Raman spectroscopy sheds new light on TiC formation during the controlled milling of titanium and carbon

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Abstract

A magneto ball mill was used to mill titanium and carbon elemental powder mixtures with compositions of Ti50C50 and Ti60C40 under a helium atmosphere. Previous studies on the milling of titanium and carbon powder mixtures have reported a sudden increase in the temperature of the milling vial, which occurs after a specific milling interval, referred to as tig [Z.G. Liu, J.T. Guo, L.L. Ye, G.S. Li, Z.Q. Hu, Appl. Phys. Lett. 65 (1994) 2666–2668; G.B. Schaffer, J.S. Forrester, J. Mater. Sci. 32 (1997) 3157–3162; N.Q. Wu, S. Lin, J.M. Wu, Z.Z. Li, Mater. Sci. Technol. 14 (1998) 287–291; Z. Xinkun, Z. Kunyu, C. Baochang, L. Qiushi, Z. Xiuqin, C. Tieli, S. Yunsheng, Mater. Sci. Eng. C 16 (2001) 103–105; C. Deidda, S. Doppiu, M. Monagheddu, G. Cocco, J. Metastable Nanocryst. Mater. 15/16 (2003) 215–220]. This sudden temperature increase has been found to correspond to the formation of TiC via a rapid, highly exothermic reaction. In these cases, XRD analysis did not detect TiC in powder sampled before tig. These results, combined with those from studies suggested that the milling period prior to tig represents an incubation period during which the powders become mechanically activated and that no reaction between the starting powders occurs during this time [L. Takacs, J. Solid State Chem. 125 (1996) 75–84; B.K. Yen, T. Aizawa, J. Kihara, J. Am. Ceram. Soc. 81 (1998) 1953–1956; M. Puttaswamy, Y. Chen, B. Jar, J.S. Williams, Mater. Sci. Forum 312–314 (1999) 79–84; G.B. Schaffer, P.G. McCormick, Metall. Transact. A 23A (1992) 1285–1290; M. Mingliang, L. Xinkuan, X. Shenqui, C. Donglang, Z. Jingen, J. Mater. Process. Technol. 116 (2001) 124–127].

In the current investigation a sudden increase in the temperature of the milling vial was also observed after a specific milling duration of tig. XRD analysis of powder sampled before tig did not detect TiC, whilst for powder sampled after tig, XRD analysis indicated that the powder had almost completely transformed into TiC. However, Raman spectroscopy showed the formation of non-stoichiometric TiC in Ti50C50 and Ti60C40 powders sampled before tig. It is believed that the current, and many previous XRD analyses did not detect the formation of TiC prior to tig either because the TiC grain size was too small and/or the phase represented too small a volume fraction of the powder samples to be detected by the XRD method employed. These Raman spectroscopy results suggest that a significant component of the heat generated at tig may be due to a combination of growth of TiC accompanied by consumption of unreacted Ti and carbon, and/or recrystallisation of the TiC formed prior to tig, rather than the direct formation of TiC.

Introduction

Titanium carbide (TiC) is suited to a number of commercial applications, such as abrasives, cutting tools, grinding wheels and coated cutting tips because it exhibits very high hardness, high melting temperature and excellent thermal and chemical stability [1], [11], [12], [13], [14]. Recent studies have shown that high-energy milling of titanium and carbon powders may be a viable synthesis method for the production of TiC powder [1], [2], [3], [4], [5], [6], [12], [13], [14], [15], [16]. However, the process by which titanium and carbon react to form TiC during milling is not yet well understood. The aim of this study is to further the understanding of this reaction through the use of Raman spectroscopy to characterise the milling products.

Very little has been reported on the use of Raman spectroscopy to study TiC. The literature states that stoichiometric TiC has no Raman active vibrational modes and that Raman scattering in TiC is due to disorder induced by carbon vacancies [17], [18]. Klein et al. [17] produced Raman spectra of TiCx where x = 0.97, 0.90 and 0.80, whilst Amer et al. [18] published a Raman spectrum of TiC0.67.

Section snippets

Experimental

Titanium powder of particle size <250 μm and minimum purity of 99.9% was mixed with high purity activated carbon powder to give compositions of Ti50C50 and Ti60C40. Controlled ball milling was performed using a magneto ball mill (Uni-Ball-Mill 5) operating in impact mode under a high purity helium atmosphere. Samples were taken using a glovebag to prevent contamination of the powders. The external temperature of the milling vial was monitored during milling using an infrared thermometer.

X-ray

XRD analysis of as-milled Ti–C powders

An abrupt increase in the temperature of the milling vial was observed after milling for a specific duration, referred to as the ignition time, tig. The average ignition time for Ti50C50 was approximately 71 h, whilst that for Ti60C40 was approximately 41 h. Typical plots of the milling vial temperature versus milling time are shown in Fig. 1. The ignition time was repeatable within ±2 h of the average ignition time.

The XRD patterns for samples taken before and after tig are shown in Fig. 2, Fig. 3

Discussion

When milling Ti50C50 and Ti60C40 elemental powder mixtures, a sudden increase in the temperature of the milling vial was observed after a milling duration of tig. XRD analysis of powder sampled before tig revealed only peaks corresponding to titanium. For powder sampled after tig, XRD analysis revealed strong peaks corresponding to TiC and a very weak peak corresponding to a small amount of unreacted titanium. These results suggest that the sudden temperature increase detected during milling is

Conclusions

Raman spectroscopy detected the formation of TiC well before it was detected by XRD analysis. For Ti50C50 and Ti60C40 elemental powder mixtures, the combined results of external mill temperature monitoring and X-ray diffractommetry indicated that, after a milling duration of tig, TiC formed rapidly via a mechanically induced reaction which resulted in sudden heating of the milling vial. However, Raman spectroscopy clearly showed the formation of non-stoichiometric TiC prior to tig. This is a

Acknowledgements

The authors wish to thank Dr. Peter Innis from the Intelligent Polymer Research Institute and ARC Centre for Nanostructured Electromaterials at the University of Wollongong for his help and advice with the Raman spectroscopy. The authors also gratefully acknowledge financial support from the Australian Research Council, under ARC-Large Grant No. A00103022 and ARC-Discovery Grant No. DP0451907. The Reviewer is also acknowledged for valuable suggestions for improvements to the article.

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