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...

Full description

Saved in:
Bibliographic Details
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
Tags: Add Tag
No Tags, Be the first to tag this record!
Institution: Nanyang Technological University
Language: English
Description
Summary: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).