A relation between strain and stress, which is satisfied by transversely hemitropic hyperelastic materials for all finite deformations, is shown to characterize completely this symmetry class.
Get full access to this article
View all access options for this article.
References
1.
[1] Beatty, M. F.: Topics in finite elasticity: Hyperelasticity of rubber, elastomers, and biological tissues-with examples. Appl. Mech. Rev., 40(12), 1699-1734 (1987).
2.
[2] Beatty, M. F.: A class of universal relations in isotropic elasticity theory. J. Elasticity, 17, 113-121 (1987).
3.
[3] Pucci, E. and Saccomandi, G.: Universal relations in continuum mechanics. Cont. Mech. Thermodynamics. forthcoming.
[6] Blume, J. A.: Elastic materials with coincident principal stress and strain axes. J. Elasticity, 35, 275-280 (1994).
7.
[7] Vianello, M.: Optimization of the stored energy and coaxiality of strain and stress in finite elasticity. J. Elasticity, 44, 193-202 (1996).
8.
[8] Gurtin, M. E.: An Introduction to Continuum Mechanics, Academic Press, New York, 1981.
9.
[9] Xiao, H.: General irreducible representations to constitutive equations of elastic crystals and transversely isotropic elastic solids. J. Elasticity, 39, 47-73 (1995).
10.
[10] Beatty, M. F.: A class of universal relations for constrained isotropic materials. Acta Mechanica, 80, 299-312 (1989).
11.
[11] Pucci, E., Saccomandi, G.: Universal relations in constrained elasticity. Mathematics & Mechanics of Solids, 1, 207-217 (1996).