Abstract

The interfacial mechanics and electrical properties of SiC reinforced copper matrix composites were studied via the first principles method. The work of adhesion (Wad) and the interfacial energies were calculated to evaluate the stabilities of the SiC/Cu interfacial models. The carbon terminated (CT)-SiC/Cu interfaces were predicted to be more stable than those of the silicon terminated (ST)-SiC/Cu from the results of the Wad and interfacial energies. The interfacial electron properties of SiC/Cu were studied via charge density distribution, charge density difference, electron localized functions and partial density of the state. Covalent C–Cu bonds were formed based on the results of electron properties, which further explained the fact that the interfaces of the CT-SiC/Cu are more stable than those of the ST-SiC/Cu. The interfacial mechanics of the SiC/Cu were investigated via the interfacial fracture toughness and ultimate tensile stress, and the results indicate that both CT- and ST-SiC/Cu interfaces are hard to fracture. The ultimate tensile stress of the CT-SiC/Cu is nearly 23 GPa, which is smaller than those of the ST-SiC/Cu of 25 GPa. The strains corresponding to their ultimate tensile stresses of the CT- and ST-SiC/Cu are about 0.28 and 0.26, respectively. The higher strains of CT-SiC/Cu indicate their stronger plastic properties on the interfaces of the composites.

Highlights

  • The partial density of state (PDOS) of other carbon terminated (CT)-6HSiC(0001)/Cu(111) and silicon terminated (ST)-6H-SiC(0001)/Cu(111) interfacial models had similar results to those obtained by CT-HCP(a) and ST-HCP(a), and they can be seen in Figures S7 to S8

  • (1) The work adhesion and interfacial energies indicate that the CT-SiC(0001)/Cu(111)

  • (2) The charge density distribution, charge density difference, electron localization function and PDOS were calculated to investigate the electronic properties of 6HSiC(0001)/Cu(111), and the results indicate that covalent C-Cu bonds are formed at the

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Summary

Computational Details

To construct the 6H-SiC/Cu heterogeneous interfacial models, (0001) and (111) crystal surfaces were utilized to build the SiC, Cu slab and SiC/Cu composites models, respectively. Along the c axis directo meet the interior features of SiC and Cu bulks. Along the c axis direction for tionSiC forand theCu. Å vacuum layer to was added the to eliminate the the slab, a 15 Åslab, vacuum was added eliminate interactions interactions betweenatoms. Forconsidering the sake ofall considering allof possibetween the surface the sake of possibilities the bilities interfaces, of the SiC/Cu interfaces, different of stacking. SiC and different atomic terminations (CT) and silicon terminated atomic terminations (carbon terminated (carbon (CT) andterminated silicon terminated (ST)).

The played in Figure of
Bulk Properties
Method
Interfacial and Surface Energy
Charge density interfacial of all types of 6HFigure
Charge
Electron
Partial
Interfacial Mechanical Properties
Ultimate Tensile Strength
Conclusions
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