Qs. Zheng et If. Collins, THE RELATIONSHIP BETWEEN DAMAGE VARIABLES AND THEIR EVOLUTION LAWS AND MICROSTRUCTURAL AND PHYSICAL-PROPERTIES, Proceedings - Royal Society. Mathematical, physical and engineering sciences, 454(1973), 1998, pp. 1469-1498
Citations number
58
Categorie Soggetti
Multidisciplinary Sciences
Journal title
Proceedings - Royal Society. Mathematical, physical and engineering sciences
The major objective of this paper is to give a rational approach to id
entify the dam age parameters in tensorial form, based on the microstr
ucture of the defects (voids, cavities, microcracks) and the overall p
hysical properties of a solid material. First, the general representat
ions for the effective linear and nonlinear reversible physical proper
ties (e.g. elastic and piezoelectric moduli) of a material representat
ive volume element (RVE) containing a single defect of any shape are i
nvestigated. Second, it is emphasized that the orientation distributio
n functions (ODFs) of shapes, separations, etc., of defects constitute
the dominant and physically measurable signatures of the changing mic
rostructure of a damaged material, by assuming that the matrix behaves
reversibly during damage nucleation and growth. Third, it is shown th
at the ODFs can be expanded as absolutely convergent Fourier series wi
th irreducible tensorial coefficients, and that these infinitely many
irreducible tensorial coefficients constitute the full list of generic
damage variables. Furthermore, to specify any given physical property
, only certain leading tensorial coefficients in these series are need
ed and, therefore: these leading coefficients act as the real damage t
ensors for such a physical property. These physically based damage ten
sors vary significantly from one physical property to another. For exa
mple, it is shown that only the second and fourth tensorial coefficien
ts effect the linear elastic moduli, while only the first and third te
nsorial coefficients are needed in linear piezoelectricity theory. Fin
ally, it is observed from a simple example that the evolution equation
s for these physically based damage tensors normally involve tensorial
terms of higher order than those needed to define the considered phys
ically based damage tensors. Consequently, the evolution equations are
not self-closed.