Studies on dielectric properties of Al–Zr oxide composites sintered by thermal plasma
Introduction
Al–Zr composites of fine monoclinic/tetragonal zirconia particles dispersed in an alumina matrix have long been recognized to yield toughened Ceramics [1]. Al–Zr composites are of interest for various structural applications [2], [3], [4]. Finer grain size in this system result in higher fracture toughness [5], [6] and strength [7], [8], [9]. Composites of Al–Zr system required high-temperature sintering to densify and are ideal materials to examine as possible candidate for low-temperature compaction. The metastable structure of the rapid solidification processed (RSP) materials may not necessarily be retained after conventional densification, which typically involve sintering at high temperature. Many advanced sintering techniques are being used for rapid sintering of high temperature ceramic materials including the use of laser, microwave and plasma source. However, using plasmas heating source, samples are heated to high temperature within very short period to promote rapid densification with restrained grain growth [10], [11]. Both DC and RF plasma system are used for sintering in a thermally equilibrium state where electron and ion temperature are identical. Condition satisfying this is termed as thermal plasma, which has a number of advantages as compared to conventional heating technique. This includes the potential for rapid heating, lower energy requirement, uniform grain size with no runway grain growth, etc. Most of the work on thermal plasma reported to date has focus on the relationship between density and temperature. It is desirable to achieve maximum density with minimum grain growth within minimum sintering time and power consumption. We have prepared a series of oxide materials with Alx–Zr100−x (x=0, 10, 20,…100) and attempts were taken to sintered using extended arc thermal plasma heating (EATPH) source. However, to our knowledge, no work in the area of sintering using EATPH has been reported except our group [12], [13]. Further to it, authors are not aware of any report regarding the dielectric properties of these plasma-sintered materials using EATPH. The aim of our paper is to study the dielectric property of highly dense sintered materials prepared by thermal plasma heating and compared with conventional sintered sample.
Section snippets
Experimental
One EATPH system has been designed and fabricated using 30-kW DC power supply. Water-cooled stainless steel double wall cylindrical chamber (outer) is fixed with suitable thermal insulation by bubble alumina for the confinement of plasma heating. Provisions were made for fine adjustment of the electrode distance to get required arc length. Plasmagen gas (argon) flow into the electrode space is provided through a narrow hole through upper electrode (cathode). Sample holder is placed coaxially
Result and discussion
Dense and homogenous sintered pellets were obtained for each of the compaction within 15 min using 15-kW plasma power. Physical densifications of the pellets were observed at different plasma power and sintering time. It is observed that the final density of the materials can be achieved close to the theoretical value using proper plasma power and sintering time. A typical XRD pattern of a sample (Al30–Zr70) sintered by plasma and conventional route is shown in Fig. 1. It is noted that sharp
Conclusion
Higher density (≥95%) sintered product of Al–Zr-based oxide ceramics are produced using only 20 min of sintering time using EATPH system. Preliminary measurements of dielectric properties as a function of frequencies and temperature gave useful information regarding possible dipole mechanism to understand pinning behavior of dipoles operating under alternating field. It is also noted that microstructure also plays an important role which may induced local change ordering in dipole network and,
Acknowledgements
The authors are thankful to the Council of Scientific and Industrial Research (CSIR), NewDelhi for providing financial support to carryout this work. We acknowledge the experimental support and facilities extended to us by Physics Department, IIT Kharagpur, India.
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