What Is Superplastic Deformation?

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It is tensile deformation process where alloys undergo plastic deformation without formation of neck and give rise to high percentage of elongation. It’s given by a constitutive equation. σ=Kε ̇m where σ is the true flow stress, k is a constant and ε ̇ is strain rate and m is the stain rate of sensitivity. Stain rate sensitivity should be greater than .33 for achieving superplastic deformation. But, for most of metals and alloys the m value is less than 0.2 that is this is why this behavior is not achieved easily for most of metals and alloys. The major area of superplastic behavior includes in metals, ceramics, intermetallic and composites. For making it cost effective and near net shape forming process for commercial applications, extensive …show more content…

At the deformation temperature the grains are highly unstable so grain growth is major problem and that can be solved by the presence of second phase. Shape, size and distribution of second phase play important role for controlling cavitation and growth during deformation [6]. Maehara has shown elongation of around 2000% at a stain rate of 2×10-3s-1 in the temperature range of 950-1000°C. He proposed different mechanism for in this type of case. The presence of hard particles can lead to recrystallization in soft matrix. The σ phase acts as heterogeneous nucleation sites for recrystallization. Soft particles in hard matrix are not beneficial but reverse of this can be advantageous for superplasticity provided optimum quantity of second phase is maintained for …show more content…

Grain boundary sliding is dominant mechanism in superplasticity, high angle grain boundary is preferred over lower angle grain boundary. Equiaxed grains show better superplasticity than that of elongated grain; the grains along the transverse direction is fine but has limited superplasticity when tested along the longitudinal direction. The direction perpendicular to longitudinal direction i.e. transverse direction has poor elongation due to problem of cavitation; strain accommodation is difficult in the case of textured grain [6]. We know that m= ln σ/lnε ̇. Dependency of the value of m on strain rate is such that the m and ε ̇ curve has a dome-like shape. The maximum value mmax corresponds to the optimum strain rate ε ̇ optimal for superplastic deformation for the given average grain size and temperature of deformation. The region II could be divided into region II (a) (left of the maximum) and II (b) (right of the maximum). This is because physical mechanisms operating in the two regions are different. Also, in region II (a), an increase in strain rate increases the m value, while in region II (b), a strain rate increase will decrease the m value. Evidently, the necking resistance in the two regions resulting from such strain rate changes would be different [6]. The value m depends upon a number of factors: strain, strain rate, structure

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