By T. Abe, T. Tsuta
AEPA '96 presents a discussion board for dialogue on present advancements in plasticity. An emphasis is put on the shut interplay of the theories from macroplasticity, mesoplasticity and microplasticity including their purposes in numerous engineering disciplines reminiscent of stable mechanics, steel forming, structural research, geo-mechanics and micromechanics. those complaints comprise over a hundred and forty papers from the convention together with case reports displaying purposes of plasticity in inter-disciplinary or nonconventional components.
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Extra resources for Advances in Engineering Plasticity and its Applications (AEPA 1996)
Reinforced Plastics & Composites, 14, 588-617. Kausch (1991). Creep failure mechanisms in a particulate-filled epoxy resin. J. ,26, 5534-5542. Hui (1995). On creep of unidirectional fiber composites with fiber damage. ActaMetalletMaterialia, 43, 2615-1623. (1978). Physical Aging of Amorphous Polymers and Other Materials. Elsevier, Amsterdam. The mechanical and physical ageing of semicrystalline polymers:Part 1. Polymer, 28, 1521-1533; Part 2. 1534-1542. (1989) Ditto Part 3, Prediction of long term creep from short time tests, Polymer, 30, 799-814; Part 4, 815-830.
Fig. 9 (111) pole figure showing measured (contours) and calculated ( · , ■ ) recrystallization textures. ( Ο , Δ : indexed by Butler et al (1991). and (ili) with rotation angle about  from the (001) orientation to the (112)[lli] orientation calculated using the Taylor-Bishop-Hill theory are shown in Fig. 11. The contribution of the slip systems to the deformation may be approximated to be proportional to the area under the related shear strain γ - rotation angle Θ curves. 6 where subscripts indicate slip systems shown in Fig.
Among others Ohno and Wang (1993) succeeded in representing the complete, or near, closure of stress-strain hysteresis loops, which is an important feature to simulate ratchetting. They achieved it within the framework of the hardening and dynamic recovery format mentioned above; they assumed that each component of back stress has the critical state of dynamic recovery. This model enables us to simulate ratchetting much more accurately than the Armstrong and Frederick rule. This paper describes characteristics of the Ohno and Wang model mentioned above and its applications to uniaxial, multiaxial and thermal ratchettings as well as to nonproportional deformations without ratchetting.
Advances in Engineering Plasticity and its Applications (AEPA 1996) by T. Abe, T. Tsuta