Simulations
of defects inside copper point the way to making stronger metals
Strong metals have a tendency to be less ductile —
unless the metal happens to be a peculiar form of copper known as nanotwinned
copper. The crystal structure of nanotwinned copper exhibits many
closely-spaced interruptions in an otherwise regular atomic array. These
interruptions, despite being termed ‘defects’, actually increase the metal’s
strength without reducing its ductility, making it attractive for applications
such as semiconductor devices and thin film coatings. However, the relationship
between the properties of these defects and those of the metals containing
defects remains unclear.
Now, Zhaoxuan Wu and co-workers at the A*STAR Institute
for High Performance Computing have now performed a large-scale numerical
simulation that sheds light on this relationship1. The simulation addressed
some of their previous, unexplained experimental data.
In 2009, the researchers had observed that the
strength of nanotwinned copper reached a maximum when the size of the defects
in its crystal structure was about 15 nanometers. When the defects were made
smaller or larger, the copper’s strength decreased. This contradicted the
classical model, which predicted that the metal’s strength would increase
continually as the defect size was reduced.
Wu and co-workers addressed this contradiction by
using a very large-scale molecular dynamics simulation to calculate how a
nanotwinned copper crystal consisting of more than 60 million atoms deforms
under pressure. They observed that its deformation was facilitated by three
types of mobile dislocations in its crystal structure. Significantly, they
found that one of these three types of dislocation, called a 60° dislocation,
interacted with defects in a way that depended on the defect size.
The 60° dislocations were able to pass through small
defects in a continuous manner, creating many new, highly mobile dislocations
that softened the copper. On the other hand, when they encountered large
defects, a three-dimensional dislocation network formed that acted as a barrier
for subsequent dislocation motion, thus strengthening the copper. The
simulation predicted that the critical defect size separating these two regimes
of behavior occurred at 13 nanometers, very close to the experimentally
measured value of 15 nanometers.
The results show that there are many different
deformation mechanisms occurring in nano-structured materials like nanotwinned
copper. Understanding each of them will allow scientists to tune material
properties — as Wu comments: “For example, we could introduce dislocation
barriers to stop their motion, or change defect interface energies to change
how they deform.” Wu adds that the next step for his research team will be to
take into account the diversity in defect sizes within a single material.
The A*STAR-affiliated researchers contributing to
this research are from the Institute
for High Performance Computing
References
- Wu, Z. X., Zhang, Y. W., & Srolovitz, D. J. Deformation
mechanisms, length scales and optimizing the mechanical properties of
nanotwinned metals. Acta Materialia 59, 6890–6900
(2011). | article
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