occur due to the overheated liquid metal. The developed technique is applied to complete-penetration keyhole laser beam welding of 2 mm thick austenitic stainless-steel plate 316L at a Welding speed of 20 mm/s and a laser power of 2.3 kW. The results show a theoretical increase in the weld end crater length of up to 19% compared to the length of the steady-state weld pool. It is found that at the moment of switch off, the weld end crater center, where solidification of the liquid metal ends, is shifted from the heat source axis toward the weld pool tail. The solidification rate and the direction of crystallization of the molten material during the welding process and those in the weld end crater differ significantly. A good agreement between the computational results and the welding experiments is achieved.
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.
The shape of the weld pool in laser beam welding plays a major role to understand the dynamics of the melt and its solidification behavior. The aim of the present work was its experimental and numerical investigation. To visualize the geometry of the melt pool in the longitudinal section a butt joint configuration of 15 mm thick structural steel and transparent quartz glass was used. The weld pool shape was recorded by means of a high-speed video camera and two thermal imaging MWIR and VIS cameras. The observations show that the dimensions of the weld pool vary depending on the depth. The regions close to the surface form a teardrop shaped weld pool. A bulge-region and its temporal evolution were observed approximately in the middle of the depth of the weld pool. Additionally, a transient numerical simulation was performed until reaching a steady state to obtain the weld pool shape and to understand the formation mechanism of the observed bulging phenomena. A fixed keyhole with an experimentally obtained shape was used to represent the full-penetration laser beam welding process. The model considers the local temperature field, the effects of phase transition, thermo-capillary convection, natural convection and temperature-dependent material properties up to evaporation temperature. It was found that the Marangoni convection and the movement of the laser heat source are the dominant factors for the formation of the bulging-region. Good correlation between the numerically calculated and the experimentally observed weld bead shapes and the time-temperature curves on the upper and bottom surface were found.