Toward a Field Theory for Elastic Bodies
Undergoing Disarrangements

Luca Deseri
Departimento di Ingegneria
Universitdi Ferrara
44100 Ferrara, Italy


David Owen
Carnegie Mellon University
Department of mathematical Sciences
Pittsburgh, PA 15213

Abstract Structured deoformations are used to refine the basic ingredients of continuum field theories and to derive a syste of field equations for elastic bodies undergoing submacroscopically smooth genmetrical changes as well as submacroscopically non-smooth geometrical changes (disarrangements). The constitutive assumptions employed in this derivation permit the body to store energy as well as to dissipate energy in smooth dynamical processes. Only one non-classical field $G$, the deformation without disarrangements, appears in the field equations, and a consistency relation based on a decomposition of the Piola-Kirchhoff stress circumvents the use of additional balance laws orphenomenological evolution laws to restrict $G$. The field equations are applied to an elastic body whose free energy depends only upon the volume fraction for the structured deformation. Existence is established of two universal phases, a spherical phase and an elongated phase, whose volume fractions are $(1 - \gamma_0)^3$ and $(1-\gamma_0)$ respectively, with $\gamma_) := (\sqrt{5} -1)/2$ the ``golden mean.''

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