A novel pressure-controlled joule-heat forge welding method to fabricate sound carbon steel joints below the A1 point
Graphical abstract
Introduction
Extensive efforts have been made to strengthen structural materials to improve the collision safety of transportation vehicles, and lower their weight to improve fuel efficiency [[1], [2], [3], [4]]. Since carbon steels can provide a good strength-ductility combination with low cost by carbon content increasing and appropriate microstructural tailoring, they are considered as promising structural materials for use in the automotive industries. However, for medium and high carbon steels, it is hard to obtain sound weld joints by conventional fusion welding methods due to the brittle martensitic transformation undergoing upon cooling from the high-temperature field (above the phase transformation point, A1) that may cause an occurrence of cracking in the weld zone, and other typical fusion-welding-associated issues, such as coarse columnar grains, high residual stresses, severe welding distortions and solidification voids/defects, which significantly deteriorate the joint qualities [[5], [6], [7]]. Solid-state joining techniques with a low welding temperature below the A1 point are, therefore, promising and strongly required to join medium and high carbon steels [8,9].
Rotary friction welding (RFW) is one of the solid-state joining techniques in which the friction heat is generated between the faying surfaces of two components to soften the interface materials, then they are plasticized out to the outer region as flashes to produce the joint. Since RFW allows a fast joining with a welding temperature much lower than that of the fusion welding, it has been extensively adopted to join carbon steels [[10], [11], [12], [13], [14]]. However, the large difference in peripheral velocities between the weld interface center and periphery induces an inhomogeneous heat generation over the weld interface, making the welding temperature and the associated interface microstructure also inhomogeneous and hard to control in the RFW [15,16].
In light of these issues, we propose a novel joining concept in which the electric resistance heat is utilized to soften the interface materials, then they are plasticized out as flashes by a high pressure to produce the joint. Since the electric resistance heat is utilized as the heat source rather than the rotary friction heat, the heat generation is expected to distribute homogeneously over the weld interface. Moreover, since a high pressure is applied, the interface materials can be deformed at a relatively low temperature, thus allowing the welding temperature possibly lower than the A1 point. This view has been well verified in our previous studies on linear friction welding (LFW) and RFW [[17], [18], [19]].
In this study, a novel welding apparatus was designed in-house for this novel joining method that we named “Pressure-controlled Joule-heat Forge Welding (PJFW)”. Medium carbon steel rods were joined by this method, and the effects of the processing parameters on microstructure and mechanical properties of the joints were systematically investigated in order to obtain a sound carbon steel joint below the A1 point.
Section snippets
Experimental procedures
Fig. 1 shows the image of the self-made welding apparatus, which is composed of a power supply (CHUO SEISAKUSHO HVS4E-160-103), an electric servo press (CORETEC FMS100-B), a control panel and a welding unit (both self-made) as magnified in the red dotted rectangle. The power supply is capable of supplying a current up to a maximum 10,000 A at a maximum voltage of 16 V. The electric servo press can provide a maximum load of 100 kN. The welding unit contains two cylindrical jigs having an outer
Thermal cycles
Fig. 5a shows the thermal cycles measured during the PJFW processes under the different currents of 3000 A, 4000 A, and 5000 A with the constant pressure of 250 MPa and constant burn-off length of 4 mm. The corresponding peak welding temperatures and temperature rising rates from 100 °C to 600 °C are also extracted in Fig. 5b for an intuitive view. All the welding processes were completed within a short time of several seconds. For all the conditions, the temperature increased to an almost
Conclusions
Based on these findings, it is summarized that the welding temperature can be uniquely determined by the applied pressure, and neither the current nor the burn-off length have obvious effects on the welding temperature during the PJFW of S45C. Since the electric resistance heat is utilized as the heat source, the uniform temperature and hence hardness distribution can be achieved over the entire weld interfaces. A sound S45C PJFW joint having the BM tensile properties with the absence of the
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
The authors wish to acknowledge the financial support by JST-Mirai Program Grant Number JPMJMI19E5, JSPS KAKENHI Grant Numbers JP19H00826 and JP20K05169, and an ISIJ Research Promotion Grant.
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