• Title/Summary/Keyword: 심재엽

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Damage Potential of a Domestic Metropolitan Railway Bridge subjected to 2016 Gyeongju Earthquake (2016년 경주지진에 의한 국내 도시철도 교량의 잠재적 손상평가)

  • Lee, Do Hyung;Shim, Jae Yeob;Jeon, Jong-Su
    • Journal of the Earthquake Engineering Society of Korea
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    • v.20 no.7_spc
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    • pp.461-472
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    • 2016
  • Damage potential has been investigated for a domestic metropolitan railway bridge subjected to 2016 Gyeongju earthquake which has been reported as the strongest earthquake in Korea. For this purpose, nonlinear static pushover analyses for the bridge piers have been carried out to evaluate ductility capacities. Then, the capacities have been compared with those suggested by Railway Design Standards of Korea. This comparison shows that all piers possess enough safety margins. Nonlinear dynamic time-history analysis has also been conducted to estimate both displacement and shear force demands for the bridge subjected to ground motions recorded at stations in near of Gyeongju. Maximum demands reveal that response under the ground motions remains essentially in elastic. In addition, for a further assessment of the bridge under the Gyeongju earthquake, fragility analyses have been performed using those ground motions. The fragility results indicate that the recorded earthquakes do not significantly affect the damage exceedance probability of the bridge piers.

Q-band MMIC Driver and Power Amplifiers for Wideband wireless Multimedia (Q-band 광대역 무선 멀티미디어용 MMIC구동 및 전력증폭기)

  • 강동민;이진희;윤형섭;심재엽;이경호
    • Proceedings of the IEEK Conference
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    • 2002.06a
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    • pp.167-170
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    • 2002
  • The design and fabrication of Q-band 3-stage monolithic microwave integrated circuit(MMIC) driver and power amplifiers for WLAN are presented using 0.2${\mu}{\textrm}{m}$ AlGaAs/InGaAs/GaAs pseudomorphic high electron mobility transistor(PHEMT). In each stage of the MMIC DA, a negative feedback is used for both broadband and good stability. The MMIC PA has employed a balanced configuration to overcome these difficulties and achieve high power with low VSWR over a wide frequency range. In the MMIC DA, the measurement results arc achieved as an input return loss under -4dB, an output return loss under -l0dB, a gain of 14dB, and a PldB of 17dB at C-band(36~ 44GHz). The chip size is 28mm$\times$1.3mm. The developed MMIC PA has the l0dB linear gain over 360Hz to 420Hz band and 22dBm PldB performance at 400Hz. The size of fabricated MMIC PA is 4mm x3mm. These results closely match with design results. This MMIC DA Sl PA will be used as the unit cells to develop millimeter-wave transmitters for use in wideband wireless LAN systems.

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Phase sequence in Codeposition and Solid State Reaction of Co-Si System and Low Temperature Epitaxial Growth of $CoSi_2$ Layer (Co-Si계의 동시증착과 고상반응시 상전이 및 $CoSi_2$ 층의 저온정합성장)

  • 박상욱;심재엽;지응준;최정동;곽준섭;백홍구
    • Journal of the Korean Vacuum Society
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    • v.2 no.4
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    • pp.439-454
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    • 1993
  • The phase sequence of codeposited Co-Si alloy and Co/si multilayer thin film was investigated by differential scanning calormetry(DSC) and X-ray diffraction (XRD) analysis, The phase sequence in codeposition and codeposited amorphous Co-Si alloy thin film were CoSilongrightarrow Co2Si and those in Co/Si multilayer thin film were CoSilongrightarrowCo2Silongrightarrow and CoSilongrightarrowCo2Si longrightarrowCoSilongrightarrowCoSi2 with the atomic concentration ration of Co to Si layer being 2:1 and 1:2 respectively. The observed phase sequence was analyzed by the effectvie heat of formatin . The phase determining factor (PDF) considering structural facotr in addition to the effectvie heat of formation was used to explain the difference in the first crystalline phase between codeposition, codeposited amorphous Co-Si alloy thin film and Co/Si multilayer thin film. The crystallinity of Co-silicide deposited by multitarget bias cosputter deposition (MBCD) wasinvestigated as a funcion of deposition temperature and substrate bias voltage by transmission electron microscopy (TEM) and epitaxial CoSi2 layer was grown at $200^{\circ}C$ . Parameters, Ear, $\alpha$(As), were calculate dto quantitatively explain the low temperature epitaxial grpwth of CoSi2 layer. The phase sequence and crystallinity had a stronger dependence on the substrate bias voltage than on the deposition temperature due to the collisional daxcade mixing, in-situ cleannin g, and increase in the number of nucleation sites by ion bombardment of growing surface.

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Interfacial reactions in Cu/NbTi multilayer thin films and superconducting wires (임게전류밀도 향상을 위한 Cu/NbTi다층박막과 초전도 선재에서의 계면반응)

  • 심재엽;백홍구;하동우;오상수;류강식
    • Electrical & Electronic Materials
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    • v.8 no.4
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    • pp.478-486
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    • 1995
  • Cu/NbTi multilayer thin films and superconducting wires were fabricated and heat treated with conventional annealing and analyzed by differential scanning calorimetry (DSC) as a basic study for the enhancement of Jc. Interfacial reactions of Cu/NbTi multilayer thin films and superconducting wires were investigated with optical microscope, SEM, and XRD. According to the effective heat of formation (EHF) model, CU$\_$3/Ti was predicted as a first phase. However, considering the crystalline structure and thermodynamics, CuTi was predicted as a first phase. According to the results of DSC and XRD, CU$\_$2/Ti was found to be the first phase, followed by the formation Of CU$\_$4/Ti. The difference in first crystalline phase between the experimental result and the predicted one was discussed. In case of Cu/NbTi superconducting wires, the compounds formed at the Cu/NbTi interface grew with annealing time and the amount of compounds formed in Nb-47wt%Ti alloy was larger than that in Nb-50wt%Ti alloy. It seemed that the incubation time for the formation of compounds in Nb-50wt%Ti alloy was longer than that formed in Nb-47wt%Ti alloy. Also, the diffusion was the rate controlling step for the growth of compounds in all specimens. These compounds were formed at 500-600.deg. C for I hour annealing and, thus, the drawing time below I hour must be required to minimize the growth of compounds for the enhancement of Jc.

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A 77GHz MMIC Transceiver Module for Automotive Forward-Looking Radar Sensor

  • Kang, Dong-Min;Hong, Ju-Yeon;Shim, Jae-Yeob;Yoon, Hyung-Sup;Lee, Kyung-Ho
    • Proceedings of the IEEK Conference
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    • 2006.06a
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    • pp.609-610
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    • 2006
  • A 77GHz MMIC transceiver module consisting of a power amplifier, a low noise amplifier, a drive amplifier, a frequency doubler and a down-mixer has been developed for automotive forward-looking radar sensor. The MMIC chip set was fabricated using $0.15{\mu}m$ gate-length InGaAs/InAlAs/GaAs mHEMT process based on 4-inch substrate. The power amplifier demonstrated a measured small signal gain of over 20dB from $76{\sim}77GHz$ with 15.5dBm output power. The chip size is $2mm{\times}2mm$. The low noise amplifier achieved a gain of 20dB in a band between $76{\sim}77\;GHz$ with an output power of 10dBm. The chip size is $2.2mm{\times}2mm$. The driver amplifier exhibited a gain of 23dB over a $76{\sim}77\;GHz$ band with an output power of 13dBm. The chip size is $2.1mm{\times}2mm$. The frequency doubler achieved an output power of -16dBm at 76.5GHz with a conversion gain of -16dB for an input power of 10dBm and a 38.25GHz input frequency. The chip size is $1.2mm{\times}1.2mm$. The down-mixer demonstrated a measured conversion gain of over -9dB. The chip size is $1.3mm{\times}1.9mm$. The transceiver module achieved an output power of 10dBm in a band between $76{\sim}77GHz$ with a receiver P1dB of -28dBm. The module size is $8{\times}9.5{\times}2.4mm^3$. This MMIC transceiver module is suitable for the 77GHz automotive radar systems and related applications in W-band.

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Seismic Fragility Analysis of Reinforced Concrete Bridge Piers According to Damage State (철근콘크리트 교량 교각의 손상상태에 따른 지진취약도 해석)

  • Jeon, Jeong Moon;Shin, Jae Kwan;Shim, Jae Yeob;Lee, Do Hyung
    • KSCE Journal of Civil and Environmental Engineering Research
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    • v.34 no.6
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    • pp.1695-1705
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    • 2014
  • In the present study, a total of 275 tested specimens (149 of non-seismically designed and 126 of seismically designed) for reinforced concrete bridge piers with circular section have been investigated in order to suggest drift limits probabilistically according to damage states in seismic fragility analysis. Thus, quantitative damage states of the piers have been evaluated depending on details of the piers. Nonlinear time-history analyses have been conducted for a damaged bridge in terms of using the suggested drift limits. Then, seismic fragility analysis for a reinforced concrete bridge structure has been conducted using both suggested and existing drift limits. Comparative analyses have revealed that median values by the suggested limits is smaller than those by the existing limits. This implies that seismic performance of the structure can be overestimated when the existing limits are used.

Formation of amorphous and crystalline phase, phase sequence by solid state reaction in Co/Si multilayer thin films (Co/Si 다층박막에서의 고상반응에 의한 비정질상과 결정상의 생성 및 상전이)

  • Sim, Jae-Yeop;Park, Sang-Uk;Ji, Eung-Jun;Gwak, Jun-Seop;Choe, Jeong-Dong;Baek, Hong-Gu
    • Korean Journal of Materials Research
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    • v.4 no.3
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    • pp.301-311
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    • 1994
  • The growth of amorphous and first crystalline phase, and phase sequence by solid state reaction were examined in Co/Si multilayer thin films by DSC and XRD. The experimental results were compared with the results expected by effective driving force models, PDF and effective heat of formation models.Amorphous phase growth was not observed in Co/Si system and it was consistent with the predicted result by effective driving force. It was observed that the first crystalline phase is CoSi. According to the PDF and effective heat of formation models, the first crystalline phases were CoSi and $CO_2Si$, respectively. The experiemental results were coincident with the PDF model considering structure factors. In case of the atomic concentration ratios of 2Co : 1Si and 1Co : 2Si, the phases sequences were $CoSi\to Co_2Si$ and $CoSi \to Co_2Si \to CoSi \to CoSi_2$, respectively and it was analysized through the effective heat of formation model. The formations of CoSi, $CO_2Si$ and $COSi_2$ in initial stage were controlled by nucleation and the activation energies for the nucleation of three phases were 1.71, 2.34 and 2.79eV.

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수소처리와 후성장층의 특성이 다이아몬드 박막의 전계방출 특성에 미치는 영향

  • 심재엽;송기문;이세종;백홍구
    • Proceedings of the Korean Vacuum Society Conference
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    • 2000.02a
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    • pp.96-96
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    • 2000
  • 화학증착법으로 증착된 다이아몬드 박막은 우수한 전기적 특성과 뛰어난 화학적, 열적 안정성 때문에 전계방출소재로 많은 관심을 불러 일으키고 있다. 다이아몬드 박막의 전계방출은 저전계에서 일어나는 것으로 알려져 있으며, 저전계방출의 원인을 규명하려는 많은 연구가 진행되어 왔다. 한편, 다이아몬드 박막의 전계방출전류는 금속기판의 사용에 의한 기판/다이아몬드 접촉의 개선, 다이아몬드 박막내의 흑연성분의 조절에 의한 구조변화, 보론이나 인 (P), 질소의 도핑, 수소 플라즈마나 cesium 등의 금속을 이용한 표면처리 등의 여러 방법에 의하여 향상된다는 것이 입증되었다. 그 외에 메탄과 대기 분위기 처리, 암모니아 분위기에서의 레이저 조사도 전계방출특성을 향상시키는 것으로 보고되었다. 그러나, 다이아몬드 박막의 성장후 구조적 특성이 다른 박막의 후성장이나 열분해된 운자수소 처리가 다이아몬드 박막의 전계방출특성에 미치는 영향에 관한 연구는 지금까지 이루어지지 않았다. 본 연구에서는 수소처리와 후성장이 다이아몬드 박막의 전계방출특성에 미치는 영향을 고찰하고 이로부터 그 원인을 규명하고자 하였다. 다이아몬드 박막은 hot-filament 화학증착법을 이용하여 증착하였다. 후성장한 다잉아몬드 박막내의 흑연성분과 박막의 두께를 체계적으로 조절하여 후성장 박막의 구조적 특성과 그 두께의 영향을 확인할 수 있었다. 후성장층내의 흑연성분과 두께가 증가할수록 전계방출특성은 향상되다가 저하되었다. 한편, 다이아몬드 박막을 성장시킨 후 수소분위기 처리를 함에 따라 전계방출특성은 향상되었지만 수소처리시간이 5분 이상으로 증가함에 따라 그 특성은 저하되었다. 본 연구에서는 수소처리와 후성장시 나타나는 전계방출특성의 변화 원인을 규명하고자 한다.기판위에서 polymer-like Carbon 구조는 향상되는 경향을 보였다.0 mm인 백금 망을 마스크로 사용하여 실제 3차원 미세구조를 제작하여 보았다. 그림 1에서 제작된 구조물의 SEM 사진을 보여주었으며, 식각된 면의 조도가 매우 뛰어나며 모서리의 직각성도 우수함을 확인할 수 있다. 이와 같이 도출된 시험 조건을 기초로 하여 리소그래피 후에 전기 도금을 이용한 금속 몰드 제작 및 이온빔 리소그래피 장점을 최대한 살릴수 있는 미세구조 제작에 대한 연구를 계속 추진할 계획이다. 비정질 Si1-xCx 박막을 증착하여 특성을 분석한 결과 성장된 박막의 성장률은 Carbonfid의 증가에 따라 다른 성장특성을 보였고, Silcne(SiH4) 가스량의 감소와 함께 박막의 성장률이 둔화됨을 볼 수 있다. 또한 Silane 가스량이 적어지는 영역에서는 가스량의 감소에 의해 성장속도가 둔화됨을 볼 수 있다. 또한 Silane 가스량이 적어지는 영역에서는 가스량의 감소에 의해 성장속도가 줄어들어 성장률이 Silane가스량에 의해 지배됨을 볼 수 있다. UV-VIS spectrophotometer에 의한 비정질 SiC 박막의 투과도와 파장과의 관계에 있어 유리를 기판으로 사용했으므로 유리의투과도를 감안했으며, 유리에 대한 상대적인 비율 관계로 투과도를 나타냈었다. 또한 비저질 SiC 박막의 흡수계수는 Ellipsometry에 의해 측정된 Δ과 Ψ값을 이용하여 시뮬레이션한 결과로 비정질 SiC 박막의 두께를 이용하여 구하였다. 또한 Tauc Plot을 통해 박막의 optical band gap을 2.6~3.7eV로 조절할 수 있었다. 20$0^{\circ}C$이상으로 증가시켜도 광투과율은 큰 변화를 나타내지 않았다.부터

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