3.1 Stability and accuracy of process
In this paper, six different EP/EN ratios were used in the deposition process to understand their effects on the stability of WAAM process, as listed in Table 1, ranging from 4/16 to 19/1. Figure 2 showed the surface morphology of as-fabricated materials deposited in single-layer and single-pass, and at different EP/EN ratios. Evidently, discontinuous deposition was only observed at the lowest EP/EN ratio of 4/16. With the increase of EP/EN ratio, e.g., from 7/13 to 7/13, discontinuity of the deposited materials disappeared and corrugated fish-scale patterns dominated. With further increase of EP/EN ratio to around 19/1, i.e., significantly higher EP CMT cycles with substantially higher heat input, corrugated fish-scale patterns faded away due to improved wettability. Furthermore, it shall be noted that increasing EP/EN ratio led to significant reduction of voids and spatters during the deposition process. These results indicated that the electrical signals and droplet transfer of the above deposition process needed to be investigated.
Table 1
A list of EP/EN ratios applied in the deposition processes with wire feeding rate 6 m/min and traveling speed 0.6 m/s.
Test number | Case 1 | Case 2 | Case 3 | Case 4 | Case 5 | Case6 |
EP/EN ratio | 4/16 | 7/13 | 10/10 | 13/7 | 16/4 | 19/1 |
Figure 3 showed the current/voltage waveforms of the VP-CMT process and the corresponding high speed camera recordings of arc/metal transfer at different EP/EN ratios. EN CMT cycles were characterized as a “cold” process, which had a lower heat input than that of the EP CMT cycles. With the decrease in EN CMT cycles, EN CMT cycles started to dominate the processing time. When the EP/EN ratio was 4/16, i.e., the process has the most EN CMT cycles, the wettability of the molten pool was deteriorated due to …, which contributed to the formation of higher liquid position. In the meantime, the molten pool with poor wettability cannot be spread to below the wire, resulting in difficulties direct transfer of droplets to the molten pool. Instead droplets moved to the unmelted substrate in wait phase, which prolonged the wait phase duration (Fig. 3a). The same phenomenon was observed in State 2, in which both the distance of wire feeding and wait phase duration in the first EP CMT cycle increased. With the prolonged current holding period, droplets grew to be oversized. and an additional projected droplet appeared in Fig. 3a before the normal short-circuiting transfer due to its large mass.
When the EP/EN ratio increased to 7:13, abnormal electric waveforms and metal transfer behavior deteriorated the process stability in Fig. 3b. As compared with the metal transfer behaviors in Case 1, the droplet in Case 2 was more likely to touch the molten pool instead of the unmelted substrate in shorting-circuit (SC) phase due to the more EP CMT cycles and higher heat input. The characteristics of electric waveforms and metal transfer behavior in Case 2 were: (1) A short SC phase duration appeared in Stage 3, as shown in Fig. 3b. The droplet grew in the wait phase and tended to move from opposite to along the travelling direction. When the droplet touched the molten pool, the SC phase started. Then the droplet continued to swing along the travelling direction, which caused a quick separation between the welding wire and molten pool and resulted in a short SC phase. (2) In Stage 4, due to the large viscosity of the molten pool, the separation between the wire and molten pool was hard to proceed at the last section of the SC phase. As a result, prolonged SC phase duration and several large spatters appeared in Fig. 3b.
To evaluate the forming accuracy of WAAM samples with different EP/EN ratios, the standard deviations of the contour lines in the stable part of the samples were measured. The standard deviation (S) was calculated as:
where n represents the number of coordinate points on the sample contour lines. yi and yj are the coordinate value and average coordinate value of the contour lines, respectively.
Figure 4 shows the macroscopic morphologies and statistical results of WAAM samples’ cross-sections under different EP/EN ratios. The average S first went down and then up with the increasing EP/EN ratio, and it had the minimum value of 0.141 when the EP/EN ratio was set as 13:7, which indicated optimal forming accuracy. The reasons for this phenomenon were: (1) The CMT advance mode had the characteristic of low heat input, dilution and high contact angle, especially in the condition with a low EP/EN ratio. Hence, the bead-shaped deposition appearance appeared in Fig. 4a, which significantly deteriorated the forming accuracy. (2) When the EP/EN ratio was higher than 13:7, the average S shows an upward tendency. The excessive heat input was achieved with a high EP/EN ratio, which strengthened the surface tension gradient of the molten pool and Marangoni convection. This strong convection induced the overflow phenomenon of the molten pool, which had a negative effect on the forming accuracy.
Meanwhile, when the EP/EN ratio was higher than 13:7, the stable current/voltage waveforms and deposition process occurred. As a result, the optimal forming accuracy with a stable deposition process was achieved when the EP/EN ratio was 13:7.
3.2 Microstructure
Figure 5 shows OM images of deposited samples under different Cases. Three special regions were focused in Fig. 5a, ie, top region, inter-layer region ,and inner layer region .The grain type was all distinguished as equiaxed grains in top and inner-layer regions as s the EP/EN ratio ranging from 4:16 to 19:1, while the grain size exhibited a growing trend. The high EP/EN ratio indicated more EP cycles and higher heat input, prolonging the duration of the liquid molten pool. Hence, the grains in the top and inner-layer regions with higher EP/EN ratios had a longer time to grow and coarsen. Additionally, the grain morphology in inter-layer region exhibited the characteristics of various grain types under different Cases. Firstly, when the droplet just touched the molten pool, the large undercooling was induced due to the highest temperature gradient. This large undercooling was conducive to the formation of pony-size equiaxed grains in the remelting zone. Then the columnar grains presented epitaxial growth at the transition region between the inter-layer region and inner-layer region. The temperature gradient decreased as the development of the columnar grain growth. Hence, the heat dissipation n and the grain growth directions turned to be random, which contributed to the transition from inter-layer region to inner-layer region. Meanwhile, with the increase of EP/EN ratio, the proportion of columnar grains in transition region decreased, while the proportion of pony-size equiaxed grains in remelting region increased. A combination of columnar grains and pony-size equiaxed grains appeared with an EP/EN ratio ranging from 4:16 to 10:10, and the columnar grains were almost missing with a higher EP/EN ratio (≥ 13:7). When the elevated EP/EN ratio were employed, the remelted area of deposited samples expanded and the temperature gradient of molten pool increased, thereby promoting the formation of equiaxed grains.
To further investigate the grain morphology and orientation of the CMT advanced-based WAAM Al-Zn-Mg-Cu alloy, the EBSD analysis of Case 4 also carried out, as illustrated in Fig. 6 regions. A located at the last deposition, where was free of remelting process. Region B was extracted from the stable area of the deposited samples. Figure 6a and c shows the inverse pole figures (IPFs) results of Regions A and B.The pony-size equiaxed grains, columnar grains, and coarse equiaxed grains occurred alternately along the building direction, which was consistent with the results of OM observation. The < 001 > orientation (red region), < 101 > orientation (green region), and < 101 > orientation (green region) in Regions A and B exhibited a uniform distribution, indicating a weak grain orientation. As a response, the values of the maximum multiples of uniform density (MUD) of Regions A and B were very low (2.07 and 1.62), according to the pole figures (IPF) results in in Fig. 6b and d. There are two reasons accounting for the low MUD values and weak grain orientation: (1) the CMT advance mode used in the WAAM process was characterized by the alternate transformation of EP and EN CMT periods, This rapid polarity change induced a stirring effect on the molten pool, contributing to the formation of a more random grain growth direction. As a result, the grain orientation became weak; (2) This strong turbulence in molten pool was conducive to break the dendrite and form more nucleation sites, thereby realizing the grain refinement. The average grain size of Regions A and B were only 48.36 µm and 51.31 µm, respectively.. The fine grains had a weaker grain orientation compared with that of columnar grains. Hence, the low MUD values and weak grain orientation of deposited sample were achieved by the CMT advanced-based WAAM process.
Al-Zn-Mg-Cu alloy is considered as a typical precipitation-strengthened aluminium alloy. and the precipitated phases play a crucial role in the mechanical property response, The coarse precipitated phases were generated massively during the deposition process, which distributed along the grain boundary and in the grain interior. as illustrated in Fig. 7. Meanwhile, the Zn, Mg, Cu alloy elements were enriched in these precipitated phases based on the map scanning results, which indicated that they may be the η Mg(Al, Zn, Cu) phases.., These coarse precipitated phases were easy to be the origin region of crack and harmful to the improvement of mechanical properties [17].
To identify the special type of these precipitated phases, the SEM images and corresponding EDS results were presented in Fig. 8. It was shown that the morphologies of the second phases varied little under different EP/EN ratios. Figure 8a and b shows low magnification backscattered electron (BSE) images of Cases 1 and 6. These net-shaped precipitated phases were continuously distributed along grain boundaries, forming a complex network. Meanwhile, many lamellar-shaped, net-shaped, cell-shaped, line-shaped and rod-shaped precipitated phases were mainly generated in the grain interior, as shown in Fig. 8c-f. To determine the chemical composition, EDS analysis was conducted on nine points within these precipitated phases. and the results are listed in Table 2. The majority of them contained a high content of Al, Zn, Mg, and Cu, indicating maybe they are η(Mg(Zn, Cu, Al)2)phases. The phase η in Al-Zn-Mg-Cu alloy was generally indicated as MgZn2, and the Zn atom was easy to be replaced by the Cu and Al atoms without changing the lattice structure [18], forming this solid solution Mg(Zn, Cu, Al)2 phases. Interestingly, the grey second phases (P3, P5, P9) had special grey values compared with other precipitated phases. Based on the EDS analysis, they were Fe-riched phases. The line scanning was also performed in Fig. 8i, the similar result indicated that the grey second phases may be Al7Cu2Fe. This Fe-riched phases with a high melting point were hard to be dissolved into the Al matrix [19], which were easy to be the initiation of the crack propagation [20].
What is more, the nano-scale precipitated phases were observed in the grain interior of bottom regions of WAAM samples (Cases 4 and 5), as shown in Fig. 8g and h. Instead, it almost disappeared in the top and middle regions of WAAM samples with the SEM analysis. Compared with the top and middle regions, the bottom regions of WAAM samples experienced the most reheating process, which could be regarded as a transient aging treatment, inducing the formation of more nano-scale precipitated phases.
Table 2
Chemical composition of second phases (wt%).
Position | Al | Zn | Mg | Cu | Fe | Possible phase |
P1 | Bal. | 17.2 | 7.5 | 14.9 | -- | Mg(Zn, Cu, Al)2 |
P2 | Bal. | 24.7 | 11.9 | 19.8 | -- | Mg(Zn, Cu, Al)2 |
P3 | Bal. | 4.6 | 1.3 | 5 | 14.9 | Al7Cu2Fe |
P4 | Bal. | 20.4 | 10.9 | 14.8 | 0.1 | Mg(Zn, Cu, Al)2 |
P5 | Bal. | 5.3 | 1.6 | 5.8 | 15.4 | Al7Cu2Fe |
P6 | Bal. | 13.8 | 5.9 | 8.2 | -- | Mg(Zn, Cu, Al)2 |
P7 | Bal. | 17.2 | 8.1 | 14.2 | 0.1 | Mg(Zn, Cu, Al)2 |
P8 | Bal. | 17.7 | 8.5 | 14.4 | 0.1 | Mg(Zn, Cu, Al)2 |
P9 | Bal. | 4.5 | 1.4 | 6.7 | 19.6 | Al7Cu2Fe |
3.3 Mechanical properties
Figure 9 shows the microhardness distribution and statistical results of deposited samples under different EP/EN ratios. The micro hardness values of all samples were ~ 130 HV0.2, while it was slightly lower in Case 6 (EP/EN ratio = 19:1) due to the formation of the coarser grains. The micro hardness distribution of all samples had an apparent fluctuation along the building direction without a significant spike, which was unlike the results (first increased and then decreased) of samples in Ref. [20, 21]. Firstly, more was formed in this study due to its higher deposition speed (0.6 m/min) compared with that (0.1 and 0.15 m/min) in Ref. [20, 21]. The Zn element had a low melting point, which caused the evaporation of Zn elements and formation of Zn pores during the WAAM process. Hence, The WAAM of Al-Zn-Mg-Cu was easier to produce the pores than other series aluminium, especially under this high deposition speed (0.6 m/min) in this study. The appearance of more pore defects contributed to this fluctuant characteristic of micro hardness distribution. Secondly, Dong et al. and Qie et al. [20, 21] considered nano-scale precipitated phases difference led to the micro hardness distribution of WAAM Al-Zn-Mg-Cu alloy first increased and then decreased along the building direction. Instead, in this paper, the micro hardness specimens were treated by a long-time natural aging, which eliminated the difference in density and size of nano-scale precipitated phases along the building direction. In addition, as mentioned in Section 3.3, the pony-size equiaxed grains, columnar grains, and coarse equiaxed grains occurred alternately along the building direction, which also caused this fluctuant micro hardness distribution. As a result, the appearance of pores and the grain morphology difference contributed to this fluctuant micro hardness distribution. In our next step, the deposition speed and its matched wire feeding rate need to be further investigated to reduce the pore defect.
Additionally, the standard deviation of the Micronesian distribution first decreased and then increased as a whole as the EP/EN ratio increased from 4:16 to 19:1, as shown in Fig. 9. The minimum value was 4.67 when the EP/EN ratio was 13:7. The less EP CMT cycles and heat input were achieved with a low EP/EN ratio, which meant that the solidification rate of Cases 1 and 2 were higher than other Cases. The time for pore escape was less, inducing the formation of more pore defects. When the high EP/EN ratio (Cases 5 and 6) was used, the area and duration of the molten pool was increased, and the grains coarsening phenomenon appeared. Meanwhile, the equal gas flow rate was used in all Cases, the expanded molten pool increased the possibility of gas entering the molten pool. Hence, the number of pore defects was increased more under conditions of low or high EP/EN ratio, which caused the occurrence of high standard deviation of the microhardness distribution.