Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres

This work involves an investigation of the neck growth kinetics of free-packed spherical shaped binderless tungsten carbide particles during microwave and spark-plasma sintering. The application of a classical sphere to sphere approach showed the possibility of identifying the main diffusion mechani...

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Main Authors: Demirskyi, Dmytro, Borodianska, Hanna, Agrawal, Dinesh, Ragulya, Andrey, Sakka, Yoshio, Vasylkiv, Oleg
Other Authors: Temasek Laboratories
Format: Article
Language:English
Published: 2013
Online Access:https://hdl.handle.net/10356/96832
http://hdl.handle.net/10220/11673
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-968322020-03-07T12:47:16Z Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres Demirskyi, Dmytro Borodianska, Hanna Agrawal, Dinesh Ragulya, Andrey Sakka, Yoshio Vasylkiv, Oleg Temasek Laboratories This work involves an investigation of the neck growth kinetics of free-packed spherical shaped binderless tungsten carbide particles during microwave and spark-plasma sintering. The application of a classical sphere to sphere approach showed the possibility of identifying the main diffusion mechanisms operating during the initial stage of microwave sintering of tungsten carbide powder. An anomalous neck growth rate in the initial period during microwave and spark-plasma sintering processes, up to 100 times faster in comparison to conventional sintering, was also revealed. Volume diffusion was enhanced by a small amount of a liquid phase, and surface diffusion was proposed as the primary mass transport mechanism for microwave sintering. The simulation operation of grain-boundary diffusion and power law creep was responsible for neck growth during spark-plasma sintering. Numerical simulation of neck growth revealed high values of the diffusion coefficient for microwave (3.41 × 10−8 m2 s−1 at 1200 °C) and spark-plasma sintering (5.41 × 10−8 m2 s−1 at 1200 °C). In the case of conventional sintering, the diffusion coefficients calculated are in good agreement with values for diffusion of W and C in a W–C system (8.6 × 10−16 m2 s−1 at 1200 °C). Low values of the apparent activation energy (Ea) for microwave and spark-plasma sintering (62 and 52 kJ mol−1) have been obtained. For conventional sintering, all data collected indicate grain-boundary diffusion as the primary sintering mechanism (272 kJ mol−1). 2013-07-17T03:32:21Z 2019-12-06T19:35:32Z 2013-07-17T03:32:21Z 2019-12-06T19:35:32Z 2012 2012 Journal Article Demirskyi, D., Borodianska, H., Agrawal, D., Ragulya, A., Sakka, Y., & Vasylkiv, O. (2012). Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres. Journal of Alloys and Compounds, 523, 1-10. 0925-8388 https://hdl.handle.net/10356/96832 http://hdl.handle.net/10220/11673 10.1016/j.jallcom.2012.01.146 en Journal of alloys and compounds © 2012 Elsevier B.V.
institution Nanyang Technological University
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country Singapore
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description This work involves an investigation of the neck growth kinetics of free-packed spherical shaped binderless tungsten carbide particles during microwave and spark-plasma sintering. The application of a classical sphere to sphere approach showed the possibility of identifying the main diffusion mechanisms operating during the initial stage of microwave sintering of tungsten carbide powder. An anomalous neck growth rate in the initial period during microwave and spark-plasma sintering processes, up to 100 times faster in comparison to conventional sintering, was also revealed. Volume diffusion was enhanced by a small amount of a liquid phase, and surface diffusion was proposed as the primary mass transport mechanism for microwave sintering. The simulation operation of grain-boundary diffusion and power law creep was responsible for neck growth during spark-plasma sintering. Numerical simulation of neck growth revealed high values of the diffusion coefficient for microwave (3.41 × 10−8 m2 s−1 at 1200 °C) and spark-plasma sintering (5.41 × 10−8 m2 s−1 at 1200 °C). In the case of conventional sintering, the diffusion coefficients calculated are in good agreement with values for diffusion of W and C in a W–C system (8.6 × 10−16 m2 s−1 at 1200 °C). Low values of the apparent activation energy (Ea) for microwave and spark-plasma sintering (62 and 52 kJ mol−1) have been obtained. For conventional sintering, all data collected indicate grain-boundary diffusion as the primary sintering mechanism (272 kJ mol−1).
author2 Temasek Laboratories
author_facet Temasek Laboratories
Demirskyi, Dmytro
Borodianska, Hanna
Agrawal, Dinesh
Ragulya, Andrey
Sakka, Yoshio
Vasylkiv, Oleg
format Article
author Demirskyi, Dmytro
Borodianska, Hanna
Agrawal, Dinesh
Ragulya, Andrey
Sakka, Yoshio
Vasylkiv, Oleg
spellingShingle Demirskyi, Dmytro
Borodianska, Hanna
Agrawal, Dinesh
Ragulya, Andrey
Sakka, Yoshio
Vasylkiv, Oleg
Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres
author_sort Demirskyi, Dmytro
title Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres
title_short Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres
title_full Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres
title_fullStr Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres
title_full_unstemmed Peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of WC spheres
title_sort peculiarities of the neck growth process during initial stage of spark-plasma, microwave and conventional sintering of wc spheres
publishDate 2013
url https://hdl.handle.net/10356/96832
http://hdl.handle.net/10220/11673
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