22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Crystal structure changes of polypropylene films during surface modification by atmospheric pressure dielectric barrier discharge D.A.G. Sawtell1, Z. Abd Allah2, L. Simmons3, J.W. Bradley2, G.T. West1 and P.J. Kelly1 1 2 Surface Engineering Group, Manchester Metropolitan University, Manchester, U.K. Department of Electrical Engineering and Electronics, University of Liverpool, Liverpool, U.K. 3 School of Engineering, Manchester Metropolitan University, Manchester, U.K. Abstract: Atmospheric pressure plasma treatment of polypropylene films is an industrially significant process. Work presented here aims to further understanding of the mechanisms occurring during the plasma modification process, in particular the effects of the plasma on the crystal structure of the polypropylene films. This is supported by comprehensive XRD and FTIR studies of treated films. Keywords: surface modification, atmospheric pressure plasma, polypropylene 1. Introduction Efficient plasma modification of polymeric web at atmospheric pressure is of great industrial interest, due to the environmental benefits and cost savings such a process route provides. Atmospheric pressure plasma systems used for this purpose are characterised by high throughputs of polymeric web, and wide electrodes perpendicular to the direction of web transfer. Although some work has been carried out to elucidate the mechanisms occurring on the surface of the polypropylene during plasma treatment, they have been under a limited set of conditions, and do not take into account the crystal structure of the polymer [1, 2]. Understanding mechanisms and the structural changes that occur to the polypropylene when plasma treatments are made is key to improving the surface treatment process. This suggests that there is a structural change in the polypropylene film caused by the plasma treatment. 2. Methodology A series of treatments have been made to polypropylene films using a dielectric barrier discharge reactor. Nitrogen, both on its own, and with small concentrations of acetylene, nitrous oxide and carbon dioxide, were used as the process gases. XRD was then used to assess crystal structure changes of the polypropylene due to the treatment process, whilst FTIR spectroscopy was used to corroborate these measurements as well as examine the functional groups that have been formed on the surface of the treated polypropylene. White light profilometry was used to assess changes in surface topology, whilst surface energy calculations were made from contact angle measurements. Fig. 1. XRD patterns of treated and untreated polypropylene films. 3. Results XRD results are shown in Fig. 1. The shift to higher angles exhibited in the diffraction patterns by the nitrogen plasma treated polypropylene samples indicates a decrease in the lattice parameters of the crystal structure. P-III-6-47 Fig. 2 represents example FTIR spectra for untreated and plasma treated polypropylene. The peaks at 997 cm-1, 973 cm-1 and 840 cm-1 all exhibit changes after plasma treatment, and this is due to changes in crystalline structure of the polypropylene samples [3]. Fig. 3 shows the ratios of these peaks with increasing plasma treatment time, and they all exhibit an increase in crystallinity after plasma treatment. This is perhaps due to preferential etching of the amorphous regions in between the crystalline lamella within the polypropylene. 4. Conclusions Polypropylene films treated by atmospheric pressure dielectric barrier discharge exhibit crystallinity changes that appear to be due to the preferential etching of amorphous regions during the plasma treatment process. 1 Fig. 2. FTIR spectra of treated and untreated polypropylene films. Fig. 3. Infrared peak ratios at 997 and 973 cm-1 for different treatment times and powers. 5. References [1] R. Dorai and M. Kushner. J. Phys. D: Appl. Phys., 36, 6 (2003) [2] C. Klages, et al. J. Adhesion Sci. Technol., 24, 6 (2010) [3] R.G. Quynn, et al. J. Appl. Polymer Sci., 2, 5 (1959) 2 P-III-6-47
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