A thermodynamic framework to develop rate-type models for fluids without instantaneous elasticity

In this paper, we apply the thermodynamic framework recently put into place by Rajagopal and co-workers, to develop rate-type models for viscoelastic fluids which do not possess instantaneous elasticity. To illustrate the capabilities of such models, we make a specific choice for the specific Helmholtz potential and the rate of dissipation and consider the creep and stress relaxation response associated with the model. Given specific forms for the Helmholtz potential and the rate of dissipation, the rate of dissipation is maximized with the constraint that the difference between the stress power and the rate of change of Helmholtz potential is equal to the rate of dissipation and any other constraint that may be applicable such as incompressibility. We show that the class of models that are developed exhibit fluid-like characteristics, when none of the material moduli that appear in the model are not zero, and are incapable of instantaneous elastic response. They also include Maxwell-like and Kelvin-Voigt-like viscoelastic materials (when certain material moduli take special values).

[1]  K. Rajagopal,et al.  A thermodynamic framework for the study of crystallization in polymers , 2002 .

[2]  C. Truesdell,et al.  The Non-Linear Field Theories Of Mechanics , 1992 .

[3]  K. Kannan,et al.  A Thermomechanical Framework for the Transition of a Miscoelastic Liquid to a Viscoelastic Solid , 2004 .

[4]  Arun R. Srinivasa,et al.  Modeling anisotropic fluids within the framework of bodies with multiple natural configurations , 2001 .

[5]  Ilya Prigogine,et al.  Introduction to Thermodynamics of Irreversible Processes , 1967 .

[6]  Arun R. Srinivasa,et al.  On the thermomechanics of materials that have multiple natural configurations , 2004 .

[7]  K. R. Rajagopal,et al.  On thermomechanical restrictions of continua , 2004, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[8]  E. A. Second Report on Viscosity and Plasticity , 1939, Nature.

[9]  Kumbakonam R. Rajagopal,et al.  THERMODYNAMIC FRAMEWORK FOR THE CONSTITUTIVE MODELING OF ASPHALT CONCRETE: THEORY AND APPLICATIONS , 2004 .

[10]  K. Janáček [Introduction to thermodynamics]. , 1973, Ceskoslovenska fysiologie.

[11]  Arun R. Srinivasa,et al.  Inelastic behavior of materials. Part II. Energetics associated with discontinuous deformation twinning , 1997 .

[12]  J. Oldroyd On the formulation of rheological equations of state , 1950, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[13]  W. Voigt,et al.  Ueber innere Reibung fester Körper, insbesondere der Metalle , 1892 .

[14]  Arun R. Srinivasa,et al.  Mechanics of the inelastic behavior of materials. Part II: inelastic response , 1998 .

[15]  Kumbakonam R. Rajagopal,et al.  Chapter 5 – Mathematical Issues Concerning the Navier–Stokes Equations and Some of Its Generalizations , 2005 .

[16]  Y.V.C. Rao An Introduction to Thermodynamics , 2004 .

[17]  Arun R. Srinivasa,et al.  On the thermodynamics of fluids defined by implicit constitutive relations , 2008 .

[18]  Kumbakonam R. Rajagopal,et al.  Mechanical Response of Polymers: An Introduction , 2000 .

[19]  Arun R. Srinivasa,et al.  On the thermomechanics of materials that have multiple natural configurations Part I: Viscoelasticity and classical plasticity , 2004 .

[20]  K. Rajagopal,et al.  A thermomechanical framework for the glass transition phenomenon in certain polymers and its application to fiber spinning , 2002 .

[21]  K. Kannan A note on aging of a viscoelastic cylinder , 2007, Comput. Math. Appl..

[22]  Kumbakonam R. Rajagopal,et al.  On a new interpretation of the classical Maxwell model , 2007 .

[24]  A. Srinivasa Large deformation plasticity and the Poynting effect , 2001 .

[25]  J. Christian CHAPTER 4 – The Thermodynamics of Irreversible Processes , 2002 .

[26]  Christoph Wehrli,et al.  The Derivation of Constitutive Relations from the Free Energy and the Dissipation Function , 1987 .

[27]  William Thomson,et al.  IV. On the elasticity and viscosity of metals , 1865, Proceedings of the Royal Society of London.

[28]  Kumbakonam R. Rajagopal,et al.  A CONSTITUTIVE EQUATION FOR NONLINEAR SOLIDS WHICH UNDERGO DEFORMATION INDUCED MICROSTRUCTURAL CHANGES , 1992 .

[29]  K. Rajagopal,et al.  A thermodynamic frame work for rate type fluid models , 2000 .

[30]  K. Rajagopal,et al.  A continuum model for the creep of single crystal nickel-base superalloys , 2005 .

[31]  P. Glansdorff,et al.  Thermodynamic theory of structure, stability and fluctuations , 1971 .

[32]  Koninklijke Nederlandse Akademie van Wetenschappen Second report on viscosity and plasticity , 1938 .

[33]  K. Rajagopal,et al.  A continuum model for the anisotropic creep of single crystal nickel-based superalloys , 2006 .

[34]  Satish Karra,et al.  Development of three dimensional constitutive theories based on lower dimensional experimental data , 2010, ArXiv.

[35]  G. B. The Dynamical Theory of Gases , 1916, Nature.

[36]  Koninklijke Nederlandse Akademie van Wetenschappen First report on viscosity and plasticity , 1939 .

[37]  Carl Eckart,et al.  The Thermodynamics of Irreversible Processes. IV. The Theory of Elasticity and Anelasticity , 1948 .