N. Sreenivasan Centre for Advanced Materials Joining, University of Waterloo, Waterloo, ON, N2K 4K8, Canada M. Xia Centre for Advanced Materials Joining, University of Waterloo, Waterloo, ON, N2K 4K8, Canada; Central Iron and Steel Research Institute, Beijing 100081, P.R.C. S. Lawson Y. Zhou Centre for Advanced Materials Joining, University of Waterloo, Waterloo, ON, N2K 4K8, Canada Effect of Laser Welding on Formability of DP980 steel Limiting dome height (LDH) tests were used to evaluate the formability of laser butt welded blanks of the dual phase 980 steel in comparison with the base metal. Two different lasers were used: diode and Nd:YAG, giving a wide range of welding thermal cycles. A sharp decrease in LDH was observed in the welded specimens due to the formation of a softened zone in the outer heat affected zone. Softened zone characteristics were correlated with the LDH. Larger softened zones led to a larger reduction in the LDH. The welding orientation relative to the rolling direction or to the punch surface did not influence the formability, as the softened zone dominated the formability behavior. It was observed that in both uniaxial and biaxial strain tests, the fracture occurred in the softened zone of the welded samples consistently slightly farther out from the weld cen- terline than in the location of the minimum hardness. DOI: 10.1115/1.2969246 Keywords: diode laser, Nd:YAG laser, formability, DP980 steel, softened HAZ 1 Introduction Currently, many new types of advanced high strength steels AHSSs, including dual phase DPsteels, are being produced by steel manufacturers that have higher strength and ductility, which contribute to weight reduction in the automotive industries. Most of the early weldability research on DP steels was focused on the resistance spot weld RSWtechnique 1,2. Recent re- search has dealt with laser welding of DP steels with focus on the process development and optimization of the laser welding pro- cess 3–5. Most commonly used lasers for welding are CO 2 and Nd:YAG 6–8; however, the high power diode laser HPDLhas also been confirmed to be well suited for welding of butt and lap-fillet joint geometries in the aluminum sheet for automotive applications as well as for butt welds in the steel 9–11. Formability aspects of these steels and tailor welded blanks TWBsare also of interest and have been studied. Numerous studies have confirmed that in formability experiments of TWB, strain is concentrated and fracture occurs in the thinner/weaker side of the blank 12–15. Further research has also suggested that the welding and rolling direction of the material may influence the formability 8,16. On the other hand, it is known that laser welds in AHSS are harder/stronger than the base metal 17, and the surrounding heat affected zone HAZcontains regions that may be harder or softer 17. Therefore, some significant effects of welding on formability would be expected. The softened HAZ phenomenon has been observed in DP steels with various welding processes such as arc, RSW, and laser 5. The softened HAZ in the arc and resistance welded DP steels had a significant influence on the formability 5. Laser welding cre- ated a narrower softened zone with higher laser power and weld- ing speed 6 kW, 7 m/min, in contrast to a wider softened zone created with lower power and speed 3 kW, 4 m/min18. An introductory study on the influence of welding phenomena on the formability of high strength low alloy HSLAand DP980 steels was conducted at the authors’ laboratory 19. It was found that formability was not affected by the laser welding process on the HSLA material, whereas a decrease in formability was ob- served on the DP980 steel. Uniaxial transverse tensile testing of DP980 also showed a sharp decrease in maximum strain after welding. Furthermore, the influence of softened outer HAZs of the welds of the DP980 steel on the formability was observed. This study focuses on the formability effects of the welds made with two different power density types of laser on the DP 980 steel, spanning a wide range of welding thermal cycles. The in- fluence of the softened zone on formability is examined. The ef- fect of the welding speed on fracture and softened zone distances from the weld centerline is studied. Furthermore, the relationship between uniaxial and biaxial strains is examined. 2 Experimental Procedures 2.1 Material. The DP 980 steel of 1.17 mm thickness with a coating described as galvannealed GA48–55 g / m 2 with about 10% Fe was used in this study. The chemical and mechanical properties are summarized in Tables 1 and 2. Since the full chemi- cal composition of the steel was considered proprietary, a sum- mary of the alloying is provided including carbon equivalent us- ing the well known Yurioka formula 20. This DP steel has a ferrite matrix with a significant volume fraction of fine martensite laths. 2.2 Laser Properties. Diode and Nd:YAG are the two lasers used in this work and their characteristics are shown in Table 3. The Nuvonyx 4 kW diode laser was mounted on the manipulator arm of a welding robot. Its laser beam is rectangular in shape, with dimensions 12 0.5 mm 2 at the focal point. The energy density/irradiance of the diode laser, which is less than 10 6 W / cm 2 , generates only a conduction mode of laser welding 21,22. Ultrahigh purity argon gas was supplied at a flow rate of 14 l/min as a shielding gas at the leading edge of the laser beam spot on the top surface side of the welds. Welds were conducted in the bead on a plate mode, i.e., a butt weld with full penetration on the blanks of uniform thickness and material. Welding was con- ducted on the blanks within the speed range of 0.7–1.9 m/min. The welding speed of less than 0.7 m/min led to excess weld size and sag; the speed above 1.9 m/min resulted in partial penetration. The Haas HL3006D Nd:YAG laser employed fiber optic beam delivery from a remote laser system to the final delivery optics without any inert gas shielding. The full power of 3 kW was used for the welding process. The energy density/irradiance of the Nd:YAG laser, which is higher than 10 6 W / cm 2 , generates a key- hole mode of laser welding 21,22. Operating speeds were used Contributed by the Materials Division of ASME for publication in the JOURNAL OF ENGINERING MATERIALS AND TECHNOLOGY. Manuscript received April 3, 2007; final manuscript received October 17, 2007; published online September 9, 2008. Assoc. Editor: Hamid Garmestani. Journal of Engineering Materials and Technology OCTOBER 2008, Vol. 130 / 041004-1 Copyright © 2008 by ASME Downloaded 27 Mar 2009 to 129.97.27.206. Redistribution subject to ASME license or copyright; see http://www.asme.org/terms/Terms_Use.cfm