Materials Science and Engineering A 410–411 (2005) 413–416
Elevated temperature behavior of SePD materials:
Superplasticity or enhanced ductility?
A.V. Sergueeva
a
, N.A. Mara
a
, R.Z. Valiev
b
, A.K. Mukherjee
a,∗
a
University of California, Chemical Engineering and Material Science Department, Davis, CA 95616, USA
b
Ufa State Aviation Technical University, Institute of Physics of Advanced Materials, 12 Marks Str., Ufa 450000, Russia
Received in revised form 1 March 2005
Abstract
The generated results on superplastic flow (SPF) in materials produced by severe plastic deformation (SePD) have been analyzed. Formation
of sliding surfaces with subsequent cooperative grain boundary sliding (CGBS) has been demonstrated to be a main deformation mechanism of
superplasticity under conditions of microstructural stability. A substantial role of dislocation glide in accommodation processes is shown. When
grain growth is observed during deformation, continuous grain boundary migration prevents formation of slide surfaces and CGBS is restrained.
In this case, deformation of the material is more likely to occur by dislocation or diffusion creep than true SPF despite relatively large strains being
reached.
© 2005 Elsevier B.V. All rights reserved.
Keywords: Severe plastic deformation; Plastic behavior; Superplasticity
1. Introduction
Superplasticity as a phenomenon or an effect can be defined as
the capacity of materials to undergo abnormally large (hundreds
or thousands of a percent) uniform tensile elongations at low flow
stresses which are in order of magnitude lower than those under
the conditions of ordinary plastic deformation and have a high
sensitivity to a change in deformation rate. In general, in order
to understand the nature and origin of deformation mechanisms
at high temperatures, information related to the dependence of
strain rate on stress, temperature and grain size (GS) is essential
and constitutive equations are very helpful in this case. In micro-
crystalline materials (MCM), superplasticity is well established
as a GS dependent phenomenon that can be described by the con-
stitutive equation for elevated temperature crystalline plasticity
[1]:
˙ ε = A
DGb
kT
b
d
p
σ
G
n
(1)
where ˙ ε is the strain rate, D the appropriate diffusivity (grain
boundary (GB) in the case of superplasticity), G the shear mod-
∗
Corresponding author. Tel.: +1 530 752 1776; fax: +1 530 752 9554.
E-mail address: akmukherjee@ucdavis.edu (A.K. Mukherjee).
ulus, b the Burgers vector, k the Boltzmanns constant, T the test
temperature, d the GS, p the GS exponent (usually 2 for lattice
diffusion and 3 for GB diffusion controlled flow), σ the applied
stress and n is stress exponent (n = 1/m, where m is strain rate
sensitivity; n = 2 in the case of superplasticity). This equation
describes behavior has been observed for metals, intermetallics
and ceramics materials. This relationship predicts a shifting of
the optimum strain rate to higher values and/or the optimum
temperatures to lower values with microstructural refinement.
In current investigation, the elevated temperature deforma-
tion behavior of metals and intermetallics subjected to severe
plastic deformation (SePD) was analyzed to establish possible
deformation mechanisms and microstructural effects.
2. Grain size dependence of plasticity
Fig. 1 represents a summary of experimental data on GS
dependence of maximum elongation observed in different SePD
materials tested in tension at optimal conditions. It can be seen
that despite a theoretical prediction for advanced superplasticity
in nanocrystalline materials (NCM), tensile elongation contin-
uously decreases with decreasing GS in microcrystalline range.
In addition, Al-alloys have demonstrated a greater propensity
for SPF than other metals (solid symbols in Fig. 1). But it was
noticed [20] that superplasticity in ultrafine materials is achieved
0921-5093/$ – see front matter © 2005 Elsevier B.V. All rights reserved.
doi:10.1016/j.msea.2005.08.020