Abstract.
We present results from molecular dynamics simulations of strictly two-dimensional (2D) polymer melts and thin polymer films in a slit geometry of thickness of the order of the radius of gyration. We find that the dynamics of the 2D melt is qualitatively different from that of the films. The 2D monomer mean-square displacement shows a t8/15 power law at intermediate times instead of the t1/2 law expected from Rouse theory for nonentangled chains. In films of finite thickness, chain entanglements may occur. The impact of confinement on the entanglement length Ne has been analyzed by a primitive path analysis. The analysis reveals that Ne increases strongly with decreasing film thickness.
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References
S. Granick et al., J. Polym. Sci. B: Polym. Phys. 41, 2755 (2003)
M. Rubinstein, R.H. Colby, Polymer Physics (Oxford University Press, Oxford, 2003)
A.J. Silberberg, Colloid Interface Sci. 90, 86 (1982)
H.R. Brown, T.P. Russell, Macromolecules 29, 798 (1996)
L. Si et al., Phys. Rev. Lett. 94, 127801 (2005)
A.N. Semenov, A. Johner, Eur. Phys. J. E 12, 469 (2003)
J. Baschnagel, F. Varnik, J. Phys.: Condens. Matter 17, R851 (2005)
S. Peter, H. Meyer, J. Baschnagel, J. Polym. Sci. B: Polym. Phys. (2006) (in press)
H. Meyer, F. Müller-Plathe, J. Chem. Phys. 115, 7807 (2001)
H. Meyer, F. Müller-Plathe, Macromolecules 35, 1241 (2002)
K. Kremer, G.S. Grest, J. Chem. Phys. 92, 5057 (1990)
The energy cost for two polymers to cross each other is Ex ≈70 kB T if D=1.9. By contrast, we found a maximum energy of Ec ≈8 kB T for the closest approach between two monomers in the simulation. Since Ec ≪Ex, no chain crossings were observed; the film with D=1.9 may be considered as “strictly” two-dimensional
A. Cavallo, M. Müller, K. Binder, Europhys. Lett. 61, 214 (2003)
M. Müller, J. Chem. Phys. 116, 9930 (2002)
A. Cavallo et al., J. Phys.: Condens. Matter 17, S1697 (2005)
R.L. Jones et al., Nature 400, 147 (1999)
J.P. Wittmer et al., Phys. Rev. Lett. 93, 147801 (2004)
R. Everaers et al., Science 303, 823 (2004)
S.K. Sumumaran et al., J. Polym. Sci. B: Polym. Phys. 43, 917 (2005)
We feel that our results should not be interpreted in the sense that the criterion for an increase of Ne is necessarily h < Rg bulk. It may be that it rather requires h to become smaller than the tube diameter dt bulk. A test of this hypothesis necessitates simulations of larger N because the two scales, dt bulk and Rg bulk, are not well separated for the studied chain length N=256
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Meyer, H., Kreer, T., Cavallo, A. et al. On the dynamics and disentanglement in thin and two-dimensional polymer films. Eur. Phys. J. Spec. Top. 141, 167–172 (2007). https://doi.org/10.1140/epjst/e2007-00035-9
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DOI: https://doi.org/10.1140/epjst/e2007-00035-9