Applications of tensor functions to the formulation of constitutive equations involving damage and initial anisotropy

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Abstract

In this paper some results of the tensor function theory are applied to the formulation of constitutive equations of isotropic and anisotropic materials in the secondary and tertiary creep stage. The creep process, in its tertiary phase, is characterized by a damage tensor. Because of its microscopic nature, damage has, in general, an anisotropic character even in cases where the material was originally isotropic, i.e. isotropic in its virgin state. Fissure orientation and length cause anisotropic macroscopic behaviour. In the first part of the paper some possible ways of representing constitutive equations involving (initial) anisotropy of the material (e.g. from rolling) and involving anisotropic creep-damage are dealt with. The formulations of such equations are based upon theorems concerning tensor-valued functions. Furthermore, some simplified constitutive equations for more practical use are discussed. The main problem of this part is: to find an irreducible set of tensor generators. Besides the problem of finding such tensor generators it is very important to determine the scalar coefficients in constitutive equations as functions of the invariants and experimental data. The second part of the paper is concerned with the determination of the scalar functions. This can be done by using tensorial interpolation methods as pointed out in detail.

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    The effective stress tensor of anisotropic damage was introduced by definition of different tensorial form of damage parameter to explain damage induced anisotropy. For example, the 2nd rank symmetric damage tensor was proposed by some authors [16,10,17,14]. Transformation of real stress tensor to the effective stress tensor was also carried out by the definition of the fourth rank damage tensor [18,19].

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    This approach finds its limitation when the damage develops in plans of different orientations. Damage representation by second-rank tensors (Vakulenko and Kachanov, 1971; Dragon and Mroz, 1979; Cordebois and Sidoroff, 1979, 1980; Kachanov, 1980; Murakami and Ohno, 1981; Oda, 1983; Betten, 1986; Murakami, 1987; Suaris, 1987; Murakami, 1988, 2012; Chaboche, 1992, 1993; Ladevèze, 1993; Hansen and Schreyer, 1994; Voyiadjis and Kattan, 1996; Desmorat, 2000; Lemaitre et al., 2000; Brünig, 2002, 2003; Lemaitre and Desmorat, 2005; Desmorat and Cantournet, 2007; among others.) : The geometrical properties of the microcracks may be described, in a continuum sense, by a second-rank tensor.

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