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Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V
To increase building rate and save cost, the selective laser melting (SLM) of Ti6Al4V with a high layer thickness (200 μm) and low cost coarse powders (53 μm–106 μm) at a laser power of 400 W is investigated in this preliminary study. A relatively large laser beam with a diameter of 200 μm is utiliz...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5456986/ https://www.ncbi.nlm.nih.gov/pubmed/28774097 http://dx.doi.org/10.3390/ma9120975 |
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author | Shi, Xuezhi Ma, Shuyuan Liu, Changmeng Chen, Cheng Wu, Qianru Chen, Xianping Lu, Jiping |
author_facet | Shi, Xuezhi Ma, Shuyuan Liu, Changmeng Chen, Cheng Wu, Qianru Chen, Xianping Lu, Jiping |
author_sort | Shi, Xuezhi |
collection | PubMed |
description | To increase building rate and save cost, the selective laser melting (SLM) of Ti6Al4V with a high layer thickness (200 μm) and low cost coarse powders (53 μm–106 μm) at a laser power of 400 W is investigated in this preliminary study. A relatively large laser beam with a diameter of 200 μm is utilized to produce a stable melt pool at high layer thickness, and the appropriate scanning track, which has a smooth surface with a shallow contact angle, can be obtained at the scanning speeds from 40 mm/s to 80 mm/s. By adjusting the hatch spacings, the density of multi-layer samples can be up to 99.99%, which is much higher than that achieved in previous studies about high layer thickness selective laser melting. Meanwhile, the building rate can be up to 7.2 mm(3)/s, which is about 2 times–9 times that of the commercial equipment. Besides, two kinds of defects are observed: the large un-melted defects and the small spherical micropores. The formation of the un-melted defects is mainly attributed to the inappropriate overlap rates and the unstable scanning tracks, which can be eliminated by adjusting the processing parameters. Nevertheless, the micropores cannot be completely eliminated. It is worth noting that the high layer thickness plays a key role on surface roughness rather than tensile properties during the SLM process. Although a sample with a relatively coarse surface is generated, the average values of yield strength, ultimate tensile strength, and elongation are 1050 MPa, 1140 MPa, and 7.03%, respectively, which are not obviously different than those with the thin layer thickness used in previous research; this is due to the similar metallurgical bonding and microstructure. |
format | Online Article Text |
id | pubmed-5456986 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-54569862017-07-28 Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V Shi, Xuezhi Ma, Shuyuan Liu, Changmeng Chen, Cheng Wu, Qianru Chen, Xianping Lu, Jiping Materials (Basel) Article To increase building rate and save cost, the selective laser melting (SLM) of Ti6Al4V with a high layer thickness (200 μm) and low cost coarse powders (53 μm–106 μm) at a laser power of 400 W is investigated in this preliminary study. A relatively large laser beam with a diameter of 200 μm is utilized to produce a stable melt pool at high layer thickness, and the appropriate scanning track, which has a smooth surface with a shallow contact angle, can be obtained at the scanning speeds from 40 mm/s to 80 mm/s. By adjusting the hatch spacings, the density of multi-layer samples can be up to 99.99%, which is much higher than that achieved in previous studies about high layer thickness selective laser melting. Meanwhile, the building rate can be up to 7.2 mm(3)/s, which is about 2 times–9 times that of the commercial equipment. Besides, two kinds of defects are observed: the large un-melted defects and the small spherical micropores. The formation of the un-melted defects is mainly attributed to the inappropriate overlap rates and the unstable scanning tracks, which can be eliminated by adjusting the processing parameters. Nevertheless, the micropores cannot be completely eliminated. It is worth noting that the high layer thickness plays a key role on surface roughness rather than tensile properties during the SLM process. Although a sample with a relatively coarse surface is generated, the average values of yield strength, ultimate tensile strength, and elongation are 1050 MPa, 1140 MPa, and 7.03%, respectively, which are not obviously different than those with the thin layer thickness used in previous research; this is due to the similar metallurgical bonding and microstructure. MDPI 2016-12-01 /pmc/articles/PMC5456986/ /pubmed/28774097 http://dx.doi.org/10.3390/ma9120975 Text en © 2016 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC-BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Shi, Xuezhi Ma, Shuyuan Liu, Changmeng Chen, Cheng Wu, Qianru Chen, Xianping Lu, Jiping Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V |
title | Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V |
title_full | Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V |
title_fullStr | Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V |
title_full_unstemmed | Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V |
title_short | Performance of High Layer Thickness in Selective Laser Melting of Ti6Al4V |
title_sort | performance of high layer thickness in selective laser melting of ti6al4v |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5456986/ https://www.ncbi.nlm.nih.gov/pubmed/28774097 http://dx.doi.org/10.3390/ma9120975 |
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