On the glassy state of multiphase and pure polymer materials

Abstract In this work we formulate a new glass theory and investigate its suitability for describing the mechanical response of thermoplastic elastomers composed of styrenic-block copolymers. These materials are composed of glassy domains of polystyrene, which physically link soft rubbery chain segments made of either polybutadiene or polyisoprene. We demonstrate that the crossover in the shift factors, observed experimentally to change from Williams–Landel–Ferry to Arrhenius behavior passing through a characteristic crossover temperature T∗ from below, coincides with the crossover from power-law to stretched-exponential behavior of the stress relaxation found in recent tensile experiments. Moreover, we show that the characteristic crossover temperature T∗ is identical with the underlying true equilibrium second-order phase transition temperature T2 of the polystyrene crosslinks, predicted by the thermodynamic theory of Gibbs and Di Marzio for pure glassy polystyrene in the infinite-time limit. By combining the recently introduced theory of Di Marzio and Yang with the significant-structure theory of Eyring and Ree, we develop a new glass theory, which is capable of explaining the mechanical response of multiphase as well as pure glassy materials. Moreover, we show a clear evidence for the existence of T2 postulated in 1950s for pure glasses and hotly debated since then.

[1]  Ludger Santen,et al.  Absence of thermodynamic phase transition in a model glass former , 2000, Nature.

[2]  J. H. Gibbs,et al.  Chain Stiffness and the Lattice Theory of Polymer Phases , 1958 .

[3]  J. H. Gibbs,et al.  Nature of the Glass Transition and the Glassy State , 1958 .

[4]  B. Wunderlich STUDY OF THE CHANGE IN SPECIFIC HEAT OF MONOMERIC AND POLYMERIC GLASSES DURING THE GLASS TRANSITION , 1960 .

[5]  P. Flory,et al.  Second‐Order Transition Temperatures and Related Properties of Polystyrene. I. Influence of Molecular Weight , 1950 .

[6]  T. L. Smith,et al.  Viscoelastic and ultimate tensile properties of styrene‐butadiene‐styrene block copolymers , 2007 .

[7]  R. Landel,et al.  The Temperature Dependence of Relaxation Mechanisms in Amorphous Polymers and Other Glass-Forming Liquids , 1955 .

[8]  G. Adam,et al.  On the Temperature Dependence of Cooperative Relaxation Properties in Glass‐Forming Liquids , 1965 .

[9]  A. Yang,et al.  Configurational Entropy Approach to the Kinetics of Glasses , 1997, Journal of research of the National Institute of Standards and Technology.

[10]  H. Eyring Viscosity, Plasticity, and Diffusion as Examples of Absolute Reaction Rates , 1936 .

[11]  Y. Yue,et al.  Clarifying the glass-transition behaviour of water by comparison with hyperquenched inorganic glasses , 2004, Nature.

[12]  D. Luchinsky Deterministic patterns of noise and the control of chaos , 2002 .

[13]  S. Clarke,et al.  Stress relaxation in transient networks of symmetric triblock styrene-isoprene-styrene copolymer , 2002 .

[14]  J. Beecher,et al.  Morphology and mechanical behavior of block polymers , 1969 .

[15]  P. Pincus,et al.  A theoretical basis for viscoelastic relaxation of elastomers in the long-time limit , 1983 .

[16]  G. Fredrickson,et al.  Prediction of Elastic Properties of a Poly(styrene−butadiene−styrene) Copolymer Using a Mixed Finite Element Approach , 2004 .

[17]  P. M. Lundquist,et al.  Organic Glasses: A New Class of Photorefractive Materials , 1996, Science.

[18]  H. Eyring,et al.  SIGNIFICANT LIQUID STRUCTURES, VI. THE VACANCY THEORY OF LIQUIDS. , 1961, Proceedings of the National Academy of Sciences of the United States of America.

[19]  G. Fredrickson,et al.  Field-Theoretic Computer Simulation Methods for Polymers and Complex Fluids , 2002 .

[20]  Linda J. Broadbelt,et al.  Structural Relaxation of Polymer Glasses at Surfaces, Interfaces, and In Between , 2005, Science.

[21]  S. A. Baeurle Grand canonical auxiliary field Monte Carlo: a new technique for simulating open systems at high density , 2004 .

[22]  Investigation on the kinetic mechanism of structure healing for block copolymer materials after large elongation , 2004 .

[23]  G. Fredrickson Recent Developments in Dynamical Theories of the Liquid-Glass Transition , 1988 .

[24]  S. Torquato Glass transition: Hard knock for thermodynamics , 2000, Nature.

[25]  S. A. Baeurle Computation within the auxiliary field approach , 2003 .

[26]  J. Barěs Glass Transition of the Polymer Microphase , 1975 .

[27]  J. H. Gibbs Nature of the Glass Transition in Polymers , 1956 .

[28]  A. Macfarlane,et al.  A World of Glass , 2004, Science.

[29]  Gregory B. McKenna,et al.  Arrhenius-type temperature dependence of the segmental relaxation below Tg , 1999 .

[30]  W. Kauzmann The Nature of the Glassy State and the Behavior of Liquids at Low Temperatures. , 1948 .

[31]  Daniel B. Miracle A structural model for metallic glasses , 2004 .

[32]  C. Angell Relaxation in liquids, polymers and plastic crystals — strong/fragile patterns and problems☆ , 1991 .

[33]  D. Long,et al.  Heterogeneous nature of the dynamics and glass transition in thin polymer films , 2004, The European physical journal. E, Soft matter.

[34]  A. A. Gurtovenko,et al.  Dynamics of inhomogeneous cross-linked polymers consisting of domains of different sizes , 2001 .

[35]  Sindee L. Simon,et al.  Volume and enthalpy recovery of polystyrene , 2001 .

[36]  M. Parrinello,et al.  A field-theoretical approach to simulation in the classical canonical and grand canonical ensemble , 2002 .

[37]  Marcus T. Cicerone,et al.  Anomalous Diffusion of Probe Molecules in Polystyrene: Evidence for Spatially Heterogeneous Segmental Dynamics , 1995 .

[38]  F. Cohen Tenoudji,et al.  Mechanical properties of cement pastes and mortars at early ages: Evolution with time and degree of hydration , 1996 .

[39]  B. Wunderlich,et al.  50°C ``Transition'' in Polystyrene , 1964 .

[40]  L. Sperling Introduction to physical polymer science , 1986 .

[41]  J. Kurchan,et al.  In and out of equilibrium , 2005, Nature.

[42]  T. L. Smith Time-Dependent Mechanical Properties of Elastomeric Block Polymers in Large Tensile Deformations , 1970 .

[43]  E. Thomas,et al.  Mechanical properties of the double gyroid phase in oriented thermoplastic elastomers , 2000 .

[44]  D. Kaelble,et al.  On the viscoelastic behavior of a styrene‐butadiene‐styrene (S‐B‐S) block copolymer , 1970 .

[45]  A. A. Gusev,et al.  A new semi-phenomenological approach to predict the stress relaxation behavior of thermoplastic elastomers , 2005 .