• 기계저널
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• 제57권6호
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• pp.42-46
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• 2017

이 글에서는 거시소재와 나노소재의 소성 거동이 상이한 이유에 대해 간략히 논하고, 전산역학을 이용한 금속나노소재의 소성 변형 메커니즘 연구를 면심입방 소재의 예를 통해 소개하고자 한다.

• 한국진공학회지
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• 제11권1호
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• pp.59-67
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• 2002

본 연구에서는 분자동력학 시뮬레이션을 이용하여 구리 나노와이어의 구조적 특성에 관하여 연구하였다. 매우 가는 구리 나노와이어의 구조는 면심입방격자 구조와는 다른 원통형 다중 껍질 구조를 가지며 상온에서 안정한 구조를 유지하였다. 원통형 다중껍질 나노기둥 및 나노와이어 확장 변형에 따른 장력의 변화에 관한 연구에서 오각형 NLC(needle-like crystal) 구조가 관찰되었다. 오각형 NLC 나노와이어 구조의 특성은 기본구성단위가 면심입방격자 구조이므로 안정된 구조라는 것을 연구하였다.

• 한국결정학회지
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• 제13권1호
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• pp.36-40
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• 2002

중성자회절법을 이용하여 여러 다른 조건으로 열처리한 (Fe/sub 0.61/Ni/sub 0.39/)₃V 합금 분말시료의 장거리 규칙도를 측정하여 규칙-불규칙 상전이의 정도를 조사하였다. 조사 결과 680℃-94 h 열처리 시료는 완전 불규칙 상태로 상전이가 발생하지 않았으며 면심입방구조를 보였다. T < 640℃의 조건에서 열처리한 시료들은 모두 장거리 규칙도 0 < S < 1으로 면심입방구조의 일부가 단순입방구조로 상전이 함을 보여주었다. 또한 Cowley의 S-T/T/sub c/ 관계식으로부터 465℃-144 h 으로 열처리한 시료가 열평형상태에 가장 근접하였음을 확인하였다

• 한국표면공학회지
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• 제31권3호
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• pp.151-156
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• 1998

코발트계 비정질 합금을 여러 온도 구간 및 시간에 대해서 열처리하며 표면 결정화 현상이 자기 이방성에 미치는 영향을 탐구하였다. 자기 이방성은 비정질 표면의 결정 구조에 민감한 변화를 보였는데 면심입방점 코발트에 많은 결함이 존재할 경우 자기이방성이 최대치를 나타내였다.

• 대한화학회지
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• 제35권4호
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• pp.324-328
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• 1991

$Li_2SO_4$를 기질로 한 Li$_2SO_4-CaSO_4$4 계를 합성하여 상온에서 700$^{\circ}C$까지의 온도구간에서 구조와 전도성을 연구하였다. CaSO$_4$의 몰비가 5${\%}$ 이상일 경우 Li$_2SO_4-CaSO_4$는 고용체를 형성하지 않음을 규명하였다. 치환되는 Ca$^{2+}$ 이온에 의해 단사정계에서 면심입방으로의 전이온도는 다소 낮아졌다. 단사정계의 전도도는 Ca$^{2+}$ 치환에 의해 생성되는 Li 공위에 의해 증가되나 면심입방구조의 전도도는 Ca$^{2+}$ 치환에 별 영향을 받지 않았다.

• 대한기계학회논문집A
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• 제32권12호
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• pp.1047-1054
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• 2008

In this paper, the molecular dynamics (MD) simulations are performed with single-crystal copper blocks under simple shear and simple tension to investigate the effect of size and crystal orientation. There are many variances to give influences such as deformation path, temperature, specimen size and crystal orientation. Among them, the crystal orientation has a primary influence on the volume averaged stress. The numerical results show that the volume averaged shear stress decreases as the specimen size increases and as the crystal orientation changes from single to octal. Furthermore, the Schmid factor and yield stress for crystal orientation are evaluated by using the MD simulation on the standard triangle of stereographic projection.

• 한국정밀공학회지
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• 제15권6호
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• pp.124-138
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• 1998

Particles reinforced MMCs have many advantages over monolithic metals including a higher specific modulus, higher specific strength, better properties at elevated temperatures and better wear resistance. SiC$_p$/A16061 composites have good results in its mechanical properties. This work investigates SiC$_p$/A16061 composites in the microscopic view and compares the analytical results with the experimental ones. The discrepancy of the material properties between the reinforced particle, SiC$_p$, and the matrix material, A16061 appears to be so significant. Especially the coefficient of thermal expansion(CTE) of A16061 is 5 times larger than that of SiC$_p$. Thermal residual stress in MMCs is induced at high temperatures. The shape of particle is various but the theoretical model is not able to consider the nonuniform shape. Particle distribution is not homogeneous in experimental specimen. However, it is assumed to be homogeneous in simulation model. The shapes of particles are assumed to be not only perfect global but hexahedral shapes. The types of particle distribution are two - simple cubic array(SC array) and face-centered cubic array(FCC array).

• 한국정밀공학회지
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• 제17권6호
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• pp.199-209
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• 2000

Particles reinforced MMCs have higher specific modulus, higher specific strength, better properties at elevated temperatures and better wear resistance than monolithic metals. But the coefficient of thermal expansion(CTE) of Al6061 is 5 times larger than that of SiCp. The discrepancy of CTE makes some residual stresses inside of MMCs. This work investigates Si$C_p$/Al6061 composites at high temperatures in the microscopic view by three-dimensional elasto-plastic finite element analyses and compares the analytical results with the experimental ones. The theoretical model is not able to consider the nonuniform shape of particle. So the shape of particle is assumed to be perfect global shape. And also particle distribution is not homogeneous in experimental specimen. It is assumed to be homogeneous in simulation model. The type of particle distribution is face-centered cubic array(FCC array). Furthermore, non-homogeneous distribution is modeled by combination of several volume fractions.

• 대한기계학회논문집A
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• 제32권3호
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• pp.250-257
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• 2008

We calculate the variation of the surface stresses according to uniaxial and biaxial strains in face-centered cubic (FCC) metals. In our study, three mainly observed free surfaces of seven representative FCC metals are considered. Employed method is molecular mechanics, in which the interaction of atoms is described by empirical interatomic potentials. As uniaxial strain increases to tensile direction, the surface stresses on {100} and {110} free surfaces decrease monotonously, while those on {111} surface increase. These tendencies are the same regardless of the species of metals and interatomic potentials employed. However, when the system is under biaxial strain, surface stresses change different according to the surface directions, the species of metals, and even interatomic potentials. On {100} and {111} surfaces, heavy metals (Pt, Au) show the opposite variation to light metals (Ni, Cu). In the cases of Pd and Ag, the surface stresses reveal the opposite tendency, depending on interatomic potentials used.

• 한국세라믹학회지
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• 제28권11호
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• pp.878-884
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• 1991

The mobility and diffusivity in an edge dislocation in an FCC crystal formed by the removal of one half of a (100) plane were evaluated in an applied field by analyzing a vacancy tight binding model using Stark's matrix technique. A model of an edge dislocation in an FCC crystal was constructed for a [100] Burgers vector where vacancy transport along the edge dislocation in an FCC crystal was constructed for a [100] Burgers vector where vacancy transport along the edge of the extrac half plane of ions was considered. The model considered a tight binding approximation of the vacancy to the compressed region of the core and carried the calculation to the limit of an infinite length of dislocation. The diffusivity and the ratio of mobility to diffusivity were found to increase without bounds in the limit where the correlation factor becomes zero. In contrast, as the correlation factor became unity, the diffusivity became zero and the ratio of mobility to diffusivity became unity associated with the uncorrelated limit of 1/kT. This implied that the phenomenon was not unique to the crystal structure but was unique to edge dislocations with vacancy tight binding.