Abstract
Connecting small pieces of parts manufactured by Selective Laser Melting (SLM) and traditional formed parts into large structural component by using welding technology provides a high-efficiency and low-cost way for expanding additive manufacturing technology. SLMed parts usually exhibit similar or superior tensile strength but lower ductility compared to that of cast or rolled ones due to the rapid cooling and cyclic heating deposition characteristics. What about the weldability of the dissimilar joints of SLMed parts and rolled ones? Whether the properties of the welded joints can be improved by heat treatment under the premise of ensuring the reliability of the joint is unclear. The weldability and the effect of heat treatment temperature on the microstructure and properties of laser-welded joints of SLM-316 L/rolled-316 L are studied in this article. The results show that the joints exhibit good weldability without obvious defects. The low temperature annealing treatment had no significant effect on the multilayered structure and columnar austenite grains, but only changed the morphology and content of ferrite within the grains leading to the slight increase of elongation but decrease of material strength. The corrosion performance was almost unaffected. After solution annealing above 1,000°C, the ferrite was nearly dissolved in the austenite matrix. The austenite recrystallized and the multilayered structure was destroyed, which resulted in decrease of material strength, a slightly improvement in corrosion resistance, and the elongation was greatly enhanced. After the detailed study, it was concluded that the post-weld heat treatment provided an effective way for improving the overall performance of the SLM-316 L/rolled-316 L dissimilar joint.
1 Introduction
Selective laser melting (SLM), as one of the most representative additive manufacturing technology, has great advantages in rapid and free manufacturing of 3D structure with the characteristics of good surface roughness and high geometric precision [1,2]. However, the restriction on the availability of large-scale SLM equipment, the control of defects and dimensional accuracy, and the residual stress associated with SLM complex thermal process limit the application of SLM on large-scale components [3,4]. Connecting small pieces of parts manufactured by SLM and traditional formed parts into large structural component by using welding technology provides available way for expanding additive manufacturing technology. On the one hand, high-efficiency, low-cost production is achieved. On the other hand, the residual stress in the manufacturing of large-scale parts can be relieved, and the quality and forming accuracy of the welded structure are controlled more easily.
However, dissimilar welded joints encountered many associated structural integrity problems such as differences in thermal expansion coefficient, carbon migration, mismatched mechanical property, and other discontinuities like environmentally assisted problems, formation of carbon-rich, and depleted zones [5–7]. Post-weld heat treatment (PWHT) is usually an effective measure to solve the above problems. Sirohi et al. [8] had investigated heat treatment on the mechanical performance of the GTA welded dissimilar joint of P91 and SS304H steel. After PWHT, an increase in the density of Mo and Nb-enriched particles were observed, and a soft pro-eutectoid ferrite and hard zone were formed near the interface due to the C and Cr diffusion. An increase in both tensile strength and % elongation was measured after the PWHT. Sirohi et al. [9] conducted systematic study on metallographic characterization and mechanical testing on dissimilar joint of the P91/SS304H steel using the Ni-based super alloy IN617 filler for as-welded (AW) and PWHT conditions. The PWHT showed a drastic reduction in residual stress value in a different zones of the weldments and lower impact energy of the weld metal.
PWHT is also adopted to solve some problems occurring in SLM process, such as sub-crystalline structure with high-density dislocation, epitaxial columnar crystals, accumulation of residual stress, and poor ductility of components due to the characteristic of layer-by-layer forming and non-equilibrium solidification of base materials during the SLM. In order to meet the requirements of the microstructure and mechanical properties of the formed parts, the corresponding post-heat treatment of SLM formed parts were carried out. Karabulut et al. [10] conducted several heat treatments on SLMed superalloy In718, and found that appropriate post-heat treatment can increase the toughness of the morphologic alloy. Yan et al. [11] used SLM technology instead of welding to connect Ti6Al4V and conducted post-heat treatment. The results showed that the post-heat treatment process significantly changed the mechanical properties of formed parts, because the post-heat treatment changed the width, length, and distribution of Pt phase that would affect the properties. Liu et al. [12] compared the microstructure evolution, hardness, and wear resistance properties of NiCrSiB + xY2O3 formed by SLM under three different heat treatment conditions (solid solution, solid solution aging, and annealing). It is found that carbide and brittle phase appear in solution and solution aging stage, and the grain is refined after annealing treatment, and the properties are further improved. Åsberg et al. [13] evaluated the microstructure and properties of the hot die steel H13 formed by SLM after direct tempering and quenching and tempering treatment, respectively. The results showed that the cell/dendrite morphology and local hardness uneven phenomenon caused by SLM forming were eliminated by post-heat treatment, and the hardness of the tempered sample was high enough without affecting the fracture toughness. Shin et al. [14] found that the microstructure stability and mechanical properties of SLM formed 316 LSS stainless steel changed after annealing at a certain temperature. When the annealing temperature reached 400°C, the yield strength increased by 10% and elongation decreased not significantly because of the thermal stability of the crystal cell/dislocation structure. However, when the annealing temperature is higher than 400°C, the microstructure thermal stability is destroyed and silicate dissolves, which leads to the strength reduction. The above provides a possibility for controlling the properties of laser additive manufacturings forming parts.
One the most significant issues to be considered for the austenitic stainless steel joints is to avoid chromium carbide formation in the grain and grain boundaries of the weld zone. The PWHT might be an advantage for eliminating carbide precipitates and improving the tensile strength of joints since it could regiment the microstructure especially at the weld zone [15]. Ghorbani et al. [16] investigated the effects of PWHT on the microstructure, mechanical properties, and corrosion properties of the welded joint. Heat treatment of the whole series of samples at 860°C and 960°C can eliminate chromides generated during welding and homogenize the microstructure. Jiang et al. [17] studied the microstructural, tensile strength, and hardness of tungsten inert gas-welded CLAM steel joints, subjected to PWHT at 740°C for 1 h. They conducted the mechanical and micro structural tests on the welded joints and the result showed that the mechanical properties of the CLAM steel welded joints can be improved by a reasonable PWHT. Li et al. [18] investigated the different PWHT to achieve a good combination of strength, toughness, and corrosion properties.
Welding method is also one of the key factors affecting the quality of dissimilar metal joints. The existing welding techniques like gas metal arc welding need the preheating, inter-pass heating that causes the distortion and localized softening of the weld metal [19]. To overcome such difficulties, radiant beam-welding processes like laser beam welding and electron beam welding have been suggested, which improves the welds’ quality and produces the weld joint with lesser distortion and narrow heat affected zone (HAZ) [20].
In this study, 316 L stainless steel rolled plates with 3 mm thickness were connected with SLMed ones by laser welding and the acquired butt joints were then subjected to low temperature annealing (LTA) at 400°C for 4 h and solution treatment (ST) at 1,050°C for 30 min. The study focused on the effect of varying heat treatments on homogeneity across the welded joint in terms of microstructural evolution, mechanical properties, and corrosion resistance of welded joints, which provides a theoretical basis for the performance improvement of components prepared by additive manufacturing.
2 Experimentation
The SLM experiments were conducted on the industrial-grade 3D printer EOS M290, which includes a continuous wave ytterbium-doped fiber laser (maximum output power of 400 W), an automatic powder feeding device, a 3D building platform, and a set of control system. The original material for SLM in this experiment was 316 L stainless steel powder, which was purchased from Jiangsu VILORY New Material Technology Co., Ltd, with the size in the range of 20–50 μm prepared by the vacuum induction smelting gas-atomized method. The chemical composition is shown in Table 1.
Chemical compositions of 316 L stainless steel powders (wt%)
C | Si | Mn | P | S | Ni | Cr | Mo |
---|---|---|---|---|---|---|---|
0–0.03 | 0–1.0 | 0–2.00 | 0–0.045 | 0–0.03 | 10–14 | 16–18 | 2–3 |
The gas-atomized spherical 316 L powders were then deposited layer-by-layer on a 316 L stainless steel substrate through the 3D printer in an argon environment with oxygen concentration controlled below 50 ppm. Cuboid samples with dimension of 65 mm × 30 mm × 25 mm were constructed for follow-on use. The as-built samples were cut from the substrate and annealed at 650°C for 2 h in a box furnace (KSX-8-1100G) to release the residual stress, and then sliced into thin plates with a dimension of 65 mm × 30 mm × 3 mm by wire-electrode cutting to be welded. The sliced plates were brushed to remove the oxide film on the surface by sanding treatment.
A 6 kW fiber laser (IPG YLS.6000.S2T) with a wave length of 1,070 nm was employed to join the SLM-316 L plates and rolled-316 L ones. During the welding process, the laser beam transmitted through a core fiber with a diameter of 200 μm and focused by a lens with a diameter of 310 mm to get a focused radius of 0.35 mm. The welding supporting facility was ABB six-axis robot, and the laser worked in a multi-mode and continuous output. The laser head was inclined 5° to vertical direction to avoid damage caused by the reflection of the laser beam. In this experiment, the shielding gas used was 99.99% argon flowing out of a paraxial copper gas nozzle. The applied welding parameters are shown in Table 2. Schematic diagram of welding between SLMed parts and rolled parts is shown in Figure 1.
Parameters of laser welding
Laser power (P) | Welding speed (ν) | Laser defocused distance (D) | Gas flow rate (Q) |
---|---|---|---|
2.8 kW | 30 mm·min−1 | 0 mm | 20 L·min−1 |

Schematic diagram of laser-welded joints’ preparation and the tensile samples.
The acquired joints were then subjected to LTA at 400°C for 4 h with subsequent water cooling and solution annealing at 1,050°C for 30 min with subsequent air cooling, respectively. The schematic used in Figure 2 shows the heat treatment processed on laser-welded joints of SLM-316 L/rolled-316 L.

Schematic showing the heat treatment performed on base metal and SLM-316 L/rolled-316 L joints.
Metallographic specimens were grinded and polished, and then etched by aqua regia for 10 s to observe the metallography. The macroscopic morphology and microscopic structure were characterized by optical microscope (HAL1000) and scanning electron microscopes (JSM-6480). The Veronese MH5 microhardness tester tested the microhardness of the joints in various locations. Due to the limited size of the sample made by SLM in this experiment, non-standard tensile samples were prepared by proportionally minifying standard ones according to PRC National Standard GB/T228.1-2010. The specific dimension of the welded joints was designed as illustrated in Figure 3. The loading direction of tensile test as well as the laser traveling direction is marked in Figure 1. Phase identification was performed on the laser-welded joints by XRD-6000 using a CuKα radiation with a step size of 0.02° and a dwell time of 1 s per step. The electrochemical tests of all the samples were conducted on a CorrTest EG&G PARC M283 electrochemical station in a three-electrode cell at ambient temperature. The platinum sheet and saturated calomel electrode were selected as auxiliary and reference electrodes, respectively. The samples with a size of 10 mm × 10 mm × 3 mm were kept in the 3.5 wt% NaCl solution for enough time to obtain potentiodynamic polarization curve. The potential range relative to OCP was from −0.5 to 1.5 V at a scanning rate of 0.5 mV·s−1.

Tensile sample.
3 Results and discussion
3.1 Effect of heat treatment on microstructure of welded joint
Table 3 lists the surface morphologies of laser-welded seam in front and back views and the cross-section of joints. As depicted in the images, both the surface and backside of the welds were smooth and uniform, and the microstructure of the weld consists of a large amount of coarse columnar dendrites. The cross-section morphologies of the welded joints exhibited the typical features of laser deep-penetration welding. Obvious convex was observed on the surface of the weld, which was mainly due to the reduction of density and increase of volume after the rolled/SLMed base metal underwent melting, cooling, and solidification to form weld without external pressure. In addition, the up-thrust of molten material due to the Marangoni flow was also an important factor of the convex [21,22]. The base metal, weld zone, and fusion zone were discriminated clearly without an apparent transition zone, but the HAZ was not obvious in the welded joints. The fusion line on the SLMed side of the weld was clearer than that on the rolled side. There were no conspicuous defects such as cracks, pores, and non-fusions observed in the welded joint, demonstrating that it is feasible to join SLMed parts with rolled ones to obtain reliable welds.
Surface morphologies of laser-welded seam in front and back views and the cross-section of joints
Surface morphologies | Cross-section | ||
---|---|---|---|
Weld | Front |
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Back |
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The macroscopic cross-section morphology of joint and the microstructure of each area before and after heat treatment are shown in Figure 4. Figure 4(a–c) are the original microscopic morphology of AW joint, the microstructure after annealing, and ST of Zone I, respectively. Figure 4(d–f) are the original microscopic morphology of AW joint, the microstructure after annealing, and ST of Zone II, respectively. Figure 4(g–i) are the original microscopic morphology of AW joint, the microstructure after annealing, and ST of Zone III, respectively. The microstructure of the SLMed parts is the end-result of metal powder melting and solidification, with adjacent neighboring tracks responsible for partial remelting of the solidified tracks. The morphology displayed compact structures without large holes or cracks, presenting a strong metallurgical bonding formed between melt-tracks. The overlap between adjacent melted tracks and layers was clearly observed from traces of the fusion line region. Periodic regular “fish scales” molten pools were distributed in the SLMed 316 L stainless steel, each of which had roughly the same size and morphology.

Microstructure of different areas of weld before and after heat treatment: (a–c) are the microstructure of Zone I, (d–f) are the microstructure of Zone II, (g–i) are microstructure of Zone III of AW joint, the microstructure after annealing treatment at 400°C for 4 h, and ST at 1,050°C for 30 min.
A clear fusion line between the weld and the SLMed base metal in Zone I was observed. The microstructure was composed of a layer of columnar dendrites densely arranged at the edge of the weld, which grew perpendicular to the fusion line along the direction of heat dissipation, and a small part of fine cellular crystals. This structure had been extended to the center of the weld.
On the rolled side (Zone II), there was a narrow less conspicuous semi-melting zone between the weld and the base metal instead of the fusion line. The microstructure was mainly dominated by extremely fine columnar crystals perpendicular to the semi-melting zone. Zone III was the center area of the weld. In Zone III, the microstructure on SLMed side was mixed with columnar dendrites and equiaxial crystals of different forms directed toward the center line. The weld on the forged side showed the characteristics of columnar dendrites on the whole, and the grain was much finer than that on the SLMed side. This made the weld appear to be divided into two almost symmetrical parts, which had great differences in microstructure. It is because the microstructure of SLMed parts was mainly in the form of dendrite or columnar crystal, which provided a good nucleation environment for grains. The undercooling degree of the dendrite tip increased with the growth rate. Therefore, in the direction approximately parallel to the interface, the growth rate and the undercooling degree was kept minimum. In this way, the growth of grains along the dendrite tip, that is, those perpendicular to the interface, exceeded that of dendrites with other orientations [23]. Therefore, the grains on the SLMed side of the weld were more favorable to generate and grow into coarse dendrites than that on the rolled side. Nucleation difficulty on the rolled side resulted in retention of heat in the molten pool, so the grains at the boundary of the base metal appeared semi-melted.
By comparison, it can be seen that the microstructure of the base metal part in the welded joint hardly changed, both the fusion line and the boundary of each micro-molten pool in the SLM forming plane were still clearly observed. Slight refinement of grains in the weld appeared after LTA. ST had a great influence on the microstructure of welded joint. Due to the growth of grains during ST, the original boundary of the micro-molten pool was destroyed and the sub-crystal structure interior were replaced by large grains with irregular shape. Some of the fine grains near the junction between the weld and the base metal crossed through the fusion line to combine into large grains during the growing process. It is worth noting that in the process of merging and growing, the grains in the weld still preferentially grew in the direction of the original grains, that is, perpendicular to the fusion line of the weld towards the center of the weld.
Figure 5 shows the X-ray diffraction (XRD) patterns of the AW joints and heat-treated samples. The crystal indices of AW joints corresponding to the peak were (111), (200), (220), and (311), exhibiting γ austenite (FCC) structure. After the heat treatment at 400°C for 2 h, the XRD patterns have no obvious change, indicating that low temperature heat treatment has no significant effect on the austenite columnar grains. The samples at 1,050°C for 30 min still mainly exhibit the austenite γ structure, but the diffraction peaks of (111) γ, (200) γ increased and the diffraction peaks of (220) γ, (311) γ, peaks decreased. Moreover, a new diffraction peak (222) appears. It indicates that some austenite grains recrystallize and the orientation changes after heat treatment at 1,050°C.

XRD diagrams of samples under different heat treatment conditions.
The elemental line mapping across the joints of AW sample and ST sample were also performed, as shown in Figure 6, and there was no obvious variation noticed for Cr, Ni, Mo, and Fe at both sides of the weld.

Line map of (a) AW joint and (b) ST joint.
Figure 7 is the SEM morphology of weld before and after heat treatment. The microstructure of AW joint was composed of γ matrix and δ phase distributed in dendritic pattern on the austenite matrix. The δ phase was the crystal nucleus of the primary δ ferrite left after the δ → γ transition. Due to short-range diffusion, the main element of ferrite Cr diffused from the austenite to the ferrite, in contrast, the dominant element of austenite Ni diffused and dispersed from the ferrite to the austenite [24], resulting in the Cr-poor and Ni-rich γ phase matrix and the Cr-rich and Ni-poor δ ferrite in the crystal. The sampling points of energy dispersive spectroscopy (EDS) analysis of the weld are shown in Figure 7(a), and the analysis results are listed in Table 4.

SEM morphology of weld before and after heat treatment: (a) AW joint, (b) after annealing treatment at 400°C for 4 h, and (c) after ST at 1,050°C for 30 min.
EDS analysis obtained from Figure 7 (wt%)
Spectrum | Phases | Cr | Ni | Fe | Mn | Mo | Si |
---|---|---|---|---|---|---|---|
1 | γ | 17.26 | 11.34 | 59.86 | 1.76 | 2.35 | 0.52 |
2 | δ | 22.7 | 6.53 | 53.69 | — | 6.79 | 1.27 |
The diffusion of carbon in δ phase was more rapid than that in γ phase, but the solubility of carbon in ferrite was lower than that in austenite. During the cooling process, carbon in δ phase was liable to be supersaturated, which promoted the precipitation and concentration of carbide M23C6 inside the δ phase. After the joint was annealing treated at400°C for 4 h, the ferrite chains was “cut” or “break”, and its morphology changed from “dendrite” to “island,” as shown in Figure 7(b). After the joint was solution treated at 1,050°C for 30 min, the volume fraction of the δ phase was further reduced, and the morphology acquired was wormlike. Usually, the δ phase could hinder the movement of dislocations and grain boundaries, which might affect recrystallization and hinder the twin nucleation and growth processes [24]. Therefore, after heat treatment at 1,050°C, recrystallization occurred preferentially and unstrained crystal nuclei grew by the movement of the high-angle interfaces, forming coarse grains containing many twin boundaries, as shown in Figure 4(i).
3.2 Effect of heat treatment on mechanical property of welded joint
Figure 8 shows the microhardness variation across the dissimilar welds joint. The average hardness of the rolled-316 L base metal was measured 168 ± 5 and 232 ± 4 HV for SLMed-316 L steel. The hardness of weld decreased gradually from the SLM side to the rolled side. The hardness survey clearly showed the non-uniform hardness profiles along the welded joint. The higher hardness of SLM side is the layer-by-layer deposition characteristics of additive manufacturing which decided that it underwent rapid cooling and cyclic heating, which resulted in lattice distortion leading to the increase of microhardness. According to the previous microstructure analysis, the brittle hard phase M23C6 precipitated from δ phase and distributed inside γ phase, which increased the microhardness of the material to some extent [24]. The low temper annealing treatment alleviated the lattice distortion of the material and caused the precipitates to dissolve into the matrix and distribute evenly, so that the microhardness of the material slightly decreased. After ST, a reduction in hardness of each zone of the welds joint was measured, which might be due to the evolution of the secondary phases at the inter-dendritic boundaries, the coarsening of the M23C6 precipitates, and the dissolution of hard δ phase into matrix [25].

Microhardness distribution of laser-welded joints.
Figure 9 shows the engineering stress–strain curves of the tensile samples of the as-built and heat-treated samples. The tensile strength measured of the AW joint was 630.4 MPa. After LTA, the tensile strength slightly changes, which was 643.6 MPa; after heat treatment at 1,050 C it decreased to 610.3 MPa. With the increase of heat treatment temperature, the yield strength gradually decreases. PWHT has little effect on tensile strength, but played a significant role in improving ductility of welded joints. The ductility measured of AW joint was 35%, and increased to 60% in the LTA condition, both of which was less than that measured in the ST condition (65%).

Tensile test results of heat-treated samples.
The macroscopic fracture morphology of the different joints and OM image showing the fracture path of the laser-welded joint are displayed in Figure 10. All the tensile specimens were fractured in the weld with obvious necking in the break. The tensile fracture of the laser-welded joints occurred along with the fusion zone closer to the rolled parts rather than the base metals. This area was the columnar grain boundary, which was the most fragile part of the joint. The fracture of the joint between 316L stainless steel SLMed and rolled parts was characterized by typical ductile failure.

The photos of tensile test samples after tensile tests and OM image showing fracture path of laser-welded joint.
The fracture tensile specimen is shown in Figure 11. There were many dimples at the fracture morphologies of all samples, indicating that the fracture modes belong to plastic fractures in general. The fracture surface showed the tear ridges, cleavage facets, dimples, and microvoids with different sizes. In the AW joint, some cleavage facets, tear ridges, and voids along with fine size dimples were observed at the fracture surface, indicating that the fracture mode was mainly ductile fracture accompanied with some brittle fracture. The cracks may propagate along the ferrite. In the ST sample, cleavage facets and voids remained absent on the fracture surface but the size of the brittle area was decreased obviously as compared to the fracture surface in the AW joint. However, the amount of brittle area was less in the ST ones. In the ST sample, dimples of different sizes and depth were observed at the fracture surface, as shown in Figure 11(d).

Fracture morphology of tensile specimen of: (a) AW joint, (b) enlarged detail of (a), (c) after LTA, and (d) after ST.
According to Hall–Petch formula [26]:
where
After LTA, the morphology of ferrite changed from the original skeleton or reticulated shape to granular or short rod-like shape and the fraction of the second phase decreased, so the yield and tensile strength decreased while the elongation increased slightly.
After heat treatment at 1,050°C, the ferrite was basically dissolved and the columnar austenite grains recrystallized, destroying the continuous grain boundaries along the building direction. The increase of grain size resulted in the decrease of dislocation density and grain coarsening; the tensile strength was significantly reduced after heat treatment at 1,050°C. There were discontinuous microcracks along the columnar grain boundaries. The microcracks consumed the slip activation energy and reduced the number of slip lines, which severely reduced the deformation degree and decreased the elongation of sample [31]. The microcracks decreased with the migration of grain boundaries, which increased the degree of deformation and improved the elongation sharply. Additionally, after heat treatment at 1,050°C, the grains recrystallized and the austenite columnar grains transformed into equiaxed annealing twin grains, which made the deformation more uniform and further greatly improved the elongation.
3.3 Effect of heat treatment on corrosion resistance of welded joint
Figure 12 shows the polarization curve of welded joints after heat treatment. The electrochemical parameters of partial corrosion of welded joints before and after heat treatment are detailed in Table 5. It is found that the pitting resistance of the welded joint after ST at 1,050°C for 30 min was the best, while the pitting resistance of the AW joint is the worst. Both the self-corrosion potential and the self-corrosion current density of welded joints have no obvious change after LTA, indicating that LTA has little effect on the corrosion tendency and corrosion resistance of welded joints. The phenomenon of slight change of the dimensional blunt current density, the significant decrease of the breakdown potential, and the significant shortening of the passivation interval indicated that the quality of the passivation film has increased, which made the long-term corrosion resistance of the joint improved.

Planar polarization curve of the sample in hot place.
Corrosion electrochemical parameters of welded joints
Sample | Corrosion potential (V) | Corrosion current density (A·cm−3) | Passive potential (V) | Passivity current density (A·cm−3) | Disruptive potential (V) |
---|---|---|---|---|---|
AW | −0.30 | 1.2 × 10−7 | −0.045 | 1.9 × 10−6 | 0.37 |
LTA | −0.31 | 1.28 × 10−7 | −0.042 | 3.2 × 10−6 | 0.18 |
ST | −0.257 | 5.00 × 10−8 | — | — | 0.41 |
Compared to the AW joints, heat treatment could effectively promote the dissolution of ferrite into austenitic matrix, and the fraction of δ ferrite decreased with the rise of the heat-treated temperature. The corrosion resistance of the heat-treated joints enhanced owing to the dissolution of more δ ferrite, the decreased Cr-depleted region, and the more compact passive film [32]. The secondary phases and element distribution play important roles in the corrosion resistance of laser-welded joints of SLM-316 L/rolled-316 L.
4 Conclusion
The weldability and the effect of post-heat treatment on the microstructure and mechanical properties of laser-welded joints of SLM-316 L/rolled-316 L were investigated in this study. The following conclusions have been drawn:
The obtained laser-welded joints of SLM-316 L/rolled-316 L were smooth and uniform without conspicuous defects such as cracks, pores, and non-fusions. The microstructure and the microhardness of joints showed obvious inhomogeneity. The joints had superior tensile strength but poor ductility compared with rolled-316 L metal.
The heat treatment temperature had a great influence on the microstructure evolution of laser-welded joints of SLM-316 L/rolled-316 L. Low temperature treatment had little influence on the microstructure, which desalinized granular or acicular ferrite morphology and eliminate the semi-melting zone. With the increase of temperature, the morphology of ferrite changed from the original skeleton or reticulated shape to granular shape. After ST, the ferrite was basically dissolved and the columnar austenite grains recrystallized, destroying the continuous grain boundaries and obvious grain coarsening was observed.
PWHT has little effect on tensile strength and corrosion resistance, but played a significant role in improving ductility of welded joints. The tensile strength of the AW joint was 630.4 MPa, which was 643.6 MPa after LTA, and 610.3 MPa after ST. The ductility of AW joint was 35%, and increased to 60% in the LTA condition, both of which was less than that measured in the ST condition (65%). After ST, the microhardness decreased slightly and the corrosion resistance had marginal improvement. A series of changes caused by PWHT, including the decrease of dislocation density, grain coarsening resulted by grain recrystallization, and the reduction of microcracks are the main factors for these performance variations of the joints.
Acknowledgments
The authors would also like to thank the support of the Analytical and Testing Center, JUST.
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Funding information: This work was supported financially by the National Natural Science Foundation of China (NSFC, No. 51705218), Natural Science Foundation of China (NSFC, No. 51905231), and High-Tech Ship Scientific Research Project from the Ministry of Industry and InformationTechnology (No. [2019]360).
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Author contributions: Hongwei Sun: conceptualization, investigation. Xiaopeng Lin: data curation, writing – original draft preparation. Xiaoyan Gu:resources, writing – review & editing, project administration, funding acquisition. Chenfu Fang: resources, validation, supervision. Zhidong Yang: resouces, visualization.
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Conflict of interest: Authors state no conflict of interest.
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Data availability statement: The data that support the findings of this study are available from the corresponding author upon reasonable request.
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© 2022 Hongwei Sun et al., published by De Gruyter
This work is licensed under the Creative Commons Attribution 4.0 International License.
Articles in the same Issue
- Research Articles
- Numerical and experimental research on solidification of T2 copper alloy during the twin-roll casting
- Discrete probability model-based method for recognition of multicomponent combustible gas explosion hazard sources
- Dephosphorization kinetics of high-P-containing reduced iron produced from oolitic hematite ore
- In-phase thermomechanical fatigue studies on P92 steel with different hold time
- Effect of the weld parameter strategy on mechanical properties of double-sided laser-welded 2195 Al–Li alloy joints with filler wire
- The precipitation behavior of second phase in high titanium microalloyed steels and its effect on microstructure and properties of steel
- Development of a huge hybrid 3D-printer based on fused deposition modeling (FDM) incorporated with computer numerical control (CNC) machining for industrial applications
- Effect of different welding procedures on microstructure and mechanical property of TA15 titanium alloy joint
- Single-source-precursor synthesis and characterization of SiAlC(O) ceramics from a hyperbranched polyaluminocarbosilane
- Carbothermal reduction of red mud for iron extraction and sodium removal
- Reduction swelling mechanism of hematite fluxed briquettes
- Effect of in situ observation of cooling rates on acicular ferrite nucleation
- Corrosion behavior of WC–Co coating by plasma transferred arc on EH40 steel in low-temperature
- Study on the thermodynamic stability and evolution of inclusions in Al–Ti deoxidized steel
- Application on oxidation behavior of metallic copper in fire investigation
- Microstructural study of concrete performance after exposure to elevated temperatures via considering C–S–H nanostructure changes
- Prediction model of interfacial heat transfer coefficient changing with time and ingot diameter
- Design, fabrication, and testing of CVI-SiC/SiC turbine blisk under different load spectrums at elevated temperature
- Promoting of metallurgical bonding by ultrasonic insert process in steel–aluminum bimetallic castings
- Pre-reduction of carbon-containing pellets of high chromium vanadium–titanium magnetite at different temperatures
- Optimization of alkali metals discharge performance of blast furnace slag and its extreme value model
- Smelting high purity 55SiCr automobile suspension spring steel with different refractories
- Investigation into the thermal stability of a novel hot-work die steel 5CrNiMoVNb
- Residual stress relaxation considering microstructure evolution in heat treatment of metallic thin-walled part
- Experiments of Ti6Al4V manufactured by low-speed wire cut electrical discharge machining and electrical parameters optimization
- Effect of chloride ion concentration on stress corrosion cracking and electrochemical corrosion of high manganese steel
- Prediction of oxygen-blowing volume in BOF steelmaking process based on BP neural network and incremental learning
- Effect of annealing temperature on the structure and properties of FeCoCrNiMo high-entropy alloy
- Study on physical properties of Al2O3-based slags used for the self-propagating high-temperature synthesis (SHS) – metallurgy method
- Low-temperature corrosion behavior of laser cladding metal-based alloy coatings on EH40 high-strength steel for icebreaker
- Study on thermodynamics and dynamics of top slag modification in O5 automobile sheets
- Structure optimization of continuous casting tundish with channel-type induction heating using mathematical modeling
- Microstructure and mechanical properties of NbC–Ni cermets prepared by microwave sintering
- Spider-based FOPID controller design for temperature control in aluminium extrusion process
- Prediction model of BOF end-point P and O contents based on PCA–GA–BP neural network
- Study on hydrogen-induced stress corrosion of 7N01-T4 aluminum alloy for railway vehicles
- Study on the effect of micro-shrinkage porosity on the ultra-low temperature toughness of ferritic ductile iron
- Characterization of surface decarburization and oxidation behavior of Cr–Mo cold heading steel
- Effect of post-weld heat treatment on the microstructure and mechanical properties of laser-welded joints of SLM-316 L/rolled-316 L
- An investigation on as-cast microstructure and homogenization of nickel base superalloy René 65
- Effect of multiple laser re-melting on microstructure and properties of Fe-based coating
- Experimental study on the preparation of ferrophosphorus alloy using dephosphorization furnace slag by carbothermic reduction
- Research on aging behavior and safe storage life prediction of modified double base propellant
- Evaluation of the calorific value of exothermic sleeve material by the adiabatic calorimeter
- Thermodynamic calculation of phase equilibria in the Al–Fe–Zn–O system
- Effect of rare earth Y on microstructure and texture of oriented silicon steel during hot rolling and cold rolling processes
- Effect of ambient temperature on the jet characteristics of a swirl oxygen lance with mixed injection of CO2 + O2
- Research on the optimisation of the temperature field distribution of a multi microwave source agent system based on group consistency
- The dynamic softening identification and constitutive equation establishment of Ti–6.5Al–2Sn–4Zr–4Mo–1W–0.2Si alloy with initial lamellar microstructure
- Experimental investigation on microstructural characterization and mechanical properties of plasma arc welded Inconel 617 plates
- Numerical simulation and experimental research on cracking mechanism of twin-roll strip casting
- A novel method to control stress distribution and machining-induced deformation for thin-walled metallic parts
- Review Article
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- Topical Issue on Science and Technology of Solar Energy
- Synthesis of alkaline-earth Zintl phosphides MZn2P2 (M = Ca, Sr, Ba) from Sn solutions
- Dynamics at crystal/melt interface during solidification of multicrystalline silicon
- Boron removal from silicon melt by gas blowing technique
- Removal of SiC and Si3N4 inclusions in solar cell Si scraps through slag refining
- Electrochemical production of silicon
- Electrical properties of zinc nitride and zinc tin nitride semiconductor thin films toward photovoltaic applications
- Special Issue on The 4th International Conference on Graphene and Novel Nanomaterials (GNN 2022)
- Effect of microstructure on tribocorrosion of FH36 low-temperature steels
Articles in the same Issue
- Research Articles
- Numerical and experimental research on solidification of T2 copper alloy during the twin-roll casting
- Discrete probability model-based method for recognition of multicomponent combustible gas explosion hazard sources
- Dephosphorization kinetics of high-P-containing reduced iron produced from oolitic hematite ore
- In-phase thermomechanical fatigue studies on P92 steel with different hold time
- Effect of the weld parameter strategy on mechanical properties of double-sided laser-welded 2195 Al–Li alloy joints with filler wire
- The precipitation behavior of second phase in high titanium microalloyed steels and its effect on microstructure and properties of steel
- Development of a huge hybrid 3D-printer based on fused deposition modeling (FDM) incorporated with computer numerical control (CNC) machining for industrial applications
- Effect of different welding procedures on microstructure and mechanical property of TA15 titanium alloy joint
- Single-source-precursor synthesis and characterization of SiAlC(O) ceramics from a hyperbranched polyaluminocarbosilane
- Carbothermal reduction of red mud for iron extraction and sodium removal
- Reduction swelling mechanism of hematite fluxed briquettes
- Effect of in situ observation of cooling rates on acicular ferrite nucleation
- Corrosion behavior of WC–Co coating by plasma transferred arc on EH40 steel in low-temperature
- Study on the thermodynamic stability and evolution of inclusions in Al–Ti deoxidized steel
- Application on oxidation behavior of metallic copper in fire investigation
- Microstructural study of concrete performance after exposure to elevated temperatures via considering C–S–H nanostructure changes
- Prediction model of interfacial heat transfer coefficient changing with time and ingot diameter
- Design, fabrication, and testing of CVI-SiC/SiC turbine blisk under different load spectrums at elevated temperature
- Promoting of metallurgical bonding by ultrasonic insert process in steel–aluminum bimetallic castings
- Pre-reduction of carbon-containing pellets of high chromium vanadium–titanium magnetite at different temperatures
- Optimization of alkali metals discharge performance of blast furnace slag and its extreme value model
- Smelting high purity 55SiCr automobile suspension spring steel with different refractories
- Investigation into the thermal stability of a novel hot-work die steel 5CrNiMoVNb
- Residual stress relaxation considering microstructure evolution in heat treatment of metallic thin-walled part
- Experiments of Ti6Al4V manufactured by low-speed wire cut electrical discharge machining and electrical parameters optimization
- Effect of chloride ion concentration on stress corrosion cracking and electrochemical corrosion of high manganese steel
- Prediction of oxygen-blowing volume in BOF steelmaking process based on BP neural network and incremental learning
- Effect of annealing temperature on the structure and properties of FeCoCrNiMo high-entropy alloy
- Study on physical properties of Al2O3-based slags used for the self-propagating high-temperature synthesis (SHS) – metallurgy method
- Low-temperature corrosion behavior of laser cladding metal-based alloy coatings on EH40 high-strength steel for icebreaker
- Study on thermodynamics and dynamics of top slag modification in O5 automobile sheets
- Structure optimization of continuous casting tundish with channel-type induction heating using mathematical modeling
- Microstructure and mechanical properties of NbC–Ni cermets prepared by microwave sintering
- Spider-based FOPID controller design for temperature control in aluminium extrusion process
- Prediction model of BOF end-point P and O contents based on PCA–GA–BP neural network
- Study on hydrogen-induced stress corrosion of 7N01-T4 aluminum alloy for railway vehicles
- Study on the effect of micro-shrinkage porosity on the ultra-low temperature toughness of ferritic ductile iron
- Characterization of surface decarburization and oxidation behavior of Cr–Mo cold heading steel
- Effect of post-weld heat treatment on the microstructure and mechanical properties of laser-welded joints of SLM-316 L/rolled-316 L
- An investigation on as-cast microstructure and homogenization of nickel base superalloy René 65
- Effect of multiple laser re-melting on microstructure and properties of Fe-based coating
- Experimental study on the preparation of ferrophosphorus alloy using dephosphorization furnace slag by carbothermic reduction
- Research on aging behavior and safe storage life prediction of modified double base propellant
- Evaluation of the calorific value of exothermic sleeve material by the adiabatic calorimeter
- Thermodynamic calculation of phase equilibria in the Al–Fe–Zn–O system
- Effect of rare earth Y on microstructure and texture of oriented silicon steel during hot rolling and cold rolling processes
- Effect of ambient temperature on the jet characteristics of a swirl oxygen lance with mixed injection of CO2 + O2
- Research on the optimisation of the temperature field distribution of a multi microwave source agent system based on group consistency
- The dynamic softening identification and constitutive equation establishment of Ti–6.5Al–2Sn–4Zr–4Mo–1W–0.2Si alloy with initial lamellar microstructure
- Experimental investigation on microstructural characterization and mechanical properties of plasma arc welded Inconel 617 plates
- Numerical simulation and experimental research on cracking mechanism of twin-roll strip casting
- A novel method to control stress distribution and machining-induced deformation for thin-walled metallic parts
- Review Article
- A study on deep reinforcement learning-based crane scheduling model for uncertainty tasks
- Topical Issue on Science and Technology of Solar Energy
- Synthesis of alkaline-earth Zintl phosphides MZn2P2 (M = Ca, Sr, Ba) from Sn solutions
- Dynamics at crystal/melt interface during solidification of multicrystalline silicon
- Boron removal from silicon melt by gas blowing technique
- Removal of SiC and Si3N4 inclusions in solar cell Si scraps through slag refining
- Electrochemical production of silicon
- Electrical properties of zinc nitride and zinc tin nitride semiconductor thin films toward photovoltaic applications
- Special Issue on The 4th International Conference on Graphene and Novel Nanomaterials (GNN 2022)
- Effect of microstructure on tribocorrosion of FH36 low-temperature steels