Abstract
Different theoretical interpretations and possible mathematical expressions for the higher-order strain gradient plasticity theory initiated by Aifantis are investigated. These different interpretations of the theory result in different computational procedures. The effects of the orders of finite-element shape functions and the number of Gaussian quadrature points on the qualities of numerical solutions are examined for different formulations.
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Notes
- 1.
In Kuroda and Tvergaard (2010), somewhat different definitions for \(\pmb g^\mathrm {p}\) were used; i.e., \(\pmb g^\mathrm {p}~=~-~\nabla \varepsilon ^\mathrm {p}\) without the inclusion of \(\beta \) for the simplest theory, and \(\pmb g^\mathrm {p}=-l_*^2h\nabla \varepsilon ^\mathrm {p}\) to discuss an alternative formulation (corresponding to Treatment 4Â in the present study) of Fleck-Hutchinson theory (Fleck and Hutchinson 2001), where \(l_*\) is a length-scale parameter. In the present paper, to enable a broader and extended discussion, the more general definition given by Eq. (9.7) is employed.
- 2.
This type of derivation of constitutive relations for the higher-order stresses was presented in the context of gradient crystal plasticity theory (Gurtin 2002). The crystal plasticity version of Eq. (9.14) also appeared in Gurtin (2002). Thermodynamical formulations of crystal plasticity were also discussed in Forest et al. (2002).
- 3.
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Kuroda, M. (2015). Strain Gradient Plasticity: A Variety of Treatments and Related Fundamental Issues. In: Altenbach, H., Matsuda, T., Okumura, D. (eds) From Creep Damage Mechanics to Homogenization Methods. Advanced Structured Materials, vol 64. Springer, Cham. https://doi.org/10.1007/978-3-319-19440-0_9
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