At least three invariants are necessary to model the mechanical response of incompressible, transversely isotropic materials

The modelling of off-axis simple tension experiments on transversely isotropic nonlinearly elastic materials is considered. A testing protocol is proposed where normal force is applied to one edge of a rectangular specimen with the opposite edge allowed to move laterally but constrained so that no vertical displacement is allowed. Numerical simulations suggest that this deformation is likely to remain substantially homogeneous throughout the specimen for moderate deformations. It is therefore further proposed that such tests can be modelled adequately as a homogenous deformation consisting of a triaxial stretch accompanied by a simple shear. Thus the proposed test should be a viable alternative to the standard biaxial tests currently used as material characterisation tests for transversely isotropic materials in general and, in particular, for soft, biological tissue. A consequence of the analysis is a kinematical universal relation for off-axis testing that results when the strain-energy function is assumed to be a function of only one isotropic and one anisotropic invariant, as is typically the case. The universal relation provides a simple test of this assumption, which is usually made for mathematical convenience. Numerical simulations also suggest that this universal relation is unlikely to agree with experimental data and therefore that at least three invariants are necessary to fully capture the mechanical response of transversely isotropic materials.

[1]  R. J. Atkin,et al.  An introduction to the theory of elasticity , 1981 .

[2]  P. Saxena,et al.  Altered cardiac collagen and associated changes in diastolic function of infarcted rat hearts. , 2000, Cardiovascular research.

[3]  A. Wineman,et al.  New universal relations for nonlinear isotropic elastic materials , 1987 .

[4]  Michael D. Gilchrist,et al.  Automated Estimation of Collagen Fibre Dispersion in the Dermis and its Contribution to the Anisotropic Behaviour of Skin , 2012, Annals of Biomedical Engineering.

[5]  C. Horgan,et al.  Simple Shearing of Incompressible and Slightly Compressible Isotropic Nonlinearly Elastic Materials , 2010 .

[6]  Gerhard A. Holzapfel,et al.  On planar biaxial tests for anisotropic nonlinearly elastic solids. A continuum mechanical framework , 2009 .

[7]  M. Kawai,et al.  An integrated method for off-axis tension and compression testing of unidirectional composites , 2011 .

[8]  A. Spencer,et al.  Deformations of fibre-reinforced materials, , 1972 .

[9]  C. Truesdell,et al.  Interpretation of adscititious inequalities through the effects pure shear stress produces upon an isotropie elastic solid , 1974 .

[10]  Ivonne Sgura,et al.  Fitting hyperelastic models to experimental data , 2004 .

[11]  J. Whitney,et al.  Tension Buckling of Anisotropic Cylinders , 1968 .

[12]  A. Goriely,et al.  Positive or negative Poynting effect? The role of adscititious inequalities in hyperelastic materials , 2011, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[13]  Alan N. Gent,et al.  Mechanics of rubber shear springs , 2007 .

[14]  M. Destrade,et al.  Simple shear is not so simple , 2012, 1302.2411.

[15]  R. Ogden,et al.  Hyperelastic modelling of arterial layers with distributed collagen fibre orientations , 2006, Journal of The Royal Society Interface.

[16]  J. Humphrey,et al.  Determination of a constitutive relation for passive myocardium: I. A new functional form. , 1990, Journal of biomechanical engineering.

[17]  K. Hayashi,et al.  Mechanical properties of collagen fascicles from the rabbit patellar tendon. , 1999, Journal of biomechanical engineering.

[18]  Cornelius O. Horgan,et al.  Simple shearing of soft biological tissues , 2011, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[19]  R. Rivlin Large elastic deformations of isotropic materials IV. further developments of the general theory , 1948, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[20]  J D Humphrey,et al.  A new constitutive formulation for characterizing the mechanical behavior of soft tissues. , 1987, Biophysical journal.

[21]  Ray W. Ogden,et al.  Nonlinear Elasticity, Anisotropy, Material Stability and Residual Stresses in Soft Tissue , 2003 .

[22]  S. TIMOSHENKO,et al.  An Introduction to the Theory of Elasticity: , 1936, Nature.

[23]  O. H. Yeoh,et al.  A new attempt to reconcile the statistical and phenomenological theories of rubber elasticity , 1997 .

[24]  Julius M. Guccione,et al.  Finite element modeling of mitral leaflet tissue using a layered shell approximation , 2012, Medical & Biological Engineering & Computing.

[25]  C. Horgan,et al.  On the Modeling of Extension-Torsion Experimental Data for Transversely Isotropic Biological Soft Tissues , 2012 .

[26]  N. J. Pagano,et al.  Influence of End Constraint in the Testing of Anisotropic Bodies , 1968 .

[27]  F. París,et al.  Determination of G12 by means of the off-axis tension test.: Part I: review of gripping systems and correction factors , 2002 .

[28]  M. Vannier,et al.  An inverse approach to determining myocardial material properties. , 1995, Journal of biomechanics.

[29]  I. LeGrice,et al.  Shear properties of passive ventricular myocardium. , 2002, American journal of physiology. Heart and circulatory physiology.

[30]  M. Gilchrist,et al.  Surface instability of sheared soft tissues. , 2008, Journal of biomechanical engineering.

[31]  S. Margulies,et al.  A transversely isotropic viscoelastic constitutive equation for brainstem undergoing finite deformation. , 2006, Journal of biomechanical engineering.

[32]  R. Ogden,et al.  A New Constitutive Framework for Arterial Wall Mechanics and a Comparative Study of Material Models , 2000 .

[33]  J. Humphrey,et al.  Determination of a constitutive relation for passive myocardium: II. Parameter estimation. , 1990, Journal of biomechanical engineering.