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Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates
Hydroxyapatite (HA) is one of the most commonly used materials for the coating of bioceramic titanium (Ti) alloys. However, HA has poor mechanical properties and a low bonding strength. Accordingly, the present study replaces HA with a composite coating material consisting of fluorapatite (FA) and 2...
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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MDPI
2016
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5503073/ https://www.ncbi.nlm.nih.gov/pubmed/28773503 http://dx.doi.org/10.3390/ma9050380 |
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author | Chien, Chi-Sheng Liu, Cheng-Wei Kuo, Tsung-Yuan |
author_facet | Chien, Chi-Sheng Liu, Cheng-Wei Kuo, Tsung-Yuan |
author_sort | Chien, Chi-Sheng |
collection | PubMed |
description | Hydroxyapatite (HA) is one of the most commonly used materials for the coating of bioceramic titanium (Ti) alloys. However, HA has poor mechanical properties and a low bonding strength. Accordingly, the present study replaces HA with a composite coating material consisting of fluorapatite (FA) and 20 wt % yttria (3 mol %) stabilized zirconia (ZrO(2), 3Y-TZP). The FA/ZrO(2) coatings are deposited on Ti6Al4V substrates using a Nd:YAG laser cladding system with laser powers and travel speeds of 400 W/200 mm/min, 800 W/400 mm/min, and 1200 W/600 mm/min, respectively. The experimental results show that a significant inter-diffusion of the alloying elements occurs between the coating layer (CL) and the transition layer (TL). Consequently, a strong metallurgical bond is formed between them. During the cladding process, the ZrO(2) is completely decomposed, while the FA is partially decomposed. As a result, the CLs of all the specimens consist mainly of FA, Ca(4)(PO(4))(2)O (TTCP), CaF(2), CaZrO(3), CaTiO(3) and monoclinic phase ZrO(2) (m-ZrO(2)), together with a small amount of θ-Al(2)O(3). As the laser power is increased, CaO, CaCO(3) and trace amounts of tetragonal phase ZrO(2) (t-ZrO(2)) also appear. As the laser power increases from 400 to 800 W, the CL hardness also increases as a result of microstructural refinement and densification. However, at the highest laser power of 1200 W, the CL hardness reduces significantly due to the formation of large amounts of relatively soft CaO and CaCO(3) phase. |
format | Online Article Text |
id | pubmed-5503073 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-55030732017-07-28 Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates Chien, Chi-Sheng Liu, Cheng-Wei Kuo, Tsung-Yuan Materials (Basel) Article Hydroxyapatite (HA) is one of the most commonly used materials for the coating of bioceramic titanium (Ti) alloys. However, HA has poor mechanical properties and a low bonding strength. Accordingly, the present study replaces HA with a composite coating material consisting of fluorapatite (FA) and 20 wt % yttria (3 mol %) stabilized zirconia (ZrO(2), 3Y-TZP). The FA/ZrO(2) coatings are deposited on Ti6Al4V substrates using a Nd:YAG laser cladding system with laser powers and travel speeds of 400 W/200 mm/min, 800 W/400 mm/min, and 1200 W/600 mm/min, respectively. The experimental results show that a significant inter-diffusion of the alloying elements occurs between the coating layer (CL) and the transition layer (TL). Consequently, a strong metallurgical bond is formed between them. During the cladding process, the ZrO(2) is completely decomposed, while the FA is partially decomposed. As a result, the CLs of all the specimens consist mainly of FA, Ca(4)(PO(4))(2)O (TTCP), CaF(2), CaZrO(3), CaTiO(3) and monoclinic phase ZrO(2) (m-ZrO(2)), together with a small amount of θ-Al(2)O(3). As the laser power is increased, CaO, CaCO(3) and trace amounts of tetragonal phase ZrO(2) (t-ZrO(2)) also appear. As the laser power increases from 400 to 800 W, the CL hardness also increases as a result of microstructural refinement and densification. However, at the highest laser power of 1200 W, the CL hardness reduces significantly due to the formation of large amounts of relatively soft CaO and CaCO(3) phase. MDPI 2016-05-17 /pmc/articles/PMC5503073/ /pubmed/28773503 http://dx.doi.org/10.3390/ma9050380 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 Chien, Chi-Sheng Liu, Cheng-Wei Kuo, Tsung-Yuan Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates |
title | Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates |
title_full | Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates |
title_fullStr | Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates |
title_full_unstemmed | Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates |
title_short | Effects of Laser Power Level on Microstructural Properties and Phase Composition of Laser-Clad Fluorapatite/Zirconia Composite Coatings on Ti6Al4V Substrates |
title_sort | effects of laser power level on microstructural properties and phase composition of laser-clad fluorapatite/zirconia composite coatings on ti6al4v substrates |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5503073/ https://www.ncbi.nlm.nih.gov/pubmed/28773503 http://dx.doi.org/10.3390/ma9050380 |
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