90 research outputs found

    ν™˜ν™©ν•΄κΆŒ μžμœ μ§€μ—­ 연계망 κ΅¬μΆ•μ˜ μ „λž΅κ³Ό λ°©μ•ˆ(Strategies and measures for building a localized network of free zones in the Yellow Sea sub-region)

    Get PDF
    λ…ΈνŠΈ : 이 μ—°κ΅¬λ³΄κ³ μ„œμ˜ λ‚΄μš©μ€ κ΅­ν† μ—°κ΅¬μ›μ˜ 자체 μ—°κ΅¬λ¬Όλ‘œμ„œ μ •λΆ€μ˜ μ •μ±…μ΄λ‚˜ κ²¬ν•΄μ™€λŠ” μƒκ΄€μ—†μŠ΅λ‹ˆλ‹€

    ν™˜ν™©ν•΄κΆŒ μ£Όμš” ν•­λ§Œλ„μ‹œκ°„ 연계망 κ΅¬μΆ•μ „λž΅(Inter-city networking strategy in the Yellow Sea sub-region)

    Get PDF
    λ…ΈνŠΈ : 이 책은 κ΅­ν† μ—°κ΅¬μ›μ˜ 자체 μ—°κ΅¬λ¬Όλ‘œμ„œ μ •λΆ€μ˜ μ •μ±…μ΄λ‚˜ κ²¬ν•΄μ™€λŠ” μƒκ΄€μ—†μŒμ„ λ°ν˜€λ‘‘λ‹ˆλ‹€

    λ‚˜λ…ΈμŠ€μΌ€μΌμ—μ„œμ˜ ν‘œλ©΄νš¨κ³Όμ™€ κ³„λ©΄νš¨κ³Όλ₯Ό κ³ λ €ν•œ λ°•λ§‰μ˜ 연속체 λͺ¨λΈλ§

    No full text
    Due to the evolution of fabrication technology of semiconductor, a lot of micro electro-mechanical systems have been developed and have been used in daily life. Nowadays, not only micro-scale devices but also lots of nano-scale devices, such as a bio sensor and a nano resonator, have been developed. Because surface-to-volume ratio becomes very high in nano-scaled devices, surface effect makes a great effect on mechanical properties and behaviors of nano structures. The one of representative examples of surface effect is equilibrium strain of nanofilm and nanowire in relaxed state. Because the magnitude of equilibrium strain might exceed the linear elastic assumption in a thin nanofilm with a few nanometer thickness, hyperelastic material properties should be considered in nano-scale devices according to equilibrium strain. Besides this surface effect, interface effect plays an important role in equilibrium configuration and mechanical behavior in multi-layered nano structures. In this dissertation, continuum-based multiscale modeling for multi-layered nanostructures is proposed. This proposed model includes surface effect and interface effect which are calculated by atomistic simulations. In order to design and analyze multi-layer thin film using nonlinear finite element method, four modeling techniques are proposed. First, surface relaxation model for FCC crystal structure is proposed to calculate surface parameters which are required to describe surface effect on continuum modeling. In this section, the equilibrium strain in nanofilm is evaluated using calculated surface properties and the analytical solution for size-dependent elasticity is also provided using proposed surface relaxation model. Second, continuum-based multiscale model including anisotropic surface effect is proposed. In this model, linear surface elasticity model is utilized to describe surface constitutive relation. The proposed multiscale model describes the size-dependent elasticity due to surface effect very well and it is also reported that the hyperelastic effect of bulk region as well as surface effect should be considered in nanofilm. Third, Hyperelastic model for transition metal and silicon materials is proposed. A strain energy function is used to represent hyperelastic relations and is composed of polynomial based function with nine strain invariants. The hyperelastic material constants are evaluated by least square method using the results of atomistic calculation. The proposed hyperelastic model can be embedded in finite element method much easier than Cauchy-Born rule. Finally, interface model for a covalent bond is provided for multi-layered nano structures. Using this model, the equilibrium configuration of Si/SiGe bilayer nanosprings is characterized by strip orientation and width-to-thickness ratio. Although the proposed continuum-based multiscale model including surface and interface effects and hyperelastic model are far more efficient than atomistic calculations in designing nano structures, they give comparable results to Cauchy-Born rule and atomistic simulations. These continuum-based approaches will be very useful and promising designing tools for nano-scaled structures composed of nanofilms.λ°˜λ„μ²΄ μ œμž‘ 기술의 λ°œμ „μœΌλ‘œ ν˜„μž¬κΉŒμ§€ λ§Žμ€ 마이크둜 μŠ€μΌ€μΌμ˜ 전기기계적인 μž₯치(MEMS)듀이 κ°œλ°œλ˜μ–΄ μ‚¬μš©λ˜κ³  μžˆλ‹€. μ΅œκ·Όμ—λŠ” 마이크둜 μŠ€μΌ€μΌλΏλ§Œ μ•„λ‹ˆλΌ λ°”μ΄μ˜€μ„Όμ„œμ™€ λ‚˜λ…Έκ³΅μ§„κΈ°μ™€ 같은 λ§Žμ€ λ‚˜λ…Έ μŠ€μΌ€μΌμ˜ μž₯μΉ˜λ“€μ΄ 개발되고 μžˆλ‹€. λ‚˜λ…Έ μŠ€μΌ€μΌμ˜ μž₯μΉ˜μ—μ„œλŠ” ν‘œλ©΄λŒ€λΆ€ν”ΌλΉ„(surface-to-volume ratio)κ°€ 맀우 크기 λ•Œλ¬Έμ— ν‘œλ©΄νš¨κ³Όκ°€ λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ˜ 기계적 νŠΉμ„±κ³Ό 거동에 맀우 큰 영ν–₯을 미치게 λœλ‹€. ν‘œλ©΄νš¨κ³Όμ˜ λŒ€ν‘œμ μΈ 예둜 μ΄μ™„μƒνƒœ(relaxed state)μ—μ„œμ˜ λ‚˜λ…Έλ°•λ§‰κ³Ό λ‚˜λ…Έμ™€μ΄μ–΄μ˜ ν‰ν˜• λ³€ν˜•μœ¨(equilibrium strain)이 μžˆλ‹€. λ‚˜λ…Έλ°•λ§‰μ€ ν‘œλ©΄μ— μž‘μš©ν•˜λŠ” ν‘œλ©΄μ‘λ ₯에 μ˜ν•˜μ—¬ ν‰ν˜•μƒνƒœλ₯Ό 이루기 μœ„ν•΄ λ©΄λ‚΄ λ°©ν–₯으둜의 λ³€ν˜•μ΄ λ°œμƒν•˜κ²Œ λœλ‹€. λ‚˜λ…Έμ™€μ΄μ–΄μ˜ κ²½μš°λŠ” 길이방ν–₯으둜 λ³€ν˜•μ΄ μΌμ–΄λ‚œλ‹€. μ΄λ•Œ λ°œμƒν•˜λŠ” λ³€ν˜•μœ¨μ„ ν‰ν˜• λ³€ν˜•μœ¨μ΄λΌκ³  ν•œλ‹€. μ΄λŸ¬ν•œ ν‰ν˜• λ³€ν˜•μœ¨μ˜ ν¬κΈ°λŠ” 수 λ‚˜λ…Έλ―Έν„° λ‘κ»˜μ˜ λ‚˜λ…Έλ°•λ§‰μ—μ„œλŠ” μ„ ν˜• 탄성 μ˜μ—­μ„ λ²—μ–΄λ‚˜λ―€λ‘œ, λ‚˜λ…ΈμŠ€μΌ€μΌμ˜ μž₯치의 ν•΄μ„μ—λŠ” ν‰ν˜• λ³€ν˜•μœ¨μ— λ”°λ₯Έ λΉ„μ„ ν˜• 탄성 νš¨κ³Όκ°€ κ³ λ €λ˜μ–΄μ•Ό ν•œλ‹€. μ΄λŸ¬ν•œ ν‘œλ©΄νš¨κ³Ό 이외에도 κ³„λ©΄μ—μ„œ λ°œμƒν•˜λŠ” κ³„λ©΄νš¨κ³ΌλŠ” 닀쀑박막 λ‚˜λ…Έ ꡬ쑰물의 ν˜•μƒκ³Ό 기계적 거동에 맀우 μ€‘μš”ν•œ 역할을 λ‹΄λ‹Ήν•œλ‹€. λ³Έ λ…Όλ¬Έμ—μ„œλŠ” 닀쀑박막 λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ˜ 해석을 μœ„ν•œ 연속체 기반의 λ©€ν‹°μŠ€μΌ€μΌ λͺ¨λΈλ§ 기법듀을 μ œμ•ˆν•œλ‹€. λ³Έ λ…Όλ¬Έμ—μ„œ μ œμ•ˆν•˜λŠ” λ©€ν‹°μŠ€μΌ€μΌ λͺ¨λΈμ€ μ›μžμˆ˜μ€€μ˜ 계산을 ν†΅ν•˜μ—¬ κ³„μ‚°λ˜λŠ” 물성듀을 μ΄μš©ν•œ ν‘œλ©΄νš¨κ³Όμ™€ κ³„λ©΄νš¨κ³Όλ₯Ό ν¬ν•¨ν•œλ‹€. λ‹€μ€‘λ°•λ§‰μ˜ λΉ„μ„ ν˜• μœ ν•œμš”μ†Œ 해석을 μœ„ν•΄ λ³Έ λ…Όλ¬Έμ—μ„œλŠ” λ„€ 개의 λͺ¨λΈλ§ 기법이 μ œμ•ˆλœλ‹€. 첫 λΆ€λΆ„μ—μ„œλŠ” 연속체에 ν‘œλ©΄νš¨κ³Όλ₯Ό λ‚˜νƒ€λ‚΄κΈ° μœ„ν•΄ ν•„μš”ν•œ ν‘œλ©΄ 물성을 κ³„μ‚°ν•˜κΈ° μœ„ν•΄ ν‘œλ©΄ 이완 λͺ¨λΈ(surface relaxation model)이 μ œμ•ˆλœλ‹€. 이 λΆ€λΆ„μ—μ„œλŠ” κ³„μ‚°λœ ν‘œλ©΄ 물성을 μ΄μš©ν•˜μ—¬ ν‰ν˜• λ³€ν˜•μœ¨(equilibrium strain)κ³Ό 크기에 의쑴적인 탄성(size-dependent elasticity)을 κ³„μ‚°λœλ‹€. 두 번째 λΆ€λΆ„μ—μ„œλŠ” λΉ„λ“±λ°©μ„± ν‘œλ©΄νš¨κ³Όλ₯Ό κ³ λ €ν•œ 연속체 기반의 λ©€ν‹°μŠ€μΌ€μΌ λͺ¨λΈμ΄ μ œμ•ˆλœλ‹€. 이 λͺ¨λΈμ—μ„œλŠ” ν‘œλ©΄μ˜ κ΅¬μ„±λ°©μ •μ‹μœΌλ‘œ μ„ ν˜• 탄성 λͺ¨λΈμ΄ μ‚¬μš©λœλ‹€. μ œμ•ˆλœ λ©€ν‹°μŠ€μΌ€μΌ λͺ¨λΈμ„ μ΄μš©ν•˜μ—¬ 크기에 의쑴적인 νƒ„μ„±μ˜ 계산이 κ°€λŠ₯ν•˜λ©°, 이 κ²°κ³ΌλŠ” μ›μžμ  계산에 μ˜ν•΄ κ³„μ‚°λœ 해석해와 맀우 잘 μΌμΉ˜ν•œλ‹€. λ˜ν•œ, 이 λͺ¨λΈμ€ 크기에 의쑴적인 νƒ„μ„±μ˜ 계산에 μžˆμ–΄μ„œ ν‘œλ©΄νš¨κ³ΌλΏλ§Œ μ•„λ‹ˆλΌ 벌크 μ˜μ—­μ˜ λΉ„μ„ ν˜• 물성이 μ€‘μš”ν•œ 영ν–₯을 미치고 μžˆμŒμ„ 보여쀀닀. μ„Έ 번째 λΆ€λΆ„μ—μ„œλŠ” 천이 κΈˆμ†μ— λŒ€ν•œ λΉ„μ„ ν˜• 탄성λͺ¨λΈμ΄ μ œμ•ˆλœλ‹€. λ³€ν˜•μœ¨ μ—λ„ˆμ§€ ν•¨μˆ˜(strain energy density function)κ°€ λΉ„μ„ ν˜• 탄성 거동을 λ¬˜μ‚¬ν•˜κΈ° μœ„ν•΄ μ‚¬μš©λ˜λ©°, 이 ν•¨μˆ˜λŠ” 9개의 λ³€ν˜•μœ¨ λΆˆλ³€λŸ‰(strain invariant)으둜 ν‘œμ‹œλ˜λŠ” λ‹€ν•­μ‹μ˜ ν˜•μ‹μœΌλ‘œ κ΅¬μ„±λœλ‹€. λΉ„μ„ ν˜• 탄성 κ³„μˆ˜λ“€μ€ μ›μžμˆ˜μ€€μ˜ μ „μ‚°λͺ¨μ‚¬μ˜ κ²°κ³Όλ₯Ό μ΄μš©ν•˜μ—¬ μ΅œμ†ŒμžμŠΉλ²•μœΌλ‘œ κ³„μ‚°λœλ‹€. 이 λΉ„μ„ ν˜• 탄성 λͺ¨λΈμ€ Cauchy-Born 법칙에 μ˜ν•œ μ›μžμ  계산보닀 λ‹¨μˆœν•˜κΈ° λ•Œλ¬Έμ— 더 μ‰½κ²Œ μœ ν•œμš”μ†Œ 해석에 적용이 κ°€λŠ₯ν•˜λ‹€. λ§ˆμ§€λ§‰μœΌλ‘œ 닀쀑박막 λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ˜ 해석을 μœ„ν•œ κ³΅μœ κ²°ν•©μ„ κ°€μ§€λŠ” 계면에 λŒ€ν•œ λͺ¨λΈλ§ 기법이 μ œμ•ˆλœλ‹€. 이 λͺ¨λΈμ„ μ΄μš©ν•˜μ—¬ λ°©ν–₯ 및 폭과 λ‘κ»˜λΉ„μ— μ˜ν•œ Si/SiGe λ‚˜λ…ΈμŠ€ν”„λ§μ˜ ν˜•μƒ 변화에 λŒ€ ν•œ 연ꡬ가 μˆ˜ν–‰λ˜λ©°, 계면 효과뿐만 μ•„λ‹ˆλΌ λΉ„λŒ€μΉ­μ  ν‘œλ©΄ 물성을 κ°€μ§€λŠ” 닀이아λͺ¬λ“œ ꡬ쑰의 ν‘œλ©΄νš¨κ³Όλ₯Ό κ³ λ €ν•œ 해석 기법도 ν•¨κ»˜ μ œμ•ˆλœλ‹€. λ³Έ λ…Όλ¬Έμ—μ„œ μ œμ•ˆν•˜λŠ” λΉ„μ„ ν˜• 탄성 λͺ¨λΈκ³Ό ν‘œλ©΄νš¨κ³Όμ™€ κ³„λ©΄νš¨κ³Όλ₯Ό κ³ λ €ν•œ 연속체 기반의 λ©€ν‹°μŠ€μΌ€μΌ λͺ¨λΈλ§ 기법듀은 μ›μžμ  계산방법에 λΉ„ν•΄ 훨씬 더 λΉ λ₯΄κ³  κ°„νŽΈν•˜κ²Œ 계산이 κ°€λŠ₯ν•œ λ°©λ²•λ“€μ΄λ©΄μ„œλ„ Cauchy-Born 기법과 μ›μžμ  계산에 ν•„μ ν•˜λŠ” 계산 결과듀을 보여쀀닀. λ³Έ λ…Όλ¬Έμ—μ„œ μ œμ•ˆν•œ 연속체 기반의 기법듀은 λ‚˜λ…Έλ°•λ§‰μœΌλ‘œ κ΅¬μ„±λ˜λŠ” λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ˜ 해석에 맀우 μœ μš©ν•˜κ³  전망이 μžˆλŠ” 해석 도ꡬ듀이 될 것이닀.Docto

    νˆ¬κΈ°μ’…λͺ© μ„ μˆ˜μ˜ μ •μ‹ λ ₯ κ°œλ… ꡬ쑰 탐색 및 μΈ‘μ • 도ꡬ 개발

    No full text
    ν•™μœ„λ…Όλ¬Έ(박사)--μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› :체윑ꡐ윑과,2001.Docto

    동뢁아 ν˜‘λ™μ  μ§€μ—­κ°œλ°œμ˜ 사둀뢄석과 이둠 λͺ¨μƒ‰(Case studies and theoretical explorations of callaborative regional development in Northeast Asia)

    No full text
    λ…ΈνŠΈ : 이 μ—°κ΅¬λ³΄κ³ μ„œμ˜ λ‚΄μš©μ€ κ΅­ν† μ—°κ΅¬μ›μ˜ 자체 μ—°κ΅¬λ¬Όλ‘œμ„œ μ •λΆ€μ˜ μ •μ±…μ΄λ‚˜ κ²¬ν•΄μ™€λŠ” μƒκ΄€μ—†μŠ΅λ‹ˆλ‹€

    Clinical significance of classification of graves` disease according to the characteristics of TSH receptor antibodies

    No full text
    ν•™μœ„λ…Όλ¬Έ(박사)--μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› :μ˜ν•™κ³Ό 내과학전곡,1998.Docto

    톡일 ν•œλ°˜λ„ λΉ„μ „κ³Ό κ΅­ν† μ „λž΅

    No full text
    λ…ΈνŠΈ : λ³Έ 간행물은 κ΅­ν† μ—°κ΅¬μ›μ—μ„œ 2015λ…„ 1월에 λ°œν–‰ν•œ [ν†΅μΌμ‹œλŒ€μ˜ κ΅­ν† μ •μ±…λ°©ν–₯] νŠΉμ§‘μ˜ 제 1λΆ€μž…λ‹ˆλ‹€
    • …
    corecore