Poromechanics of compressible charged porous media using the theory of mixtures.

Osmotic, electrostatic, and/or hydrational swellings are essential mechanisms in the deformation behavior of porous media, such as biological tissues, synthetic hydrogels, and clay-rich rocks. Present theories are restricted to incompressible constituents. This assumption typically fails for bone, in which electrokinetic effects are closely coupled to deformation. An electrochemomechanical formulation of quasistatic finite deformation of compressible charged porous media is derived from the theory of mixtures. The model consists of a compressible charged porous solid saturated with a compressible ionic solution. Four constituents following different kinematic paths are identified: a charged solid and three streaming constituents carrying either a positive, negative, or no electrical charge, which are the cations, anions, and fluid, respectively. The finite deformation model is reduced to infinitesimal theory. In the limiting case without ionic effects, the presented model is consistent with Blot's theory. Viscous drag compression is computed under closed circuit and open circuit conditions. Viscous drag compression is shown to be independent of the storage modulus. A compressible version of the electrochemomechanical theory is formulated. Using material parameter values for bone, the theory predicts a substantial influence of density changes on a viscous drag compression simulation. In the context of quasistatic deformations, conflicts between poromechanics and mixture theory are only semantic in nature.

[1]  D Pflaster,et al.  A poroelastic finite element formulation including transport and swelling in soft tissue structures. , 1996, Journal of biomechanical engineering.

[2]  Jmrj Jacques Huyghe,et al.  Thermo-Chemo-Electro-Mechanical Formulation of Saturated Charged Porous Solids , 1999 .

[3]  F. Kiil Molecular mechanisms of osmosis. , 1989, The American journal of physiology.

[4]  R. M. Bowen,et al.  Incompressible porous media models by use of the theory of mixtures , 1980 .

[5]  H. Olphen An Introduction to Clay Colloid Chemistry , 1977 .

[6]  John H. Cushman,et al.  A multi-scale theory of swelling porous media: I. Application to one-dimensional consolidation , 1995 .

[7]  Joon B. Park Biomaterials:An Introduction , 1992 .

[8]  G. Lagaly,et al.  H. van Olphen: An Introduction to Clay Colloid Chemistry, 2nd Ed. John Wiley & Sons, New York, London, Sydney, Toronto 1977. 318 Seiten, Preis: £ 15.–, $ 25.– , 1978 .

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

[10]  W. Heidug,et al.  Hydration Swelling of Water-Absorbing Rocks: a Constitutive Model , 1996 .

[11]  M. Biot Theory of finite deformations of porous solids , 1972 .

[12]  V C Mow,et al.  The significance of electromechanical and osmotic forces in the nonequilibrium swelling behavior of articular cartilage in tension. , 1981, Journal of biomechanical engineering.

[13]  Jd Jan Janssen,et al.  Quadriphasic mechanics of swelling incompressible porous media , 1997 .

[14]  D. Drumheller The theoretical treatment of a porous solid using a mixture theory , 1978 .

[15]  W M Lai,et al.  A triphasic theory for the swelling and deformation behaviors of articular cartilage. , 1991, Journal of biomechanical engineering.

[16]  A F Mak,et al.  Numerical simulation of streaming potentials due to deformation-induced hierarchical flows in cortical bone. , 2001, Journal of biomechanical engineering.

[17]  M. Biot Theory of Propagation of Elastic Waves in a Fluid‐Saturated Porous Solid. I. Low‐Frequency Range , 1956 .

[18]  V. Mow,et al.  On the electric potentials inside a charged soft hydrated biological tissue: streaming potential versus diffusion potential. , 2000, Journal of biomechanical engineering.

[19]  A. Cheng,et al.  Fundamentals of Poroelasticity , 1993 .

[20]  R. de Boer,et al.  Theory of Porous Media , 2020, Encyclopedia of Continuum Mechanics.

[21]  M. Biot,et al.  THE ELASTIC COEFFICIENTS OF THE THEORY OF CONSOLIDATION , 1957 .

[22]  A. Cemal Eringen,et al.  A continuum theory of swelling porous elastic soils , 1994 .

[23]  S. Cowin,et al.  A case for bone canaliculi as the anatomical site of strain generated potentials. , 1995, Journal of biomechanics.

[24]  Theo H Smit,et al.  A Case for Strain‐Induced Fluid Flow as a Regulator of BMU‐Coupling and Osteonal Alignment , 2002, Journal of bone and mineral research : the official journal of the American Society for Bone and Mineral Research.

[25]  Olivier Coussy,et al.  Mechanics of porous continua , 1995 .

[26]  C. J. Davidson,et al.  Borehole Stability in Shales , 1994 .

[27]  Maurice A. Biot,et al.  Generalized Theory of Acoustic Propagation in Porous Dissipative Media , 1962 .

[28]  V. Mow,et al.  A triphasic analysis of negative osmotic flows through charged hydrated soft tissues. , 1997, Journal of biomechanics.

[29]  Theo H Smit,et al.  Estimation of the poroelastic parameters of cortical bone. , 2002, Journal of biomechanics.

[30]  R de Boer,et al.  Theory of Porous Media: Highlights in Historical Development and Current State , 2000 .

[31]  M. Biot Theory of Propagation of Elastic Waves in a Fluid-Saturated Porous Solid. II. Higher Frequency Range , 1956 .

[32]  J. Israelachvili Intermolecular and surface forces , 1985 .

[33]  Walter Noll,et al.  The thermodynamics of elastic materials with heat conduction and viscosity , 1963 .

[34]  J. Rice,et al.  Some basic stress diffusion solutions for fluid‐saturated elastic porous media with compressible constituents , 1976 .

[35]  Stephen C. Cowin,et al.  Anisotropic poroelasticity: fabric tensor formulation , 2004 .

[36]  G. Cochran,et al.  A comparative analysis of streaming potentials in vivo and in vitro , 1992, Journal of orthopaedic research : official publication of the Orthopaedic Research Society.