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Scientific Achievement A reactive, dynamic charge interatomic potential for TiC and Ti has been developed within the framework of the third generation charge optimized many-body (COMB3) potential. Significance and Impact These findings provide new insights into the generation of misfit dislocations at semi-coherent interfaces and carbide-derived carbons with residual Ti. Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations Liang, T.; Ashton, M.; Choudhary, K.; Zhang, D.; Fonseca, A. F.; Revard, B. C.; Hennig, R. G.; Phillpot, S. R.; Sinnott, S. B., “Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations”. J. Phys. Chem. C (2016), 120, 12530-12538. Research Details Structure of coherent and semi-coherent interfaces formed between close-packed TiC (111) and Ti (0001) is investigated using geometry optimization and classical MD simulations. Work of adhesion energies for coherent interfaces is calculated and compared with the DFT predictions. For relaxed semicoherent interfaces, a 2D misfit dislocation network is predicted that divides the interface into hexagonal hcp-like regions, fcc-like triangles, and smaller triangular node regions after annealing at 500 K. The semi-coherent interface is predicted to be the most stable interface with a larger work of adhesion than the “ideal” Ti-HCP coherent interface.

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Page 1: Properties of Ti/TiC Interfaces from Molecular Dynamics ...efrc.gatech.edu › sites › default › files › images › ...Properties of Ti/TiC Interfaces from Molecular Dynamics

Scientific Achievement A reactive, dynamic charge interatomic potential for TiC and Ti has been developed within the framework of the third generation charge optimized many-body (COMB3) potential.Significance and ImpactThese findings provide new insights into the generation of misfit dislocations at semi-coherent interfaces and carbide-derived carbons with residual Ti.

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

Liang, T.; Ashton, M.; Choudhary, K.; Zhang, D.; Fonseca, A. F.; Revard, B. C.; Hennig, R. G.; Phillpot, S. R.; Sinnott, S. B., “Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations”. J. Phys. Chem. C (2016), 120, 12530-12538.

Research Details– Structure of coherent and semi-coherent interfaces formed

between close-packed TiC (111) and Ti (0001) is investigated using geometry optimization and classical MD simulations.

– Work of adhesion energies for coherent interfaces is calculated and compared with the DFT predictions.

– For relaxed semicoherent interfaces, a 2D misfit dislocation network is predicted that divides the interface into hexagonal hcp-like regions, fcc-like triangles, and smaller triangular node regions after annealing at 500 K.

– The semi-coherent interface is predicted to be the most stable interface with a larger work of adhesion than the “ideal” Ti-HCP coherent interface.

Presenter
Presentation Notes
Surfaces of TiC and TiC/Ti interfaces have attracted a substantial amount of attention due to the crucial roles they play in a wide range of applications such as coating materials, thin films for electronic devices, constituent materials for composites, structural components in aerospace and military applications, and as raw materials to produce carbide derived carbon. In this work, the structure of coherent and semicoherent interfaces formed between close-packed TiC (111) and Ti (0001) is investigated in classical molecular dynamics simulations. The forces on the atoms in the simulations are determined using a newly developed TiC potential under the framework of the third-generation charge optimized many-body (COMB3) suite of potentials. The work of adhesion energies for the coherent interfaces is calculated and compared with the predictions of density functional theory calculations. In the case of relaxed semicoherent interfaces, a two-dimensional (2D) misfit dislocation network is predicted to form that separates the interface into different regions in which the positions of the atoms are similar to the positions at the corresponding coherent interfaces. After the interface is annealed at an elevated temperature, the climb of edge dislocations is activated which modifies the 2D misfit dislocation network and increases the work of adhesion. These findings can be used as inputs for sequential larger simulation models to understand and predict the macroscopic properties of TiC/Ti interfaces.
Page 2: Properties of Ti/TiC Interfaces from Molecular Dynamics ...efrc.gatech.edu › sites › default › files › images › ...Properties of Ti/TiC Interfaces from Molecular Dynamics

X

Y

b) Top view

C-FCC C-HCP C-OT

Ti-HCP Ti-FCC Ti-OT

Ti

TiCX

Z

a) Side view

Tiint

Cint

TiTiC

TiTi

Ti2nd

ab

c

a

ba

c

b

b

a

TiC/Ti coherent interfacesTiC : dTi-Ti = 3.05 ÅTi (hcp): dTi-Ti = 2.93 Å

Lattice mismatch:4%

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

Page 3: Properties of Ti/TiC Interfaces from Molecular Dynamics ...efrc.gatech.edu › sites › default › files › images › ...Properties of Ti/TiC Interfaces from Molecular Dynamics

Interface dint (Å) Wad (J/m2)DFT COMB DFT COMB

C-FCC 1.1 0.9 12.4 11.58C-HCP 1.3 1.1 10.5 5.70C-OT 1.8 2.0 6.9 1.36

Ti-HCP 2.5 2.5 4.0 1.86Ti-FCC 2.5 2.5 4.0 1.83Ti-OT 2.8 2.8 3.1 1.20

Ti

TiC

Tiint

Cint

TiTiC

TiTi

Ti2nd

Coherent interfaces

Semi-coherent TiC // Ti interfaces

Strain is released by introducing misfit dislocations

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

Page 4: Properties of Ti/TiC Interfaces from Molecular Dynamics ...efrc.gatech.edu › sites › default › files › images › ...Properties of Ti/TiC Interfaces from Molecular Dynamics

Ti

Ti-term

TiC

Tiint

TiTi

Ti2nd

Cint

Ti-termination TiC//Ti interface

Semi-coherent TiC // Ti interfaces

Extra Ti atoms relative to TiC, misfit dislocations on

each of the directions within the plane of the

interface

25x25 TiC // 26X26 Ti 0% Lattice mismatch

Tiint, TiTi, Ti2nd

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

Page 5: Properties of Ti/TiC Interfaces from Molecular Dynamics ...efrc.gatech.edu › sites › default › files › images › ...Properties of Ti/TiC Interfaces from Molecular Dynamics

Semi-coherent Ti-terminated Interfaces – As-built132.11 Å

76.2

7 Å

hcp-like fcc-likenode

TiC

Ti

TiintTiTiTi2nd

X

Y

25x25 TiC // 26X26 Ti

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

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Disregistry at semi-coherent interface

TiintTiTiTi2n

d

44.04 Å

Reference: real-time coherent interface

As-built: infinitesimal misfit dislocations

X

L=66.05 ÅAs-built: infinitesmal disregistry

Y

Relaxed interface Burger’s vector

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

Page 7: Properties of Ti/TiC Interfaces from Molecular Dynamics ...efrc.gatech.edu › sites › default › files › images › ...Properties of Ti/TiC Interfaces from Molecular Dynamics

66.05 Å

X

Y]0211[

31

]0011[31

]0101[31

]1102[31

]0101[31 ]1021[

31

fcc-likehcp-likenode

TiintTiTiTi2nd

Misfit dislocation accommodation at relaxed interfaceWork of separation2D misfit dislocation network

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

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8

Work of separation2D misfit dislocation network

Charge distribution at interfaces Work of adhesion

Accommodations by misfit dislocations lead the semicoherent interface to be the most stable with

a work of adhesion that is 0.09 J/m2 larger than the “ideal” Ti-HCP

coherent interface

Properties of Ti/TiC Interfaces from Molecular Dynamics Simulations

Misfit dislocation accommodation after annealing at 500 K