• Steel and Composite Structures
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• 제32권2호
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• pp.157-171
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• 2019

In this research, the dynamic instability region (DIR) of the sandwich nano-beams are investigated based on nonlocal strain gradient elasticity theory (NSGET) and various higher order shear deformation beam theories (HSDBTs). The sandwich piezoelectric nano-beam is including a homogenous core and face-sheets reinforced with functionally graded (FG) carbon nanotubes (CNTs). In present study, three patterns of CNTs are employed in order to reinforce the top and bottom face-sheets of the beam. In addition, different higher-order shear deformation beam theories such as trigonometric shear deformation beam theory (TSDBT), exponential shear deformation beam theory (ESDBT), hyperbolic shear deformation beam theory (HSDBT), and Aydogdu shear deformation beam theory (ASDBT) are considered to extract the governing equations for different boundary conditions. The beam is subjected to thermal and electrical loads while is resting on Visco-Pasternak foundation. Hamilton principle is used to derive the governing equations of motion based on various shear deformation theories. In order to analysis of the dynamic instability behaviors, the linear governing equations of motion are solved using differential quadrature method (DQM). After verification with validated reference, comprehensive numerical results are presented to investigate the influence of important parameters such as various shear deformation theories, nonlocal parameter, strain gradient parameter, the volume fraction of the CNTs, various distributions of the CNTs, different boundary conditions, dimensionless geometric parameters, Visco-Pasternak foundation parameters, applied voltage and temperature change on the dynamic instability characteristics of sandwich piezoelectric nano-beam.

• 항공우주시스템공학회지
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• 제17권4호
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• pp.110-117
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• 2023

본 논문에서는 회전익 항공기 통신·항법 안테나의 최적 위치와 체계 성능측정 방법에 대해 연구하였다. 통신·항법 안테나의 항공기 최적 장착 위치 선정을 위해 기체 형상 및 특성을 고려한 후 항공기 장착 안테나에 대한 복사패턴, 커플링 분석, 장비 운용 프로파일 및 안테나 종류별 분석을 수행하고, 분석결과에 따라 항공기에 장착된 안테나에 대한 지상시험 및 비행시험을 통해 VSWR 측정, 안테나 패턴시험을 순차적으로 수행하는 절차를 정립하였다. 본 논문에서 제안한 체계적인 성능 측정 방법 및 절차는 LAH(소형무장헬기)체계의 지상 및 비행시험을 통해 입증하였다.

• 한국산학기술학회논문지
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• 제20권7호
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• pp.16-19
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• 2019

박막이 얇아질수록 전기적인 특성이 좋아지려면 비정질구조가 유리하다. 비정질구조는 케리어가 공핍되는 특징을 이용하여 전도성을 높이는데 효과가 있을 수 있다. 이러한 특성을 확인하는 방법으로 전위장벽이 형성되는 쇼키접합에 대한 연구가 필요하다. 비정질구조와 쇼키접합에 대하여 조사하기 위하여 $SiO_2/SnO_2$ 박막을 준비하였으며, $SiO_2$ 박막은 Ar=20 sccm 만들고 $SnO_2$ 박막은 아르곤과 산소의 유량을 각각 20 sccm으로 혼합가스를 사용하였으며, 마그네트론 스퍼터링 방법으로 $SnO_2$의을 증착하고 $100^{\circ}C$와 $150^{\circ}C$에서 열처리를 하였다. 비정질구조가 만들어지는 조건을 알아보기 위하여 XRD 패턴을 조사하고 C-V, I-V 측정을 실시하여 Al 전극을 만들고 전기적인 분석을 실시하였다. 공핍층은 열처리과정을 통하여 전자와 홀의 재결합으로 형성되는데 $SiO_2/SnO_2$ 박막은 $100^{\circ}C$에서 열처리를 한 경우 공핍층이 잘 형성이 되었으며, 미시영역에서는 전기적으로 전류가 크게 작용하는 것을 확인하였다. $100^{\circ}C$에서 열처리를 한 비정질의 $SiO_2/SnO_2$ 박막은 XRD 패턴에서 $33^{\circ}$에서는 픽이 나타나지 않았으며, $44^{\circ}$에서는 픽이 생겼다. 쇼키접합에 의해서 거시적(-30V<전압<30V)으로는 절연체 특성이 보였으나 미시적(-5V<전압<5V)으로는 전도성이 나타났다. 케리어가 부족한 공핍층에서의 전도는 확산전류에 의하여 전도가 이루어진다. 미소영역에서 동작하는 소자인 경우에는 공핍효과에 의한 쇼키접합이 전류의 발생과 전도에 유리하다는 것을 확인하였다.

• 한국산학기술학회논문지
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• 제21권5호
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• pp.516-522
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• 2020

수트리의 진행과정은 십수년이 걸리며 보통 매우 오래된 지중케이블에서 발견된다. 이러한 지중케이블들은 이미 접근이 어려운 곳에 있어 수트리를 검출하기 위해서는 많은 비용과 시간이 소요된다. 이러한 지중케이블의 유지보수 비용과 시간을 절감하기 위해서는 수트리가 진행된 지중케이블이 전력망에 미치는 영향을 분석할 수 있는 수학적 모델링이 필요하고, 이를 이용한 수트리 탐지 기술개발이 매우 필요한 실정이다. 본 논문에서는 수트리가 포함된 XLPE 케이블 대한 수학적 모델링을 하고자 수트리의 복잡한 구조를 Vented tree의 확인된 특정 패턴 2가지를 기준으로 가정하여 단순화 하였다. 그리고 수트리의 발달에 따른 케이블 절연층의 캐패시턴스 및 레지스턴스를 계산 및 분석하기 위해 matlab으로 시뮬레이션을 실시하였으며, 모델링의 유용성을 검증하기 위해서 참고문헌 Burkes 논문의 케이블 데이터를 동일하게 적용하였다. 시뮬레이션 결과, 캐패시턴스 크기의 변화는 케이블에 수트리 영역이 절연층에 95%까지 진행되었을 때 정상대비 약 0.025×10^-13[Farads/mm] 증가됨을 확인하였다. 레지스턴스 값의 경우 정상대비 약 0.5×10¹⁶[ohm/m] 정도 감소되는 것을 확인하였다. 따라서, Burkes 논문의 물리적 모델링 시뮬레이션 결과와 비교하였을 때 그 변화값이 매우 유사하여 본 논문에서 제시한 수학적 모델링의 유용성을 검증하였다.

• 한국세라믹학회지
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• 제39권6호
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• pp.523-527
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• 2002

LiMn$_2$O$_4$ compounds were synthesized by calcining a mixture of LiOH and MnO$_2$(CMD) at 47$0^{\circ}C$ for 10 h and then calcining again at $650^{\circ}C$ to 90$0^{\circ}C$ fur 48 h in air with intermediate grinding. All the synthesized samples exhibited XRD patterns for the cubic spinel phase with a space group Fd3m. The lattice parameter increased gradually as the sintering temperature rose. The electrochemical cells were charged and discharged fur 20 cycles at a current density 300$\mu$A/$\textrm{cm}^2$ between 3.5 V and 4.3 V. The voltage vs. discharge capacity curves for all the samples showed two plateaus. The LiMn$_2$O$_4$ sample calcined at 90$0^{\circ}C$ had the largest first discharge capacity. This sample exhibited the best crystallinity, had relatively large lattice parameter and had relatively large particles with rectatively homogeneous size. All the samples showed good cycling performances. Among all the samples, the LiMn$_2$O$_4$ calcined at 85$0^{\circ}C$ had relatively large first discharge capacity and very good cycling performance. The addition of excess LiOH and the mixing in ethanol considered to help the formation of the more LiMn$_2$O$_4$ phase per unit weight sample and the more stable LiMn$_2$O$_4$phase. These led to the larger discharge capacities and the better cycling performances. The cyclic voltammograms fur the second cycle of the LiMn$_2$O$_4$ samples showed the oxidation and reduction peaks around 4.05 V and 4.18 V and around 4.08 V and 3.94 V, respectively. The larger first discharge capacity of the sample calcined at the higher temperature is related to the larger lattice parameter.

• 공업화학
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• 제7권3호
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• pp.543-553
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• 1996

산소전극 촉매로서 페롭스카이트형 산화물을 사용하여 알칼리형 연료전지에서의 산소환원반응에 관하여 연구하였다. 능금산(malic acid)을 사용하여 고표면적의 페롭스카이트형 $La_{0.6}Sr_{0.4}Co_{1-x}Fe_xO_3$(x=0.00, 0.01, 0.10, 0.20, 0.35 및 0.50) 산화물을 제조하였으며, Fe 치환량과 암모니아수 첨가량에 따른 XRD 구조와 비표면적의 변화를 고찰하여 Fe와 암모니아간에 생성되어지는 착화합물이 페롭스카이트로의 구조안정화와 비표면적 증대의 주요임을 알았다. 그리고 페롭스카이트 단일상을 얻기 위해서는 다단계 승온처리가 필요했으며, XRD 실험결과 단순 정입방체상이 형성됨을 확인하였다. $La_{0.6}Sr_{0.4}Co_{1-x}Fe_xO_3$ 산화물을 촉매로 사용한 알칼리형 연료전지용 산소전극의 산소환원반응활성을 측정하기 위하여 순환 전압-전류법, 정전압-전류법, 전류단절법 등을 이용하였다. $La_{0.6}Sr_{0.4}Co_{1-x}Fe_xO_3$ 산화물에서 Fe의 치환비가 증가함에 따라, x=0.01에서 최소, x=0.20와 0.35 사이에서 최대의 산소환원활성(전류밀도)을 보였으며, 이와 같은 경향은 표면적의 변화와 무관하였다.

• 한국태양에너지학회 논문집
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• 제25권4호
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• pp.1-11
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• 2005

The stoichiometric mixture of evaporating materials for the $CuInSe_2$ single crystal thin film was prepared from horizontal furnace. Using extrapolation method of X-ray diffraction patterns for the polycrystal $CuInSe_2$, it was found tetragonal structure whose lattice constant $a_0$ and $c_0$ were $5.783\;{\AA}$ and $11.621\;{\AA}$, respectively. To obtain the $CuInSe_2$ single crystal thin film, $CuInSe_2$ mixed crystal was deposited on throughly etched GaAs(100) by the HWE(Hot Wall Epitaxy) system. The source and substrate temperature were $620^{\circ}C$ and $410^{\circ}C$ respectively. The crystalline structure of $CuInSe_2$ single crystal thin film was investigated by the double crystal X-ray diffraction(DCXD). Hall effect on this sample was measured by the method of Van der Pauw and studied on carrier density and mobility depending on temperature. From Hall data, the mobility was likely to be decreased by impurity scattering in the temperature range 30 K to 100 K and by lattice scattering in the temperature range 100 K to 293 K. The temperature dependence of the energy band gap of the $CuInSe_2$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)=1.1851\;eV-(8.99{\times}10^{-4}\;eV/K)T^2/(T+153\;K)$. The open-circuit voltage, short current density, fill factor, and conversion efficiency of $n-CdS/p-CuGaSe_2$ heterojunction solar cells under $80\;mW/cm^2$ illumination were found to be 0.51V, $29.3\;mA/cm^2$, 0.76 and 14.3 %, respectively.

• 한국태양에너지학회 논문집
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• 제38권1호
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• pp.25-36
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• 2018

The stoichiometric mixture of evaporating materials for the $CaAl_2Se_4$: Co single crystal thin film was prepared from horizontal furnace. Using extrapolation method of X-ray diffraction patterns for the polycrystal $CaAl_2Se_4$, it was found orthorhomic structure whose lattice constant $a_0$, $b_0$ and $c_0$ were 6.4818, $11.1310{\AA}$ and $11.2443{\AA}$, respectively. To obtain the $CaAl_2Se_4$: Co single crystal thin film, $CaAl_2Se_4$: Co mixed crystal was deposited on throughly etched Si (100) by the HWE (Hot Wall Epitaxy) system. The source and substrate temperature were $600^{\circ}C$ and $440^{\circ}C$ respectively. The crystalline structure of $CaAl_2Se_4$: Co single crystal thin film was investigated by the double crystal X-ray diffraction (DCXD). Hall effect on this sample was measured by the method of Van der Pauw and studied on carrier density and mobility depending on temperature. From Hall data, the mobility was likely to be decreased by impurity scattering in the temperature range 30 K to 100 K and by lattice scattering in the temperature range 100 K to 293 K. The temperature dependence of the energy band gap of the $CaAl_2Se_4$: Co obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)=3.8239eV-(4.9823{\times}10^{-3}eV/K)T_2/(T+559K)$. The open-circuit voltage, short current density, fill factor, and conversion efficiency of $p-Si/p-CaAl_2Se_4$: Co heterojunction solar cells under $80mW/cm^2$ illumination were found to be 0.42 V, $25.3mA/cm^2$, 0.75 and 9.96%, respectively.

• 한국정보전자통신기술학회논문지
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• 제16권1호
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• pp.8-17
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• 2023

기존 liquid crystal display(LCD) 공정에서 Indium Tin Oxide(ITO) 투명전극과 폴리이미드 배향막의 러빙 공정은 액정을 정렬하고 전계를 인가하기 위하여 필수적인 공정이다. 하지만 ITO의 증착은 높은 진공을 요구하며, 러빙 공정은 정전기에 의해 소자가 손상될 수 있는 단점이 존재한다. 본 논문에서는 기존 ITO 투명전극을 대체하기 위하여 PEDOT:PSS와 Multi-wall carbon nanotube(MWNT)를 혼합하여 PEDOT:PSS 나노복합체를 제조하고, 러빙 공정을 대체하기 위하여 나노 주름 구조 몰드를 통한 나노임프린팅을 통하여 박막을 형성함으로써 기존 액정 디스플레이의 투명전극과 배향막 두 가지 박막을 PEDOT:PSS/MWNT 나노복합체 박막 하나만으로 기능하게 하여 공정을 단순화 하였다. 전사된 나노 주름을 따라 액정이 잘 배향됨을 확인하였으며, 이를 기반으로 만들어진 액정 셀에서 박막 내 MWNT의 함량이 높아질수록 박막의 전기전도도가 증가하여 낮은 구동 전압과 빠른 응답 속도를 갖는다는 것을 확인하였다. 본 연구를 통해 공정 단순화와 용액공정에 의한 공정 단가 절감, 기존 러빙 공정의 단점을 해결하는데 기여 할 수 있을 것으로 기대된다.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2011년도 춘계학술발표대회
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• pp.5-5
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• 2011

The research and development of hybrid electric vehicle (HEV), plug-in hybrid electric vehicle (PHEV) and electric vehicle (EV) are intensified due to the energy crisis and environmental concerns. In order to meet the challenging requirements of powering HEV, PHEV and EV, the current lithium battery technology needs to be significantly improved in terms of the cost, safety, power and energy density, as well as the calendar and cycle life. One new technology being developed is the utilization of composite cathode by mixing two different types of insertion compounds [e.g., spinel $LiMn_2O_4$ and layered $LiMO_2$ (M=Ni, Co, and Mn)]. Recently, some studies on mixing two different types of cathode materials to make a composite cathode have been reported, which were aimed at reducing cost and improving self-discharge. Numata et al. reported that when stored in a sealed can together with electrolyte at $80^{\circ}C$ for 10 days, the concentrations of both HF and $Mn^{2+}$ were lower in the can containing $LiMn_2O_4$ blended with $LiNi_{0.8}Co_{0.2}O_2$ than that containing $LiMn_2O_4$ only. That reports clearly showed that this blending technique can prevent the decline in capacity caused by cycling or storage at elevated temperatures. However, not much work has been reported on the charge-discharge characteristics and related structural phase transitions for these composite cathodes. In this presentation, we will report our in situ x-ray diffraction studies on this mixed composite cathode material during charge-discharge cycling. The mixed cathodes were incorporated into in situ XRD cells with a Li foil anode, a Celgard separator, and a 1M $LiPF_6$ electrolyte in a 1 : 1 EC : DMC solvent (LP 30 from EM Industries, Inc.). For in situ XRD cell, Mylar windows were used as has been described in detail elsewhere. All of these in situ XRD spectra were collected on beam line X18A at National Synchrotron Light Source (NSLS) at Brookhaven National Laboratory using two different detectors. One is a conventional scintillation detector with data collection at 0.02 degree in two theta angle for each step. The other is a wide angle position sensitive detector (PSD). The wavelengths used were 1.1950 ${\AA}$ for the scintillation detector and 0.9999 A for the PSD. The newly installed PSD at beam line X18A of NSLS can collect XRD patterns as short as a few minutes covering $90^{\circ}$ of two theta angles simultaneously with good signal to noise ratio. It significantly reduced the data collection time for each scan, giving us a great advantage in studying the phase transition in real time. The two theta angles of all the XRD spectra presented in this paper have been recalculated and converted to corresponding angles for ${\lambda}=1.54\;{\AA}$, which is the wavelength of conventional x-ray tube source with Cu-$k{\alpha}$ radiation, for easy comparison with data in other literatures. The structural changes of the composite cathode made by mixing spinel $LiMn_2O_4$ and layered $Li-Ni_{1/3}Co_{1/3}Mn_{1/3}O_2$ in 1 : 1 wt% in both Li-half and Li-ion cells during charge/discharge are studied by in situ XRD. During the first charge up to ~5.2 V vs. $Li/Li^+$, the in situ XRD spectra for the composite cathode in the Li-half cell track the structural changes of each component. At the early stage of charge, the lithium extraction takes place in the $LiNi_{1/3}Co_{1/3}Mn_{1/3}O_2$ component only. When the cell voltage reaches at ~4.0 V vs. $Li/Li^+$, lithium extraction from the spinel $LiMn_2O_4$ component starts and becomes the major contributor for the cell capacity due to the higher rate capability of $LiMn_2O_4$. When the voltage passed 4.3 V, the major structural changes are from the $LiNi_{1/3}Co_{1/3}Mn_{1/3}O_2$ component, while the $LiMn_2O_4$ component is almost unchanged. In the Li-ion cell using a MCMB anode and a composite cathode cycled between 2.5 V and 4.2 V, the structural changes are dominated by the spinel $LiMn_2O_4$ component, with much less changes in the layered $LiNi_{1/3}Co_{1/3}Mn_{1/3}O_2$ component, comparing with the Li-half cell results. These results give us valuable information about the structural changes relating to the contributions of each individual component to the cell capacity at certain charge/discharge state, which are helpful in designing and optimizing the composite cathode using spinel- and layered-type materials for Li-ion battery research. More detailed discussion will be presented at the meeting.