Solid-like rheological response of non-entangled polymers in the molten state

Abstract.We show that non-entangled polymers display an elastic-like behaviour at a macroscopic scale (probed at some 0.100 mm thickness) up to at least hundred degrees above the glass transition temperature. This observation, found under non-slippage conditions, both for side-chain liquid crystalline polymers and ordinary polymers, is in contradiction with the typically found flow behaviour of polymer melt. Our measurements were carried out with a conventional rheometer at thicknesses of several tenths millimetres. Thus, we were probing bulk properties. The observed elasticity supposedly implies that even in the melt the chains experience a cohesive effect of macroscopic distances, involving collective motions over time scales longer than the individual relaxation time of an individual polymer chain. The detection of such a solid-like property of molten non-entangled polymers is of considerable importance for a better understanding of the polymer dynamics.

[1]  T. Young III. An essay on the cohesion of fluids , 1805, Philosophical Transactions of the Royal Society of London.

[2]  H. Eyring The Activated Complex in Chemical Reactions , 1935 .

[3]  R. W. Goranson A Thermodynamic Treatment of Systems, in Particular of Solutions, from the Point of View of Activity and Related Functions , 1937 .

[4]  A. Adamson Physical chemistry of surfaces , 1960 .

[5]  J. Ferry Viscoelastic properties of polymers , 1961 .

[6]  P. Gennes,et al.  The physics of liquid crystals , 1974 .

[7]  P. Gennes Wetting: statics and dynamics , 1985 .

[8]  Carson,et al.  Relaxation time of confined liquids under shear. , 1991, Physical review letters.

[9]  J. Hubbard,et al.  Semiempirical theory of relaxation: concentrated polymer solution dynamics , 1991 .

[10]  E. W. Fischer Light scattering and dielectric studies on glass forming liquids , 1993 .

[11]  Keller,et al.  Abnormal viscoelastic behavior of side-chain liquid-crystal polymers. , 1994, Physical review letters.

[12]  A. Heuer,et al.  Length Scale of Dynamic Heterogeneities at the Glass Transition Determined by Multidimensional Nuclear Magnetic Resonance , 1998 .

[13]  P. Keller,et al.  Rheology of a comblike liquid crystalline polymer as a function of its molecular weight , 1998 .

[14]  Khanna,et al.  Real-time determination of the slippage length in autophobic polymer dewetting , 2000, Physical review letters.

[15]  Laurence Noirez,et al.  Observation of shear-induced nematic–isotropic transition in side-chain liquid crystal polymers , 2001, Nature.

[16]  K. Shull,et al.  Influence of Molecular Features on the Tackiness of Acrylic Polymer Melts , 2001 .

[17]  A. Bakai Long-range density fluctuations in glass-forming liquids , 2002 .

[18]  K. Kawasaki,et al.  Are transient positional and orientational order important approaching the glass transition , 2003 .

[19]  P. Martinoty,et al.  Dynamic macroscopic heterogeneities in a flexible linear polymer melt , 2003 .

[20]  H. Mendil,et al.  Unexpected giant elasticity in side-chain liquid-crystal polymer melts: A new approach for the understanding of shear-induced phase transitions , 2005 .

[21]  P. Martinoty,et al.  Commentary on “Solid-like rheological response of non-entangled polymers in the molten state” by H. Mendil etal. , 2006, The European physical journal. E, Soft matter.