Laser-MIG-process for automotive industry

Industrial Robot

ISSN: 0143-991x

Article publication date: 1 February 2004

283

Keywords

Citation

(2004), "Laser-MIG-process for automotive industry", Industrial Robot, Vol. 31 No. 1. https://doi.org/10.1108/ir.2004.04931aaf.006

Publisher

:

Emerald Group Publishing Limited

Copyright © 2004, Emerald Group Publishing Limited


Laser-MIG-process for automotive industry

Laser-MIG-process for automotive industry

Keywords: Laser welding, MIG, Welding, Automotive industry

1. Introduction

It has been known how to combine laser light and the arc into an amalgamated welding process ever since the 1970s, but for a long time thereafter, no further development work was undertaken. Recently, researchers have turned their attention to this topic again and attempted to unite the advantages of the arc with those of the laser, in a hybrid weld process. Whereas in the early days, laser sources still had to prove their suitability for industrial use, nowadays they are standard technological equipment in many manufacturing enterprises.

The combination of laser welding with another weld process is referred to as a “hybrid welding process”. This means that a laser beam and an arc act simultaneously in one welding zone, and influence and support one another.

2. Laser

Laser welding requires not only high laser power, but also a high-quality beam to obtain the desired “deep-weld effect”. The resulting higher quality of beam can be exploited either to obtain a smaller focus diameter or a larger focal distance.

For the development projects that are currently underway, a lamp-pumped solid-state laser with a laser beam power of 4 kW is being used. The laser light is transmitted via a 600 mm glass fibre.

The laser light is transmitted via a glass fibre, in which the beginning and the end are water-cooled. The laser beam is projected onto the workpiece by a focussing module with a focal distance of 200 mm.

3. Laser-MIG process

For welding metallic workpieces, the Nd:YAG laser beam is focussed at intensities of above 106 W/cm2. When the laser beam hits the surface of the material, it heats up this spot to vaporization temperature, and a vapour cavity is formed in the weld metal due to the escaping metal vapour. The distinguishing feature of the weld seam is its high depth-to-width ratio. The energy-flow density of the freely burning arc is slightly above 104W/cm2. Figure 3 shows the basic principle of hybrid welding. The laser beam depicted here feeds heat to the weld metal in the top part of the seam, in addition to the heat from the arc. Unlike a sequential configuration where two separate weld processes act in succession, hybrid welding may be viewed as a combination of both weld processes acting simultaneously in one and the same process zone. Depending on which arc or laser process is used, and on the process parameters, the processes will influence one another to a different extent and in different ways (Cui, 1991; Dausinger, 1995).

Figure 3 Schematic representation of Laser-MIG welding

Owing to the combination of the laser and arc processes, there is also an increase in both the weld penetration depth and the welding speed (as compared to either of the processes used on its own). The metal vapour escaping from the vapour cavity retro-acts upon the arc plasma. Absorption of the Nd:YAG laser radiation in the processing plasma remains negligible. Depending on what ratio of the two power inputs is chosen, the character of the overall process may be determined to a greater or smaller degree either by the laser or the arc (Maier et al., 1995; Steen et al., 1978).

Absorption of the laser radiation is substantially influenced by the temperature of the workpiece surface. Before the laser welding process can get underway, the initial reflectance must first be overcome, especially on aluminium surfaces. This can be achieved by starting welding with a special start program. After the vapourisation temperature has been reached, the vapour cavity is formed, with the result that nearly all the radiation energy can be input into the workpiece. The energy required for this is thus determined by the temperature-dependent absorption and by the amount of energy lost by conduction into the rest of the workpiece. In Laser-MIG welding, vaporisation takes place not only from the surface of the workpiece, but also from the filler wire, meaning that there is more metal vapour available, which in turn facilitates the input of the laser radiation. This also prevents process dropout.

4. Automotive application

By using space frame technology, a weight reduction of 43 per cent is possible in comparison to a steel car body.

Figure 4 Audi Space frame A2 concept

The Audi A2 Space frame consists of 30 m laser Figure 4 and 20 m MIG weld length. Additionally, 1,700 rivets are also used (Figure 5).

Figure 5 Comparison of profiles and joining techniques on the Audi-A2

Figure 6 shows a Laser-MIG welded joint of a ALMg3 cast material with a AlMgSi sheet material. The filler wire is AlSi5 and the shielding gas used is argon. With increasing laser power, deeper penetration is possible. Combining the laser beam with the arc in this way achieves a larger weld pool than with the laser beam weld process on its own. This makes it possible to weld components with wider gaps.

Figure 6 Overlap joint with a gap of 0.5 mm

In the automotive industry, there are many applications of overlap welding without joint preparation. At the moment, the state-of-the-art process for this welding job is the laser welding process with a cold filler wire, due to hot cracking of the AA 6xxx alloy. When the joint is welded with a filler wire, lot of the laser energy will be lost to melt that filler wire.

Figure 7 Comparison between Laser-MIG and laser without filler wire

Figure 7 shows the differences between Laser-MIG and laser welding on an overlap joint with a welding speed of 2.4 m/min. In the case of laser welding, there is no possibility to fill up the weld bead, and undercut is produced. Also, there is only a very small penetration into the base material. The weld bead width is very small, and therefore a low tensile strength will be expected. In the case of Laser-MIG welding, additional material is transported into the weld pool. The undercut is filled with the wire from the MIG process, and a portion of laser energy is saved. This saved laser energy can be used to increase the penetration into the base material and the weld bead width is larger than the material thickness, which is required from the numerical simulation.

With the Laser-MIG welding procedure, it is possible to weld materials of aluminium, steels and stainless steels of up to 4 mm material thickness. If the thickness is too high, full penetration is not possible. For joining zinc- coated materials, it is also preferable to use the laser brazing process.

Further applications in the automotive are power trains, axles and car bodies, where the laser hybrid welding process can be suitable.

4.1 Welding head

The welding head should have small geometrical dimensions, so as to ensure good accessibility to the components to be welded, especially in the auto-body field. Moreover, it should be designed to permit both a suitable detachable connection to the robot head and adjustability of such process variables as focal distance, and torch stand-off distances in all Cartesian co-ordinates. Plate 5 shows the welding head, while the process is in action. The spattering that occurs during the welding process leads to increasing soiling of the protective glass. The quartz glass is coated on both sides with an antireflective material and is intended to protect the laser optical system from damage.

Depending on the degree of soiling, the spatter accumulating on the glass can cause the laser power actually impacting upon the workpiece to decrease by as much as 90 per cent. Heavier soiling generally leads to the destruction of the protective glass, as such a large proportion of the radiant energy is then absorbed by the glass itself, causing thermal stresses in the glass.

5. Advantages of Laser-MIG welding

The following advantages result from the merging of arc and laser beam.

  1. 1.

    Advantages of Laser-MIG welding over laser welding

    • higher process stability;

    • higher bridgeability;

    • deeper penetration;

    • lower capital investment costs; and

    • greater ductility.

  2. 2.

    Advantages of Laser-MIG welding over MIG welding

    • higher welding speeds;

    • deeper penetration at higher welding speeds;

    • lower thermal input;

    • higher tensile strength; and

    • narrower weld-seams.

The arc welding process is characterized by a low-cost energy source, good bridgeability and by the facility for influencing the structure by adding filler metals. The distinguishing features of the laser beam process, on the other hand, are the great welding depth, high welding speed, low thermal load and narrow weld-seams that it achieves. Above a certain beam density, the laser beam produces a “deep-weld effect” in metallic materials which enables components with greater wall thicknesses to be welded – provided that the laser power is sufficiently high. Laser- MIG welding thus makes for higher welding speeds, process stabilisation due to the interaction between the arc and the laser beam, increased thermal efficiency and greater workpiece tolerances. Because the weld pool is smaller than that in the MIG process, there is less thermal input and thus a smaller heat- affected zone. This means less weldment distortion, which reduces the amount of subsequent post-weld straightening work that needs to be done.

Where there are two separate weld pools, the subsequent thermal input from the arc means that the laser beam – welded area – especially in the case of steel – is given a post-weld tempering treatment, spreading the hardness values more evenly across the seam. Figure 8 sums up the advantages of the combined (i.e. hybrid) process.

Plate 5 Welding head and process

Turning to the economic advantages of hybrid welding over laser welding, the following statements can be made. The weld seam consists partly of a laser weld and partly of a MIG weld. The hybrid process makes it possible to reduce the power of the laser beam, meaning that the energy consumption of the laser source can be greatly decreased, as the laser beam apparatus has an efficiency of only 3 per cent. In other words: a reduction of 1 kW in the laser beam power impacting upon the workpiece leads to a reduction of approximately 35 kVA in the power consumed from the electricity mains.

Figure 8 Advantages of combining the two processes

A laser beam apparatus costs around EUR 0.1 million for each 1 kW of laser beam power. To take just one example, in a case where the utilisation of the hybrid process makes it possible to use a 2 kW laser beam apparatus instead of one with 4 kW of beam power, this results in savings of EUR 0.2 million in investment outlays. However, it must be remembered here that for the hybrid process, a MIG machine costing around EUR 20,000 will be needed.

Owing to the higher welding speed, both the fabrication times and the welding costs can be reduced.

6. Summary

Laser-MIG welding is a wholly new technology that offers synergies for wide fields of application in metalworking industries, especially where it is not possible or financially viable to achieve the component tolerances that are required for laserbeam welding. The much wider range of application and the high capability of the combined process lead to enhanced competitiveness in terms of reduced investment outlays, shorter fabrication times, lower manufacturing costs and higher productivity.

The Laser-MIG process also offers a new approach to the welding of aluminium. However, a stable process that can be used in practice has only become possible relatively recently, owing to the higher available output powers of solid-state lasers. Numerous studies have examined the fundamentals of laser-arc- hybrid welding processes. By “hybrid welding process”, we mean the combination of laser beam welding and the arc welding processes, with only one single process zone (plasma and melt). Basic research studies (Beyer, 1997; Faißt et al., 1999; Helten, 1999; Schweißen mit Festkorörperlasern, 1995; Steen, 1996) have shown that a process is possible in which – by combining the two processes – synergies can be achieved and the drawbacks of each separate process can be compensated for, resulting in enhanced welding possibilities, weldability and welding reliability for many different materials and constructions. In particular, this has been demonstrated for aluminium alloys. By choosing favourable process parameters, it is possible to selectively influence weld properties such as geometry and structural constitution. The arc welding process increases the bridgeability by adding filler metal; it also determines the weld-seam width and thus reduces the amount of workpiece preparation that is needed. Moreover, the interactions taking place between the processes lead to a substantial increase in the efficiency of the process. This combination process also requires considerably smaller investment costs than does the laser welding process.

References

Beyer, E. (1997), Schweißen mit Laser: Grundlagen, Springer- Verlag, Berlin.

Cui, H. (1991), “Untersuchung der Wechselwirkungen zwischen Schweißlichtbogen und fokussiertem Laserstrahl und der Anwendungsmöglichkeiten kombinierter Laser-Lichtbogentechnik”, Dissertation, TU Braunschweig.

Dausinger, F. (1995), “Hohe Prozeßsicherheit beim Aluminiumschweißen mit Nd: YAG-Lasem”, Bleche und Profile, Vol. 42 No. 9, pp. S544-547.

Faißt, F., Weick, J.M., Fitz, R. and Kem, M. (1999), “Anwendungen der Twinfokus-Technik”, Stuttgarter Lasertage, pp. S50-52.

Helten, S. (1999), “Qualifizierung und Implementierung des lichbogenunterstützten Lasersrahlschweißverfahrens in den Fertigungsprozeß im Aluminiumkarosserieleicht  bau”, Diplomarbeit Audi, RWTH (ISF) Aachen.

Maier, C., Beersiek, J. and Neuenhahn, K. (1995), “Kombiniertes Lichtbogen-Laserstrahl- Schweißverfahren-On-line-Prozeßüberwachung”, Vol. DVS 170, pp. S45-51.

Schweißen mit Festkörperlasern (1995), Laser in der Materialbearbeitung, Band 2, VDI-Verlag, Dusseldorf.

Steen (1996), Laser Material Processing, Springer-Verlag, Berlin.

Steen et al., (1978), “Arc-augmented laser welding”, 4th Int. Conf. on Advances in Welding Processes, Paper No. 17, pp. 257-65.

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