D. Elata et Mb. Rubin, A NEW REPRESENTATION FOR THE STRAIN-ENERGY OF ANISOTROPIC ELASTIC-MATERIALS WITH APPLICATION TO DAMAGE EVOLUTION IN BRITTLE MATERIALS, Mechanics of materials, 19(2-3), 1995, pp. 171-192
In this paper, we develop a new representation of the strain energy of
an elastic material using twenty-one scalar measures of strain. These
measures are associated with material line elements which are directe
d along the six axes of symmetry of a regular icosahedron, and they in
clude: six measures of axial strain and fifteen measures of the angula
r strain. When the strain energy is a quadratic function of strain, th
is representation yields twenty-one elastic moduli which naturally sep
arate into only two physically different types. This is in contrast to
the five physical types of moduli associated with the common rectangu
lar Cartesian representation of the stiffness tenser. By formulating e
volution equations for the elastic moduli, we describe general changes
in the elastic state of a brittle material. Due to the physical natur
e of these moduli, we anticipate that the evolution equations will hav
e simplifying features when expressed in terms of the new representati
on of the strain energy presented here. In general, these evolution eq
uations are restricted by sufficient conditions which ensure that the
change in the elastic state is a dissipative process in the sense that
the second law of thermodynamics is satisfied. It is shown that not a
ll changes of the elastic state can be interpreted as damage evolution
, even if they are dissipative and cause reductions of the magnitudes
of the twenty-one moduli. To ensure damage evolution, we propose an ad
ditional restriction on the strain energy. Furthermore, a simple modif
ication of the strain energy is introduced to model the effect of crac
k closure. Specific equations for damage evolution which satisfy all n
ecessary restrictions are presented. These equations characterize dama
ge evolution in a material that exhibits a transition from an isotropi
c to an anisotropic elastic state. Examples are considered which show
physically reasonable brittle material response.