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Finite Strain Shape Memory Alloys Modeling - Scuola di Dottorato in ...

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such phenomena as the Bausch<strong>in</strong>ger effect and preferred orientation, which occur asa result of <strong>di</strong>fferent plastic deformation of gra<strong>in</strong>s with <strong>di</strong>fferent orientations,demonstrate the effect of crystal structure on plastic behavior. In s<strong>in</strong>gle crystals forwhich crystallographic slip is assumed to be the only mechanism of plasticdeformation, the material flows through the lattice via <strong>di</strong>slocation motion, while thelattice itself, with the material embedded to it, undergoes elastic deformation androtation. If the <strong>di</strong>screte <strong>di</strong>slocation substructure is ignored, the plastic deformationcan be considered to occur <strong>in</strong> the form of smooth shear<strong>in</strong>g on the slip planes and <strong>in</strong>the slip <strong>di</strong>rections. This cont<strong>in</strong>uum slip model from the pioneer<strong>in</strong>g work of Taylor(1938) was employed and further developed by Hill (1950), Hill and Rice (1972) andAsaro (1983). For a crystal with a s<strong>in</strong>gle slip system denoted by { sm , } withms ⋅ =0 and m = s = 1, this micromechanical description can be illustrated as <strong>in</strong>Fig. 4.1. The unit vectors { sm , } are attached to the lattice, and the plastic flow ischaracterized by the tensor Fpdef<strong>in</strong>ed as:F = 1+ γs⊗m (4.1)pwhere γ is the plastic shear<strong>in</strong>g on the crystallographic slip system def<strong>in</strong>ed by{ sm , }. Furthermore, the total deformation of the crystal is decomposed as:F= FF(4.2)epwhereFpis the part due to the slip only that moves the material through the latticevia <strong>di</strong>slocation motion, while Ferotates and <strong>di</strong>storts the crystal lattice.57

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