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eISSN: 2574-9927

Material Science & Engineering International Journal

Mini Review Volume 3 Issue 2

Effect of hatch distance on CuSn10 specimens by selective laser melting

Jinwu Kang,1 Xiang Wang,1 Chengyang Deng,1 Yunlong Feng,1 Tao Feng,2 Jihao Y,1,2 Pengyue WU2

1Tsinghua University, China
2Beijing e-Plus 3D Tech.Co. Ltd, China

Correspondence: Jinwu Kang, School of Materials Science and Engineering, Key Laboratory for Advanced Materials Processing Technology, Tsinghua University, Beijing 100084, China

Received: March 31, 2019 | Published: April 8, 2019

Citation: Kang J, Wang X, Deng C, et al. Effect of hatch distance on CuSn10 specimens by selective laser melting. Material Sci & Eng. 2019;3(2):63-65. DOI: 10.15406/mseij.2019.03.00092

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Abstract

Selective laser melting (SLM) is one of promising additive manufacturing methods, especially for precision parts. Its application in copper alloys is of significance. However, there is rare research achievements about the effect of fabrication parameters on the microstructure and quality of copper alloy parts. In this paper, tin bronze (CuSn10) bars were fabricated with different hatch distance from 0.06mm to 0.1mm and different scanning speed from 198mm/s to 330mm/s, but same area laser energy density. Porosity is mainly dependent on hatch distance instead of scanning speed. The porosity decreases with the decrease of hatch distance. Their microstructure was rose like fine grain cluster growing from melt pool border to pool center, in which fine columnar grain is about 5μm×20μm and equi-axed grains is about 3.5μm in diameter. The formed specimens achieved high hardness (78.2HRB) at hatch distance 0.06mm. Fine microstructure leads to the improvement of mechanical properties.

Keywords: selective laser melting, Cu Sn10 bronze alloy, laser energy density, hatch distance, microstructure, hardness

Introduction

Selective laser melting (SLM) is one of promising additive manufacturing methods, especially for precision parts. It can produce complicated three-dimensional shapes in a layer by-layer style. It has been mainly applied into titanium alloys, nickel alloys and steels.1–3 Tin bronze is widely used as bearing materials for its good friction and wear behaviors. Powders metallurgy (PM), and mechanical ball milling (MBM), and casting are usually used for CuSn10 powder sintering.4–8 The porosity and geometry precision are the most concern problems. Additive manufacturing provides a new way to make tin bronze parts. However, the physical properties of copper are different from titanium, nickel alloys and steels, therefore, it is necessary to investigate the principles of selective laser sintering of tin bronze powder. The main parameters of SLM are laser power, scanning speed, layer thickness and hatch distance. Scudino et al.,9 achieved far better mechanical properties of CuSn10 specimens by SLM corresponding to as-cast properties. Deng et al.,10 studied the effect of laser energy density on the microstructure, mechanical properties of Tin bronze parts by SLM and found the laser energy density is the main factor for porosity formation and the mechanical properties. In this paper, The SLM of tin bronze (CuSn10) powder was performed with same laser energy density to investigate the effect of scanning speed and hatch distance on microstructure and mechanical properties.

Experiment

A typical Tin bronze alloy CuSn10 with 90% Cu and 10% Sn is selected for the selective laser melting process. The powder is in the range of 20-50μm. Bar samples of 20mm×20mm×45mm were fabricated using the 3D printer EP-M100T (manufactured by Beijing e-Plus 3D Tech. Co. Ltd.). The fabrication parameters are listed in Table 1. Three specimens were produced by different scanning speeds and different hatch distances, but same laser energy density (laser energy divided by hatch distance and scanning speed). The fabrication chamber was filled with argon atmosphere, and the content of oxygen was below 100ppm. The base plate was at room temperature. During the fabrication process, snake scanning routes were adopted and the scanning direction was rotated 60o corresponding to the previous layer, as shown in Figure 1A. The formed bars, as shown in Figure 1B, were removed from the base plate, and then specimens were cut from them for density measurement, hardness test and microstructure observation. The microstructure of the horizontal plane of these specimens were characterized by using a Keyence VHX-6000 digital microscope. The density of the formed specimens was determined by Archimedes method. Hardness was measured by HR-150A Sclerometer.

Figure 1 Laser scanning strategy (A) and a fabricated specimen.

Specimen

Hatch distance
/mm

Scanning Speed
mm/s

Layer thickness
/mm

Laser Power
/W

Laser energy density
/J/mm2

1

0.06

330

0.02

95

240

2

0.08

247

0.02

95

240

3

0.10

198

0.02

95

240

Table 1 Experimental parameters

Results and discussion

The effect of hatch distance on the microstructure and mechanical property of the formed specimens is shown in Figure 2. It can be seen there are number and size of porosities in these specimens, and they increase with the increase of hatch distance. These porosities locate at the border of tracks. The size of porosities in the specimen of 0.06mm is around 10μm. As the hatch distance increases to 0.1mm, the profile of each track is very clear with poor overlapping with adjacent tracks, resulting into strips of porosities around 100μm long and 20μm wide. For all the three conditions, there is only uniformly distributed α-Cu phase, rose-like fine grain cluster including columnar grains of about 5μm×20μm and equi-axed grains of 3.5μm in diameter dispersed among them grows from the border of melt pool to the moving direction, as shown in Figure 3. Deng et al. found that the mechanical properties increase with the increase of laser energy density in the range of 210-220 J/mm2 with fixed hatch distance 0.06mm.11 Here, under the same laser energy condition 240 J/mm2, although the scanning speed of specimen #3 is less than that of the specimen #1, but the porosity increases, i.e., the microstructure is mainly dependent on the hatch distance for the hatch distance in the range of 0.06-0.1mm. The density and hardness decrease with the increase of hatch distance, as shown in Figure 2D. The highest density and harness of reaches 8.60kg/m3 and 78.2HRB, respectively for specimen #1. The hardness is far higher than that of the as-cast condition. The reason is the fine grains in the as-print condition.

Figure 2 Microstructure, density and hardness s at different hatch distance.

Figure 3 Microstructure (×3000) of #1 at hatch distance 0.06mm.

Conclusion

Tin bronze (CuSn10) bars were fabricated with different hatch distance from 0.06mm to 0.1mm and different scanning speed from 198mm/s to 330mm/s, but same area laser energy density. The effect of hatch distance is greater than scanning speed. The porosity decreases with the decrease of hatch distance. Their microstructure was rose like α-Cu e fine grain cluster growing to melt pool border to pool center. The fine columnar grain is about 5μm ×20μm and equi-axed grains is about 3.5μm in diameter. The formed specimens achieved high hardness (79HRB) at hatch distance 0.06mm. The fine microstructure leads to the improvement of mechanical properties.

Acknowledgements

This research study was funded by the National Science and Technology Major Project of the Ministry of Science and Technology of China under Project No. 2016YFB1100703.

Conflict of interest

Author declares that there is no conflicts of interest.

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