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STOP FEU, Oran 2010 Posters Thème V<br />

P.5.1<br />

Physical properties of polymeric matérials<br />

N.Berrahou, M.O.Bensaid, S.Hiadsi<br />

Laboratory of the Electronic Microscopy and Materials Science<br />

Physics Department-faculty of Science USTO. BP .1505 El M’Naouar, 31100 Oran,<br />

Algéria :E-mail: berrahounoria@yahoo.fr<br />

The structures and properties of polymer melts at various interfaces have been the<br />

subject of numerous studies in recent years due to the critical role p<strong>la</strong>y in such<br />

important polymer applications.Computer simu<strong>la</strong>tion has become a major tool in<br />

polymer science in the same way as analytical theory and experiment. Consequently,<br />

the <strong>de</strong>velopment of appropriate m<strong>et</strong>hod of simu<strong>la</strong>tions for the polymers is a field of<br />

active research. These m<strong>et</strong>hods allow to investigate the propertiesof the polymer un<strong>de</strong>r<br />

different conditions such as in solution, in a polymer melt or in the crystalline state. In<br />

our work we have simu<strong>la</strong>ted by molecu<strong>la</strong>r dynamics m<strong>et</strong>hod, two polymer chains in<br />

their amorphous state , (poly m<strong>et</strong>hyl m<strong>et</strong>hacry<strong>la</strong>te) PMMA and (poly m<strong>et</strong>hyl acry<strong>la</strong>te)<br />

PMA using different force fields PCFF, COMPASS, AMBER, to view their g<strong>la</strong>ss<br />

transition. Given a simu<strong>la</strong>ted difference in Tg b<strong>et</strong>ween the two chains in agreement<br />

with experimental data. Energy studies have been un<strong>de</strong>rtaken to un<strong>de</strong>rstand the<br />

reasons for this discrepancy. The first study showed an energy difference mainly<br />

attributable to differences in intermolecu<strong>la</strong>r interactions and opening angle intra-dyad.<br />

These observations may exp<strong>la</strong>in the observed difference in Tg b<strong>et</strong>ween the two<br />

polymers. Thus the difference in results b<strong>et</strong>ween the force fields used.<br />

Keywords: polym<strong>et</strong>hylm<strong>et</strong>hacry<strong>la</strong>te; polym<strong>et</strong>hyacry<strong>la</strong>te; molecu<strong>la</strong>r dynamics; g<strong>la</strong>ss<br />

transition; force fields<br />

References:<br />

[1] Kuter Bin<strong>de</strong>r, Monte Carlo and Molecu<strong>la</strong>r Dynamics simu<strong>la</strong>tion in<br />

Polymer Scienc, Oxford University Press 1995<br />

[2] Mesfin Tsige ,P.L.Taylor ,Physical rewiew E,Vol 65 , 2002 , p- p 021805<br />

[3] Ash BJ, Siegel RW, Schadler LS. Macromolecules .Vol 37, p-p.1358, 2004<br />

[4] E. Rudrik, J. Thermal Analysis, Vol 49 , p. 465-469, 1997<br />

[5] A.Sol<strong>de</strong>ra, N.M<strong>et</strong>at<strong>la</strong>, j .Molecu<strong>la</strong>r Design, Vol 4, p.721-736 2005<br />

[6] E Osawa,KB.Lipkowitz, Reviewsin computational chemistry,Vol 6,p 6,1995<br />

[7] A.Sol<strong>de</strong>ra, N.M<strong>et</strong>at<strong>la</strong>, j .Composites.PartA, Vol 36, p 521-530, 2005<br />

[8] A.Sol<strong>de</strong>ra, Polymer, Vol 43, p-p 4269-4275, 2002<br />

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