A thermo-mechanically coupled theory for fluid permeation in elastomeric materials: Application to thermally responsive gels

Abstract An elastomeric gel is a cross-linked polymer network swollen with a solvent, and certain gels can undergo large reversible volume changes as they are cycled about a critical temperature. We have developed a continuum-level theory to describe the coupled mechanical deformation, fluid permeation, and heat transfer of such thermally responsive gels. In discussing special constitutive equations we limit our attention to isotropic materials, and consider a model based on a Flory–Huggins model for the free energy change due to mixing of the fluid with the polymer network, coupled with a non-Gaussian statistical–mechanical model for the change in configurational entropy—a model which accounts for the limited extensibility of polymer chains. We have numerically implemented our theory in a finite element program. We show that our theory is capable of simulating swelling, squeezing of fluid by applied mechanical forces, and thermally responsive swelling/de-swelling of such materials.

[1]  Lallit Anand,et al.  A coupled theory of fluid permeation and large deformations for elastomeric materials , 2010 .

[2]  Quantifying deformation in gel swelling: Experiments and simulations , 2000 .

[3]  Z. Suo,et al.  A theory of coupled diffusion and large deformation in polymeric gels , 2008 .

[4]  M. Boyce,et al.  A three-dimensional constitutive model for the large stretch behavior of rubber elastic materials , 1993 .

[5]  Rui Huang,et al.  A Variational Approach and Finite Element Implementation for Swelling of Polymeric Hydrogels Under Geometric Constraints , 2010 .

[6]  Sanjay Govindjee,et al.  Coupled stress-diffusion: Case II , 1993 .

[7]  Eliot Fried,et al.  Kinetics of thermally induced swelling of hydrogels , 2006 .

[8]  Shu Yang,et al.  Self-Actuated, Thermo-Responsive Hydrogel Valves for Lab on a Chip , 2005, Biomedical microdevices.

[9]  Zhigang Suo,et al.  A finite element method for transient analysis of concurrent large deformation and mass transport in gels , 2009 .

[10]  Lallit Anand,et al.  A constitutive model for compressible elastomeric solids , 1996 .

[11]  M. Gurtin,et al.  The Mechanics and Thermodynamics of Continua , 2010 .

[12]  A. Srinivasa,et al.  Diffusion of a fluid through an elastic solid undergoing large deformation , 2004 .

[13]  J. Dolbow,et al.  Chemically induced swelling of hydrogels , 2004 .

[14]  M. Shibayama,et al.  Kinetics of Volume Phase Transition in Poly(N-isopropylacrylamide-co-acrylic acid) Gels , 1998 .

[15]  Chih-Chang Chu,et al.  Thermoresponsive hydrogel with rapid response dynamics , 2003, Journal of materials science. Materials in medicine.

[16]  D. Owen,et al.  Design of simple low order finite elements for large strain analysis of nearly incompressible solids , 1996 .

[17]  James J Mason,et al.  Preparation and mechanical characterization of a PNIPA hydrogel composite , 2008, Journal of materials science. Materials in medicine.

[18]  Shawn A. Chester Mechanics of amorphous polymers and polymer gels , 2011 .

[19]  Toyoichi Tanaka,et al.  Kinetics of swelling of gels , 1979 .

[20]  M. Biot General Theory of Three‐Dimensional Consolidation , 1941 .

[21]  M. Huggins Some Properties of Solutions of Long-chain Compounds. , 1942 .

[22]  Robin H. Liu,et al.  Functional hydrogel structures for autonomous flow control inside microfluidic channels , 2000, Nature.

[23]  H. G. Schild Poly(N-isopropylacrylamide): experiment, theory and application , 1992 .

[24]  Takehiko Gotoh,et al.  Novel synthesis of thermosensitive porous hydrogels , 1998 .

[25]  P. Flory Principles of polymer chemistry , 1953 .

[26]  J. Dolbow,et al.  A numerical strategy for investigating the kinetic response of stimulus-responsive hydrogels , 2005 .

[27]  Eliot Fried,et al.  A theory for species migration in a finitely strained solid with application to polymer network swelling , 2010 .

[28]  Prashanth K. Vijalapura,et al.  An adaptive hybrid time‐stepping scheme for highly non‐linear strongly coupled problems , 2005 .

[29]  Prashanth K. Vijalapura,et al.  Numerical simulation of coupled‐stress case II diffusion in one dimension , 2003 .

[30]  Jeffrey E. Bischoff,et al.  A new constitutive model for the compressibility of elastomers at finite deformations , 2001 .

[31]  Curtis W. Frank,et al.  A microfluidic actuator based on thermoresponsive hydrogels , 2003 .

[32]  Zhigang Suo,et al.  Using indentation to characterize the poroelasticity of gels , 2010 .

[33]  C. Durning,et al.  Nonlinear swelling of polymer gels , 1993 .

[34]  S. Baek,et al.  Inhomogeneous deformation of elastomer gels in equilibrium under saturated and unsaturated conditions , 2011 .

[35]  Z. Suo,et al.  Force generated by a swelling elastomer subject to constraint , 2010 .

[36]  Rassoul Dinarvand,et al.  The use of thermoresponsive hydrogels for on-off release of molecules , 1995 .

[37]  D. Vesely Diffusion of liquids in polymers , 2008 .

[38]  D. J. Montgomery,et al.  The physics of rubber elasticity , 1949 .

[39]  P. Flory Thermodynamics of High Polymer Solutions , 1941 .

[40]  Simon Champ,et al.  New superabsorbent thermoreversible hydrogels , 2001 .

[41]  Masao Doi,et al.  Introduction to Polymer Physics , 1996 .