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Rank one plus a null-Lagrangian is an inherited property of two-dimensional compliance tensors under homogenisation

Published online by Cambridge University Press:  14 November 2011

Yury Grabovsky
Affiliation:
Department of Mathematics, University of Utah, Salt Lake City, UT 84102, U.S.A.
Graeme W. Milton
Affiliation:
Department of Mathematics, University of Utah, Salt Lake City, UT 84102, U.S.A.

Abstract

Assume that the local compliance tensor of an elastic composite in two space dimensions is equal to a rank-one tensor plus a null-Lagrangian (there is only one symmetric one in two dimensions). The purpose of this paper is to prove that the effective compliance tensor has the same representation: rank-one plus the null-Lagrangian. This statement generalises the wellknown result of Hill that a composite of isotropic phases with a common shear modulus is necessarily elastically isotropic and shares the same shear modulus. It also generalises the surprising discovery of Avellaneda et al. that under a certain condition on the pure crystal moduli the shear modulus of an isotropic polycrystal is uniquely determined. The present paper sheds light on this effect by placing it in a more general framework and using some elliptic PDE theory rather than the translation method. Our results allow us to calculate the polycrystalline G-closure of the special class of crystals under consideration. Our analysis is contrasted with a two-dimensional model problem for shape-memory polycrystals. We show that the two problems can be thought of as ‘elastic percolation’ problems, one elliptic, one hyperbolic.

Type
Research Article
Copyright
Copyright © Royal Society of Edinburgh 1998

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References

1Avellaneda, M., Cherkaev, A. V., Gibiansky, L. V., Milton, G. W. and Rudelson, M.. A complete characterization of the possible bulk and shear moduli of planar polycrystals. J. Mech. Phys. Solids 44 (1996), 1179–218.Google Scholar
2Avellaneda, M. and Milton, G. W.. Optimal bounds on the effective bulk modulus of polycrystals. SIAM J. Appl. Math. 49 (1989), 824–37.CrossRefGoogle Scholar
3Bensoussan, A., Boccardo, L. and Murat, F.. Homogenization of elliptic equations with principal part not in divergence form and hamiltonian with quadratic growth. Comm. Pure Appl. Math. 39 (1986), 769805.CrossRefGoogle Scholar
4Bensoussan, A., Lions, J. L. and Papanicolaou, G.. Asymptotic analysis of periodic structures (Amsterdam: North-Holland, 1978).Google Scholar
5Bergman, D. J.. Eactly solvable microscopic geometries and rigorous bounds for the complex dielectric constant of a two-component composite material. Phys. Rev. Lett. 44 (1980), 1285–7.Google Scholar
6Bhattacharya, K. and Kohn, R. V.. Elastic energy minimization and the recoverable strains of polycrystalline shape-memory materials. Arch. Rational Mech. Anal. 139 (1997), 99180.Google Scholar
7Cherkaev, A. V. and Gibiansky, L. V.. Coupled estimates for the bulk and shear moduli of a twodimensional isotropic elastic composite. J. Mech. Phys. Solids 41 (1993), 937–80.Google Scholar
8Cherkaev, A. V., Kurie, K. A. and Milton, G. W.. Invariant properties of the stress in plane elasticity and equivalence classes of composites. Proc. Roy. Soc. London Ser. A (1992), 438 (1992), 519–29.Google Scholar
9Francfort, G. A. and Milton, G. W.. Sets of conductivity and elasticity tensors stable under lamination. Comm. Pure Appl. Math. 47 (1994), 257–79.Google Scholar
10Francfort, G. A. and Tartar, L.. Comportement effectif d'un melange de matériaux élastiques isotropes ayant le même module de cisaillement. C. R. Acad. Sci. Paris Sér. I 312 (1991), 301–07.Google Scholar
11Grabovsky, Y.. Bounds and extremal microstructures for two-component composites. A unified treatment based on the translation method. Proc. Roy. Soc. London Ser. A 452 (1996), 945–52.Google Scholar
12Grabovsky, Y. and Kohn, R. V.. Microstructures minimizing the energy of a two phase elastic composite in two space dimensions. I: the confocal ellipse construction. J. Mech. Phys. Solids 43 (1995), 933–47.Google Scholar
13Grabovsky, Y. and Kohn, R. V.. Microstructures minimizing the energy of a two phase elastic composite in two space dimensions. II: the Vigdergauz microstructure. J. Mech. Phys. Solids 46 (1995), 949–72.Google Scholar
14Hill, R.. Elastic propertiess of reinforced solids: Some theoretical principles. J. Mech. Phys. Solids 11 (1963), 357–72.Google Scholar
15Hill, R.. Theory of mechanical properties of fibre-strengthened materials. I. Elastic behaviour. J. Mech. Phys. Solids 12 (1964), 199212.Google Scholar
16Lurie, K. A. and Cherkaev, A. V.. Exact estimates of conductivity of composites formed by two isotropically conducting media taken in prescribed proportion. Proc. Roy. Soc. Edinburgh Sect. A 99 (1984), 7187.CrossRefGoogle Scholar
17Lurie, K. a. and Cherkaev, A. V.. G-closure of some particular sets of admissible material characteristics for the problem of bending of thin plates. J. Optim. Theory Appl. 42 (1984), 305–16.CrossRefGoogle Scholar
18Lurie, K. A., Cherkaev, A. V. and Fedorov, A. V.. On the existence of solutions to some problems of optimal design for bars and plates. J. Optim. Theory Appl. 42 (1984), 247–81.Google Scholar
19Milton, G. W.. Bounds on complex dielectric constant of a composite material. Appl. Phys. Lett. 37 (1980), 300–02.CrossRefGoogle Scholar
20Milton, G. W.. Bounds on the complex permittivity of a two-component composite material. J. Appl. Phys. 52 (1981), 5286–93.CrossRefGoogle Scholar
21Milton, G. W.. Effective moduli of composites: exact results and bounds (Preprint).Google Scholar
22Tartar, L.. Estimation fines des coefficients homogénéisés. In Ennio de Giorgi's Colloquium, ed. Kree, P., 168–87 (London: Pitman, 1985).Google Scholar
23Vigdergauz, S. B.. Three-dimensional grained composites of extreme thermal properties. J. Mech. Phys. Solids 42 (1994), 729–40.Google Scholar
24Vigdergauz, S. B.. Rhombic lattice of equi-stress inclusions in an elastic plate. Quart. J. Mech. Appl. Math. 49 (1996), 565–80.Google Scholar
25Zhikov, V. V.. Estimates for the homogenized matrix and the homogenized tensor. Russian Math. Surveys 46 (1991), 65136.Google Scholar