Abstract

Depending of the laser operating parameters, several characteristic regimes of laser welding can be observed. At low welding speeds, the aspect ratio of the keyhole can be rather large with a rather vertical cylindrical shape, whereas at high welding speeds, low aspect ratios result, where only the keyhole front is mainly irradiated. For these different regimes, the dependence of the keyhole (KH) depth or the keyhole threshold, as a function of the operating parameters and material properties, is derived and their resulting scaling laws are surprisingly very similar. This approach allows us to analyze the keyhole behavior for these welding regimes, around their keyhole generation thresholds. Specific experiments confirm the occurrence and the behavior of these unstable keyholes for these conditions. Furthermore, recent experimental results can be analyzed using these approaches. Finally, this analysis allows us to define the aspect ratio range for the occurrence of this unstable behavior and to highlight the importance of laser absorptivity for this mechanism. Consequently, the use of a short wavelength laser for the reduction of these keyhole stability issues and the corresponding improvement of weld seam quality is emphasized.

Highlights

  • Laser welding has become an extremely widely used process in the industrial world because it allows the easy assembly of metal parts having a great range of thicknesses and with a very high productivity

  • Several issues addressed in this study concern the analysis of the KH behavior for different regimes of laser welding used in several industrial applications: These processes cover deep KHs with large aspect ratios obtained at low welding speeds with multi-kilowatt lasers, and those with much smaller aspect ratios, realized at high welding speeds, with small focal spots and lasers with low incident power

  • One important issue is about the determination of the scaling law of the resulting aspect ratios for these very different operating conditions

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Summary

Introduction

Laser welding has become an extremely widely used process in the industrial world because it allows the easy assembly of metal parts having a great range of thicknesses and with a very high productivity. All these processes operate in the so-called keyhole (KH) mode; i.e., the laser radiation penetrates the material to a depth at least greater than the focal spot. One must note that these conditions are met for example, in additive powder bed manufacturing processes [1,2]

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