3.1 Optimized design of the air circulation filtration system in a metal 3D printer
3.1.1 Establishment of a fluid model
We applied the parametric modeling software Rhino to design the forming cavity of the metal 3D printers. First, we designed the parts of the forming cavity, such as the shell, powder brush, guide groove and inlet guide plate, and then, we assembled them using Autodesk Inventor Professional software to completely model the forming cavity, as shown in Fig. 3(a). The designed cavity model of the 3D printer was imported into the moldflow simulation software Autodesk Simulation CFD. In the CFD software, first, the edge merge command was applied to reduce the number of edges in the model, and then, the inlet and outlet ends of the forming cavity were closed using the creation face command to generate the inlet of the fluid area: Velocity-inlet, outlet Pressure-outlet and others: Wall, as shown in Fig. 3(b). The wall material was defined as 316L stainless steel, and the physical property of the liquid flow was defined as nitrogen (viscosity 1.78e− 5 Pa·s, density 1.25 kg/m3). The maximum flow rate of the fan inlet and exhaust used in the SLM molding equipment was 1.30 m3/min. Owing to flow loss at the inlet end of the forming cavity, we set the flow velocity at the inlet end of the curved guide plate to 7,500 mm/s, and the pressure at the outlet end as 0 Pa. Automatic meshing was adopted.
3.1.2 Flow-state analysis of the forming cavity
Usually, when the fluid enters through the lower entrance of the forming cavity, the higher the flow rate, the lower the pressure and the smaller the turbulence distribution range. Additionally, the turbulence intensity is within the range of the wind speed, so that powder is not blown, which is beneficial to the discharge of the splashing particles and “solid smog” when the laser acts on the powder. The upper inlet of the forming cavity should be adjusted to avoid polluting the protective glass of the galvo scanner; consequently, the turbulence distribution range and intensity should be as small as possible when the fluid enters the forming cavity through the upper inlet. Additionally, a sufficient flow rate should be maintained to prevent splashing particles and “solid smog” from approaching the protective glass. On the basis of this analysis, the flow rate, pressure and turbulence distribution of the fluid flowing through the forming cavity were determined to be the main factors affecting the quality of the gas circulation filtration systems in metal 3D printers. Thus, it was necessary to simulate and analyze the state of the fluid flowing through the forming cavities of metal 3D printers, comprehensively evaluate the advantages and disadvantages of the performances and determine an optimization strategy.
3.1.3 Flow-field analysis of the current forming cavity
Figure 4 shows a flow-field distribution diagram of the fluid flowing through the forming cavity. In Fig. 4(a), the flow velocity distribution of nitrogen at the lower end of the forming cavity is shown. The current forming cavity had good connectivity and a high flow velocity at the outlet end. It had a measured flow velocity of 52.35 × 103 mm/s and a volume flow rate of 10.65 × 104 mm3/s. At the upper end of the powder cylinder, the layers of fluid flow interfered with each other, and the distribution was relatively disordered. The turbulent flow severely interfered with the laminar flow at the upper end of the forming cylinder, and the flowing vacuum zones on the left side and bottom end of the powder brush, as well as the end of the guide groove, were not conducive to fluid flow. This seriously affected the ability of the guide groove to discharge splashing particles and “solid smog”, and it easily led to defects in the formed parts. In Fig. 4(d), the flow velocity distribution of nitrogen entering the forming cavity from the upper inlet end is shown. The severe local gas backflow at the upper inlet interfered with fluid inflow, and thus, turbulence occurred, which caused “solid smog” that adhered to the protective glass of the galvo scanner, thereby weakening the ability of the laser to pass through and even resulting in damage to the laser. In Fig. 4(b) and (e), the pressure distribution of nitrogen flowing through the forming cavity is shown. The pressure was evenly distributed in the forming cavity, and the pressure at the inlet end was at a maximum, up to 9,672.84 Pa. The pressure near the outlet end of the forming cavity presented a negative gradient relationship, indicating that the air did not flow smoothly and that the static pressure was not evenly distributed. Under such conditions, local air backflow may easily occur. In Fig. 4(c), the turbulence distribution of nitrogen entering the forming cavity from the lower inlet end is shown. The maximum turbulent kinetic energy of the forming cavity was mainly concentrated at the end of the guide groove, as well as the left and the rear ends of the powder brush, and this resulted in flow field disorder in the forming cavity and powder contamination owing to poor air discharge. In Fig. 4(f), the turbulence distribution of nitrogen entering the forming cavity from the upper inlet end is shown. The turbulence was mainly concentrated at the inlet end, and no obvious turbulence was found at other locations. By determining the reasons for the above phenomena that, we concluded that the optimal design of the guide groove may be related to the improper structure of the upper and lower inlet ends, which provided an important basis for the structural optimization of the inlet end of the forming cavity. Using the flow-field distribution analysis results of nitrogen flowing through the original forming cavity used in the SLM molding equipment, we optimized the flow-field distribution by adjusting the structures of the upper and lower inlet ends of the forming cavity, including setting the guide plate.
3.1.4 Optimized structural design of the air inlet end of the forming cavity
In accordance with fluid mechanics and a forming cavity performance-related factor analysis, turbulence was determined to be the main factor affecting the internal performance of the forming cavity. To reduce powder contamination and to avoid pollution on the protective glass of the galvo scanner from “solid smog”, the turbulent flow of air from the circular hole into the forming cavity must be changed to a laminar flow. This was achieved as follows: the air inlet end structure of the forming cavity was adjusted from a circular hole to the guide plate form, and a multi-layer layout was applied. Then, the part of the guide plate near the inlet end was smoothed. Here, we developed two optimization plans. In Design 1, the upper inlet end of the forming cavity was designed with two-layered curved guide plates, and the design parameters included a thickness of 1.18 mm, 0.2-mm (radius) chamfer at the tail, total length of 15.95 mm, and upper and lower intervals of 5.09 mm. The inlet mode of the lower inlet end remained unchanged, as shown in Fig. 5(b). In Design 2, the upper inlet end mode of the forming cavity was the same as in Design 1. The lower inlet end of the forming cavity was designed with two-layered curved guide plates, and the design parameters included a thickness of 1.0 mm, 0.2-mm (radius) chamfer at the tail, total length of 12.95 mm, and upper and lower intervals of 4.28 mm. To avoid powder blowing, the bottom interval was set to 5.5 mm, and the fixing frame of upper and lower guide plates of the molding cavity was chamfered at 0.2 mm to the side of the forming cavity to reduce turbulence, as shown in Fig. 5(c). In the above two design plans, the guide plates are two layered to avoid blowing the powder to form dust owing to the local airflow being too strong inside the forming cavity. For a comparative analysis, we established the original structural model of the outlet end of the air intake pipe of a 3D printer, as shown in Fig. 5(a).
3.1.5 Flow-field analysis of the forming cavity of a metal 3D printer (Optimized Design 1)
In Fig. 6, the flow-field distribution of the fluid flowing through the forming cavity is shown. In Fig. 6(a), the flow velocity distribution of nitrogen at the lower end of the forming cavity is shown. The fluid had good connectivity in the forming cavity and a high flow velocity at the outlet end, with a measured flow velocity of 53.05 × 103 mm/s and a volume flow rate of 14.01 × 104 mm3/s. Both the flow velocity and volume flow rate were slightly higher than before optimization, suggesting that the waste gas was easier to discharge from inside of the forming cavity, which is conducive to air purification in the forming cavity. Judging from the flow state of nitrogen in the forming cavity, there was still mutual interference between the fluid-flow layers at the upper end of the powder cylinder, but the distribution area decreased. The vacuum area with flow appeared on the left side and the bottom end of the powder brush, as well as the end of the guide groove, which was similar to without the guide plate and had a certain influence on the discharge of solid smog in the forming cavity. In Fig. 6(d), the flow velocity distribution of nitrogen entering the forming cavity from the upper inlet end is shown. The upper fluid in the forming cavity flowed in layers and there was no interference between them after adding the guide plate. Thus, an “isolation zone” of “solid smog” and flying particles at the lower end of the galvo formed, which eliminated contaminants adhering to the surface of the protective glass of the galvo and ensured that the laser passed through the protective glass smoothly. In Fig. 6(b) and (e), the pressure distribution of nitrogen flowing through the forming cavity is shown. The pressure was evenly distributed in the forming cavity, and the pressure at the inlet end was at a maximum, up to 9,188.76 Pa. The pressure decreased compared with no guide plate, demonstrating that the air flowed smoothly. In Fig. 6(c), the turbulence distribution of nitrogen entering the forming cavity from the lower inlet end is shown. The distribution of turbulent kinetic energy in the current forming cavity was similar to that in the original forming cavity, and no significant change was found. In Fig. 6(f), the turbulence distribution of nitrogen entering the forming cavity from the upper inlet end is shown. The turbulence was mainly concentrated at both ends of the inlet, and no obvious turbulence was found at other locations. In addition, the distribution area was smaller and the intensity was much less than those of the orbital forming cavity, indicating that the fluid distribution in the forming cavity was effectively improved by changing the guide plate from circular hole to sheet shape. In general, the fluid distribution in the forming cavity was obviously improved using Design 1, but there were still some defects. For example, the turbulence at the lower end of the forming cavity and the turbulence at both ends of the upper inlet of the forming cavity were still large. The large turbulence distribution intensity levels and areas at the above two locations may be caused by differences in the flow velocities at the inlet of the upper and lower ends of the forming cavity and the absence of a chamfer at both ends of the guide plate. Thus, we further optimized the inlet mode of the forming cavity on the basis of these two points.
3.1.6 Flow-field analysis of the forming cavity of a metal 3D printer (Optimized Design 2)
In Fig. 7, the flow-field distribution of the fluid flowing through the forming cavity is shown. In Fig. 7(a), the flow velocity distribution of nitrogen at the lower end of the forming cavity is shown. The forming cavity had good connectivity and there was a high flow velocity at the outlet end after adding the guide plate, with a measured flow velocity of 53.08 × 103 mm/s and a volume flow rate of 19.74 × 104 mm3/s. Both the flow velocity and volume flow rate are higher than those without a guide plate added, suggesting that the waste gas was easier to discharge from the inside of the forming cavity, which was conducive to air purification in the forming cavity. The distribution and optimization plans were similar to those of Design 1, but the distribution area decreased significantly. The vacuum area with flow only appeared on the left side of the powder brush, which indicated that adding the guide plate was beneficial to the discharge of solid smog in the forming cavity. In Fig. 7(d), the flow velocity distribution of nitrogen entering the forming cavity from the upper inlet end is shown. The distribution of the flow field was similar to that of Design 1. In Fig. 7(b) and (e), the pressure distribution of nitrogen flowing through the forming cavity is shown. The pressure was evenly distributed in the forming cavity, and the pressure at the inlet end was at a maximum, up to 9,206.75 Pa, which was consistent with Design 1. In Fig. 7(c), the turbulence distribution of nitrogen entering the forming cavity from the lower inlet end is shown. The distribution of turbulent kinetic energy in the current forming cavity was similar to that in the original forming cavity, and the turbulence appeared on the left side of the powder brush and at the outlet of the guide groove. Both the distribution area and size decreased compared with Design 1. In Fig. 7(f), the turbulence distribution of nitrogen entering the forming cavity from the upper inlet end is shown. The turbulence mainly concentrated at both ends of the inlet, and no obvious turbulence was found at other locations. After chamfering the guide plate holder, both the distribution area and intensity significantly decreased compared with Design 1. In general, the fluid distribution in the forming cavity was obviously improved by adding the guide plate at the upper and lower inlets of the forming cavity, which contributed to the discharge of “solid smog” and avoided polluting the protective glass of the galvo scanner.
3.2 The technology and matching of 3D printed curved guide plates
3.2.1 Research on the technology of 3D printed curved guide plates
Different placements and support addition methods during the 3D printing of parts will lead to different amounts of support additions and forming layer thicknesses of parts, which directly influences form quality and the forming efficiency of parts. When using FDM technology to manufacture curved guide plates, the holder and the substrate are placed in parallel to improve the processing efficiency. Considering the large machining section, the preheating temperature of the substrate and the addition of 25% supports can be appropriately increased to reduce the stress concentration and avoid buckling deformations. When using SLM technology to shape the curved guide plate, previous studies on the placement and support addition mode of SLM formed parts have revealed that the plane of the guide plate holder should be inclined to the machining datum plane by 55° to avoid a large machining section, reduce stress concentration and add multiple holders (Zhang et al. [19]). Moreover, to further understand the machining risks of curved guide plates, we analyzed the machining risks using Magics software [Fig. 8 (a)]. According to Fig. 8(a), the machining risks of SLM-based curved guide plates mainly appeared in the low and top ends of the guide plate holder, whereas machining risks were not detected at other locations. Thus, the machining requirements were met. We added a line support to the curved guide plate completed after the machining risk analysis, and the support addition results are shown in Fig. 8(b). According to Fig. 8(b), the support addition for the curved guide plate mainly focused on the non-critical parts in which the support was easy to remove, and the amount of support addition was small. Additionally, the level of powder waste was small. These conform to the support addition principles of SLM-formed parts. Furthermore, based on previous experience, the scanning line of a cross-section of the SLM-formed guide plate should be long and the height of the parts should be high. Furthermore, the stress accumulation was serious, and the contractility was large, which may lead to buckling deformations. We added some mixed supports (conical and linear supports) at the bottom of the guide plate holder to enhance the binding force between the guide plate holder and the datum plate, as shown in Fig. 8(b).
3.2.2 Matching 3D printed curved guide plates
The curved guide plate formed by FDM is shown in Fig. 9(a). The overall morphology of the curved guide plate formed by FDM had a high surface smoothness and a clear structure, without obvious buckling deformations or forming defects. After a surface treatment, the curved guide plate was placed into a GYD 150 metal 3D printer to test matching, and it was found that the curved guide plate formed by FDM closely matched the inlet end of the air duct of the 3D printer and the screw fixing hole was in a proper position, meeting the assembly requirements. These provide the basis for the 3D printing of metal curved guide plates. The curved guide plate formed by SLM is shown in Fig. 9(b). The overall morphology of the curved guide plate showed a bright surface and good metal texture, and the structural frames were well connected, without obvious buckling deformations or forming defects. However, adhering slags with clear directivity appeared at the lower end of the guide plate holder. The quantity of adhering slags was not great. After treatment, the use was not affected. The reason for adhering slags may be related to the plane of the guide plate holder being inclined 55° relative to the machining datum plane. The surface roughness of the curved guide plate formed by SLM was tested, and the surface roughness was 11 µm. After abrasive blasting and polishing, it was 3 µm, meeting the use requirements. After a surface treatment, the curved guide plate was placed in a GYD 150 metal 3D printer to test matching, and the curved guide plate closely matched the inlet end of the air duct of the 3D printer. The upper guide plate was fixed at a proper position using screws, and the lower guide plate was fixed and closely matched using the sticking method to avoid clogging the air inlet with “solid smoke” and splashing particles. This indicated that the matching performance of the designed curved guide plate satisfied the use requirements.
3.3 Performance tests of 3D printed curved guide plates
The composition testing of parts formed by the curved guide plate having different structures at the inlet end of the SLM equipment are shown in Table 2, and the test error line is shown in Fig. 10. According to Fig. 10, the histogram error line representing iron is longer than the others, but it is still within the permissible range. Hence, it is reliable to use the average values of elements measured many times to represent the contents of different elements. It was found by comparing Tables 1 and 2 that the dust impurity produced during the forming of parts by SLM was mainly niobium (Nb). The composition may result from the sputtering of powder when the laser acts on the metal powder. It was found by comparing dust compositions in Table 2 that the parts formed by guide plates with different structures at the inlet end of SLM equipment basically have the same compositions, with the main difference being in the Nb content. The mean Nb content of the guide plate (Design 1) was 0.25%, whereas it was 0.15% after further optimization (Design 2), indicating that there is a better internal flow-field distribution, and the quality of the formed parts is higher, after the structure of the inlet end of SLM equipment was optimized. This result verified the previous flow-field simulation analysis results on SLM equipment.
Table 2 component comparison of SLM forming equipment with different inlet deflectors
Element
|
Design 1
|
Design 2
|
Dust
|
|
1
|
2
|
3
|
AVG
|
1
|
2
|
3
|
AVG
|
1
|
2
|
3
|
AVG
|
Mo (%)
|
3.14
|
3.22
|
3.26
|
3.21
|
3.22
|
3.21
|
3.09
|
3.17
|
2.83
|
2.99
|
2.78
|
2.87
|
Ni (%)
|
12.39
|
12.89
|
12.16
|
12.48
|
10.96
|
12.10
|
11.78
|
11.61
|
11.86
|
11.77
|
12.17
|
11.93
|
Fe (%)
|
65.69
|
66.14
|
67.12
|
66.31
|
66.32
|
66.98
|
65.91
|
66.40
|
66.79
|
66.76
|
66.69
|
66.74
|
Cr (%)
|
16.77
|
16.87
|
15.68
|
16.44
|
15.92
|
16.10
|
17.02
|
16.35
|
17.22
|
17.78
|
17.06
|
17.35
|
Nb (%)
|
0.24
|
0.28
|
0.23
|
0.25
|
0.13
|
0.17
|
0.16
|
0.15
|
0.94
|
0.63
|
0.89
|
0.82
|