Abstract:Defects play a key role in the determination of material properties, especially at small scales. The influence of several kinds of defects (point vacancies, line vacancies and cracks) on the deformation and fracture characteristics of a planar copper grain boundary interface with a 45° lattice misorientation is explored using molecular dynamics simulations and the embedded-atom method. Both tensile and shear modes of interfacial separation are considered. The results show that the crystalline defects can have … Show more
“…This conclusion is analogous to that of the copper interface in Ref. [36]. The level of stress oscillation in all three cases is weaker than that of the pristine interface system, which can be attributed to the decrease in interface rigidity due to the existence of point vacancy defects.…”
Section: Effects Of Point Vacancy Defectssupporting
confidence: 83%
“…The peak stress is nearly half that of a pure copper bicrystal interface in Ref. [36], suggesting that the heterogeneous bonding between Cu and Al is weaker than that of a copper grain boundary interface. Similar to the behaviors of the copper interface, 24 36 an elastic springback stress oscillation associated with vibration of the model is observed after the occurrence of the peak stress at a displacement of about 0.6 nm.…”
Section: Deformation Of a Pristine Interfacementioning
Tensile deformation of a defective Cu/Al interface, which is used as a model system of heterogeneous metal interfaces, is explored using molecular dynamics simulations and compared with the mechanical behavior of copper grain boundaries. Results show that the heterogeneous bonding across the interface is a weaker link of the system during mechanical loading as compared with pure copper grain boundaries. Interfacial ductile fracture is the main mechanical failure mode accompanied by the nucleation and growth of voids near the interfacial region, which differs from the fracture mode of copper grain boundary. Evolution of the microstructures and its dependency on the external loading are examined with the interface models during the deformation process. In some cases of a defective interface, the nucleation of partial dislocation loops is observed and analyzed.
“…This conclusion is analogous to that of the copper interface in Ref. [36]. The level of stress oscillation in all three cases is weaker than that of the pristine interface system, which can be attributed to the decrease in interface rigidity due to the existence of point vacancy defects.…”
Section: Effects Of Point Vacancy Defectssupporting
confidence: 83%
“…The peak stress is nearly half that of a pure copper bicrystal interface in Ref. [36], suggesting that the heterogeneous bonding between Cu and Al is weaker than that of a copper grain boundary interface. Similar to the behaviors of the copper interface, 24 36 an elastic springback stress oscillation associated with vibration of the model is observed after the occurrence of the peak stress at a displacement of about 0.6 nm.…”
Section: Deformation Of a Pristine Interfacementioning
Tensile deformation of a defective Cu/Al interface, which is used as a model system of heterogeneous metal interfaces, is explored using molecular dynamics simulations and compared with the mechanical behavior of copper grain boundaries. Results show that the heterogeneous bonding across the interface is a weaker link of the system during mechanical loading as compared with pure copper grain boundaries. Interfacial ductile fracture is the main mechanical failure mode accompanied by the nucleation and growth of voids near the interfacial region, which differs from the fracture mode of copper grain boundary. Evolution of the microstructures and its dependency on the external loading are examined with the interface models during the deformation process. In some cases of a defective interface, the nucleation of partial dislocation loops is observed and analyzed.
“…14,15 For more extreme conditions exploring high strain rate behaviour, X-FEL beam line experiments, such as those at SLAC in Stanford can be conducted that allow diffraction imaging of impact events at a temporal resolution of y10 214 seconds, in the imaging burst light can only travel few microns. This is more than adequate to explore the interplay between twinning and dislocations under high and medium rate loading where the twin growth velocity is y10 km s 21 .…”
“…16,17,18,19 The value of modelling from atomistic, including quantum mechanical effects, through to crystal level approaches is maturing quickly and has already had a direct impact on industry. This includes fields as diverse as cold dwell fatigue in aerospace titanium alloys, 20,21 the prediction of the magnetic transition in iron 22 and quantitative predictive capability for the elastic field trapping of dislocation loops in metals post irradiation damage 23 and the behaviour of interstitials. 24,25 It is important to recognise that physically based models may also play a critical role in being able to extract any meaningful quantitative data from some of the experimental methods.…”
Section: Role Of Modelling -New 'Art Of the Possible'mentioning
The complexity of adopting new or using existing advanced alloy systems in demanding environments where safety is paramount is highlighted. Of particular importance is the ability to define operative deformation and degradation mechanisms that may limit part life or functionality. With respect to the underlying fundamental material science there is a high degree of commonality between the aero and power generation sectors. The vast array of new experimental and modelling techniques that can be brought to bear on long standing technical challenges offers the potential for a renaissance in materials science. Of particular interest from an industrial context would be the ability to ‘design’ material microstructure and texture optimised for service use manufactured via the most energy and time efficient route. The requirements and potential for progress in this area is summarised with an emphasis on gas turbine and nuclear reactor applications for hcp metals.
“…[10][11][12] Molecular dynamics (MD) simulation, which is promising, has been used widely to describe the fundamental mechanical properties of nanocrystalline materials. 8,[13][14][15] Wang et al 14 studied the influence of defects on mechanical properties of the copper grain boundary interface, and they showed the interfacial behaviors subjected to tensile or shear strain were sensitive to crystalline defects. Spearot et al 15 used MD simulation to study the tensile strength of <100> and <110> tilt copper interfaces, which indicated that the two critical attributions of the interface structure were crystalline in orientation and certain structural units.…”
The failure of the nanoscale metallic interface has raised concerns owing to the effect interfacial amalgamation has on its application in nanoelectronic devices. Single crystal copper [110] and [100], which are set as two components of [110]‖[100] nanocrystalline copper, are used to simulate the interfacial properties using molecular dynamics simulations. Repeated tension and compression cycles show that the two components of the interface can come into contact and separate without interfacial amalgamation. The [110]‖[100] interface could withstand momentary shocks of compression and heat produced by the momentary shocks. This property of the [110]‖[100] interface is dominated by crystalline orientations of interfacial structure, in comparison with [111]‖[100] and [111]‖[110] interfaces under the same conditions.
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