Modelling of thermomechanical behaviour of fibrous polymeric composite materials subject to relaxation transition in the matrix

BackgroundFiber–reinforced polymer composite materials are widely used in different branches of industry due to their distinctive features such as high specific strength and stiffness and due to as considerable opportunity to formulate materials with controllable variation of properties in response to the action of external factors (smart-materials). A distinguishing feature of products made of composite materials is that the processes of product and material fabrication are inseparable. Therefore the estimation of composite properties based on the composite architecture and properties of the reinforcing fibers and matrix is a very actual task.MethodsThe model of polymer behavior at glass transition recently developed by the authors was generalized to the case of fiber-reinforced polymer matrix composites using two approaches: one is base on the concept of free specific energy, the other – on the growth of matrix stiffness. For homogeneous materials these two approaches are of equal worth, whereas for composite materials they give different results under deformation in the transverse direction. The stiffness growth approach is more accurate, but is very expensive computationally and, is highly sensitive to the experimental data errors.ResultsUsing the finite element method and averaging technique the thermoelastic constants of composites containing different types of fibers in the glassy and high-elastic states were calculated based on the fiber and matrix properties. Softening of the matrix has an insignificant effect on the longitudinal modulus of a composite but leads to a considerable decrease of the transverse and shear moduli. The coefficient of thermal expansion in the transverse direction is much higher than the coefficient of thermal expansion in the longitudinal direction, especially when the composite is in the high-elastic state.ConclusionThe model of polymer behavior at glass transition recently developed by the authors can be generalized to the case of fiber-reinforced polymer matrix composites. The thermoelastic constants of composites containing different types of fibers can be calculated from the fiber and matrix properties using the finite element method and averaging technique.

[1]  Lallit Anand,et al.  A constitutive theory for the mechanical response of amorphous metals at high temperatures spanning the glass transition temperature: Application to microscale thermoplastic forming , 2008 .

[2]  Yiping Liu,et al.  Thermomechanics of shape memory polymers: Uniaxial experiments and constitutive modeling , 2006 .

[3]  A. Muliana,et al.  Responses of viscoelastic polymer composites with temperature and time dependent constituents , 2009 .

[4]  Rodney Hill,et al.  Theory of mechanical properties of fibre-strengthened materials—III. self-consistent model , 1965 .

[5]  N. Brown Deformation of Polymers , 1973 .

[6]  Thao D. Nguyen,et al.  A thermoviscoelastic model for amorphous shape memory polymers: Incorporating structural and stress relaxation , 2008 .

[7]  Rodney Hill,et al.  Theory of mechanical properties of fibre-strengthened materials: I. Elastic behaviour , 1964 .

[8]  Lallit Anand,et al.  Thermally actuated shape-memory polymers: Experiments, theory, and numerical simulations , 2010 .

[9]  R. Christensen,et al.  Mechanics of composite materials , 1979 .

[10]  R. Hill A self-consistent mechanics of composite materials , 1965 .

[11]  C. P. Buckley,et al.  Glass-rubber constitutive model for amorphous polymers near the glass transition , 1995 .

[12]  Thao D. Nguyen,et al.  Finite deformation thermo-mechanical behavior of thermally induced shape memory polymers , 2008 .

[13]  Yanju Liu,et al.  Thermal mechanical constitutive model of fiber reinforced shape memory polymer composite: Based on bridging model , 2014 .

[14]  K. Sze,et al.  Studying the thermomechanical behavior of SM composites with aligned SMA short fibers by micromechanical approaches , 2001 .

[15]  Lallit Anand,et al.  A thermo-mechanically-coupled large-deformation theory for amorphous polymers in a temperature range which spans their glass transition , 2010 .

[16]  F. Auricchio,et al.  An experimental, theoretical and numerical investigation of shape memory polymers , 2015 .

[17]  Matthias Fuchs,et al.  Glass rheology: From mode-coupling theory to a dynamical yield criterion , 2009, Proceedings of the National Academy of Sciences.

[18]  T. Tervoort,et al.  A multi‐mode approach to finite, three‐dimensional, nonlinear viscoelastic behavior of polymer glasses , 1996 .

[19]  Martin L. Dunn,et al.  A finite deformation thermomechanical constitutive model for triple shape polymeric composites based on dual thermal transitions , 2014 .

[20]  Jinwoo Choi,et al.  Modeling the glass transition of amorphous networks for shape-memory behavior , 2013 .

[21]  V. Matveenko,et al.  Models of thermomechanical behavior of polymeric materials undergoing glass transition , 2012 .

[22]  Martin L. Dunn,et al.  Thermomechanical behavior of shape memory elastomeric composites , 2012 .

[23]  Rheological constitutive equation for a model of soft glassy materials , 1997, cond-mat/9712001.

[24]  Mary C. Boyce,et al.  Constitutive modeling of the finite strain behavior of amorphous polymers in and above the glass transition , 2007 .

[25]  Self-consistent approach of the constitutive law of a two-phase visco-elastic material described by fractional derivative models , 2010 .

[26]  James M. Caruthers,et al.  Thermodynamic constitutive equations for materials with memory on a material time scale , 1996 .

[27]  O. Smetannikov,et al.  Constitutive relations for viscoelastic materials under thermorelaxation transition , 2015 .