• 한국안전학회지
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• 제29권6호
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• pp.9-14
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• 2014

Recently many efforts and researches have been done to cope with industrial facilities that require a low energy machines due to the gradual depletion of the natural resources. The fiber-reinforced composite materials in general have good properties and have the proper mechanical properties according to the change of the ply sequences and fiber distribution types. However, in the fiber-reinforced composite material, there are several problems, including fiber breaking, peeling, layer lamination, fiber cracking that can not be seen from the metallic material. Particularly, the fracture and delamination are likely to be affected by the thickness of the stacking laminates when the bi-material laminated structure is subjected to a load of the mixed mode. In this study, we investigated the effect of the thickness ratio of the difference in the CFRP/GFRP bi-material laminate composites by measuring the cracking behavior and the AE characteristics in a mixed mode loading, which may be generated in the actual structure. The results show that the thickness of the CFRP becomes more thick, the mode I energy release rate becomes a larger, and also the influence of mode I is greater than that of mode II. In addition, AE amplitude which shows the level of the damage in the structure was obtained the more damage in the CFRP with the thin thickness.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2007년도 추계학술대회 논문집
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• pp.147-148
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• 2007

Dye-sensitized solar cell using conversion of solar energy to electrical energy appeared that which solves a environmental matter. The dye-sensitized solar cell uses nano-crystalline oxide semiconductor for absorbing dye. The $TiO_2$ is used most plentifully. The efficiency of the dye-sensitized solar cell changes consequently in the particle size, morphology, crystallization and surface state of the $TiO_2$. In this paper, we report The effect of titania$(TiO_2)$ thickness on the performance of dye-sensitized solar cells. Using doctor blade method, It produced the thickness of the $TiO_2$ with $7\;{\mu}m,\;10\;{\mu}m,\;13\;{\mu}m$. The efficiency was the best from $10{\mu}m$. It had relatively low efficiency on the thickness from $7\;{\mu}m\;to\;13\;{\mu}m$. The reason why it presents low efficiency on $7\;{\mu}m$ thickness is that excited electrons can not be delivered enough due to thin thickness of $7\;{\mu}m\;TiO_2$. And The reason why it presents low efficiency on $13\;{\mu}m$ thickness is that thick $13\;{\mu}m\;TiO_2$ can not penetrate the sunlight enough.

• Structural Engineering and Mechanics
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• 제77권1호
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• pp.137-149
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• 2021

In engineering design, the axial equivalent elastic modulus of laminated FRP pipe was mostly calculated by the average elastic modulus method or the classical laminated plate theory method, which are based on relatively simplified assumptions, and may be not accurate enough sometimes. A new analytical calculation method for the axial equivalent elastic modulus of laminated FRP pipe was established based on three-dimensional stress state. By comparing the results calculated by this method with those by the above two traditional analytical methods and the finite element method, it is found that this method for the axial equivalent elastic modulus fits well not only for thin-walled pipes with orthotropic layers, but also for thick-walled pipes with arbitrary layers. Besides, the influence of the layer stacking on the axial equivalent elastic modulus was studied with this method. It is found that a proper content of circumferential layer is beneficial for improving the axial equivalent elastic modulus of the laminated FRP pipe with oblique layers, and then can reduce its material quantity under the premise that its axial stiffness remains unchanged. Finally, the meso-mechanical mechanism of this effect was analyzed. The improving effect of circumferential layer on the axial equivalent elastic modulus of the laminated FRP pipe with oblique layers is mainly because that, the circumferential fibers can restrain the rigid body rotations of the oblique fibers, which tend to cause the significant deformations of the pipe wall units and the relatively low axial equivalent elastic modulus of the pipe.

• 한국약용작물학회지
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• 제12권4호
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• pp.300-303
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• 2004

고추냉이 재식밀도가 생육 및 수량에 미치는 영향을 구명하기 위하며 소식구$(30{\times}25\;cm)$와 밀식구$(30{\times}15\;cm)$로 정식하고 시험한 결과 지상부 생육은 초장, 엽병장, 엽수, 분지수 등 모든 형질에서 소식구의 생육이 양호하였다. 근경의 생육 및 수량에서 개체별 근경은 소식구에서 우수하였으나 10a당 수량은 밀식구에서 높았으며 상품근경중도 많았다. 그러나 상품율은 소식구에서 높았다. 근경장의 분포는 소식구에서는 비교적 큰 12 cm 이상이 50%가 분포하였으나 밀식구에서는 10 cm 이하에 65%가 분포하여 큰 대조를 이루었다. 근경폭의 분포도 이와 비슷하여 소식구에서는 27 mm 이상에 50%가 분포하였고, 밀식구에서는 27 mm 이하에 75%가 분포하였다. 그러나 등급별 분포는 소식구와 밀식구간에 큰 차이가 없었다.

• 수산해양기술연구
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• 제24권1호
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• pp.44-49
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• 1988

본 연구에서는 피로파괴에 영향을 주는 여러 인자중에서 우선 피로크랙전파에 대한 시험편 두께의 영향을 검토하기 위하여 최초 두께 25mm인 일반구조용 압연강재를 평면가공하여 두께 5, 10, 15, 20, 25mm인 CT 시험편을 가공한 후 인장-인장편진반 복피로시험을 행하여 실험한 결과 다음과 같은 결론을 얻었다. 1. 피로수명이 가장 짧게 나타나는 임의의 시험편 두께가 존재하며, 본 실험의 경우에는 두께 15m인 시험편의 경우 피로수명이 가장 짧게 나타났다. 2. 피로크랙의 발생은 두께가 두꺼운 시험편의 경우가 늦지만 피로크랙 성장은 두꺼운 시험편의 경우가 빠르게 나타났다. 3. 본 실험에서 paris시의 계수 m의 값은 절위는 1.98~4.59로서 시험편의 두께가 두꺼울수록 m의 값이 크게 된다.

• 한국자기학회지
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• 제10권5호
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• pp.196-202
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• 2000

FeMn에 의해 교환 바이어스된 Synthetic antiferromagnet(CoFe/Ru/CoFe)을 가진 Top Ta/NiFe/CoFe/Cu/CoFe/Ru/CoFe/FeMm/Ta 스핀밸브 구조를 마그네트론 스퍼터링 법으로 제조하여 유효 교환이방성 및 자기저항 특성을 조사하였다. FeMn 반강자성층의 두께가 100$\AA$정도일 때 자기저항비와 유효 교환바이어스 자장이 최대값을 나타내었으며, 100 $\AA$ 이상 두께 증가시 FeMn층을 통한 션팅 전류에 의한 자기저항 효율의 저하로 자기저항이 점점 감소하였다. 자유층의 두께가 40 $\AA$일 때 7.5% 이상의 최대 자기저항비가 얻어졌으며, 자유층의 두께 감소에 따라 자기저항비는 감소하였다. Synthetic antiferrormagnet 구조에서 Cu층에 인접한 CoFe(Pl)층의 두께를 증가시키고 FeMn층에 인접한 CoFe(P2)층의 두께를 감소시켜 그 두께 차이가 증가할수록 자기저항비는 증가하였고 반면 유효 교환 바이어스 자장은 감소하였다. 자기저항특성의 증가는 Pl층 두께 증가로 인한 스핀의존산란 효율의 증가로 이해되었으며, 유효 교환 바이어스 자장의 감소는 최소에너지 모델의 이론적 계산을 통해 감소경향을 검증할 수 있었다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2010년도 하계학술대회 논문집
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• pp.264-264
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• 2010

Single-walled carbon nanotubes (SWCNTs) were grown on a Si wafer by using thermal chemical vapor deposition (t-CVD). We investigated the effect of the catalyst deposition rate on the types of CNTs grown on the substrate. In general, smaller islands of catalyst occur by agglomeration of a catalyst layer upon annealing as the catalyst layer becomes thinner, which results in the growth of CNTs with smaller diameters. For the same thickness of catalyst, a slower deposition rate will cause a more uniformly thin catalyst layer, which will be agglomerated during annealing, producing smaller catalyst islands. Thus, we can expect that the smaller-diameter CNTs will grow on the catalyst deposited with a lower rate even for the same thickness of catalyst. The 0.5-nm-thick Fe served as a catalyst, underneath which Al was coated as a catalyst support as well as a diffusion barrier on the Si substrate. The catalyst layers were. coated by using thermal evaporation. The deposition rates of the Al and Fe layers varied to be 90, 180 sec/nm and 70, 140 sec/nm, respectively. We prepared the four different combinations of the deposition rates of the AI and Fe layers. CNTs were synthesized for 10 min by flowing 60 sccm of Ar and 60 sccm of $H_2$ as a carrier gas and 20 sccm of $C_2H_2$ as a feedstock at 95 torr and $810^{\circ}C$. The substrates were subject to annealing for 20 sec for every case to form small catalyst islands prior to CNT growth. As-grown CNTs were characterized by using field emission scanning electron microscopy, high resolution transmission electron microscopy, Raman spectroscopy, UV-Vis NIR spectroscopy, and atomic force microscopy. The fast deposition of both the Al and Fe layers gave rise to the growth of thin multiwalled CNTs with the height of ${\sim}680\;{\mu}m$ for 10 min while the slow deposition caused the growth of ${\sim}800\;{\mu}m$ high SWCNTs. Several radial breathing mode (RBM) peaks in the Raman spectra were observed at the Raman shifts of $113.3{\sim}281.3\;cm^{-1}$, implying the presence of SWCNTs (or double-walled CNTs) with the tube diameters 2.07~0.83 nm. The Raman spectra of the as-grown SWCNTs showed very low G/D peak intensity ratios, indicating their low defect concentrations.

• 마이크로전자및패키징학회지
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• 제28권4호
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• pp.41-45
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• 2021

본 연구에서는 멤리스터 소자의 높은 신뢰성을 확보하기 위해 소자 제작 단계에서 30 nm 두께의 ZrO₂ 금속산화물 박막 위 국부영역에 리튬 filament seed 층을 패턴하여 작은 이온반경의 리튬이온을 저항변화 주체로 활용하는 멤리스터 소자를 구현하였다. 패턴 된 리튬 filament seed 대비 다양한 상부전극의 면적을 적용하여 멤리스터-커패시턴스 병렬 구조의 이온형 저항변화 소자에서 커패시턴스가 filament type 저항변화 특성에 미치는 영향을 조사하고자 하였다. 이를 위해 ZrO₂ 박막 위에 5 nm 두께, 5 ㎛ × 5 ㎛ 면적의 리튬 filament seed 증착 후 50 ㎛, 100 ㎛ 직경의 상부전극을 증착, 리튬 메탈의 확산을 위한 250℃ 열처리 전 후 샘플에서 저항변화 특성을 확인하였다. 열확산에 의해 형성된 전도성 filament의 경우 전압에 의한 제어가 불가함을 확인하였으며, 전압에 의해 형성된 filament만이 electrochemical migration에 의한 가역적 저항변화 특성 구현이 가능한 것을 확인하였다. 전압에 의한 filament 형성 시 병렬로 존재하는 커패시턴스의 크기가 filament의 형성 및 소실에 중요한 인자임을 확인하였다.

• 한국자원식물학회지
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• 제34권1호
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• pp.37-43
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• 2021

본 연구는 참당귀 가공 시에 버려지는 부산물인 세미를 기능성 화장품 원료로 활용가능성이 있는지 평가하기 위해 수행하였다. MTS assay 수행결과 70% 주정을 이용한 뿌리 부위별 추출물의 경우 처리농도 25 ~ 200 ㎍/mL까지 세포독성이 없었다. 추출물 200 ㎍/mL를 처리하였을 때의 melanin 생성 억제효과는 추출 부위별로 12% ~ 19%로 나타났으며, 세미와 약재의 melanin 생성 억제효과가 비슷하게 나타났다. 그리고 DPPH radical 소거능이 50%에 달하는 IC50 값은 세미 677.9 ± 30.5 ㎍/mL, 약재 728.0 ± 42.4 ㎍/mL로 나타났고, ABTS radical 소거능이 50%에 달하는 IC50 값은 세미 114.9 ± 0.1 ㎍/mL, 약재 173.6 ± 1.3 ㎍/mL으로 나타나 세미가 약재보다 항산화활성이 높게 나타났다. 따라서 본 실험결과를 고려해 봤을 때, 부산물인 세미는 기능성 화장품 원료로 이용 가능성이 높은 것으로 생각된다.

• Steel and Composite Structures
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• 제36권4호
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• pp.447-462
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• 2020

The paper aims to investigate the mechanical mechanism and seismic effect of stiffeners in blind bolt endplate connection to CFST column. A precise 3D finite element model with considering the cyclic properties of concrete and steel materials was established, and the efficiency was validated through monotonic and cyclic test data. The deforming pattern and the seismic performance of the unstiffened and stiffened blind bolt endplate connections were investigated. Then a parametric analysis was conducted to analyze the contribution of stiffeners and the joint working behaviors with endplate under cyclic load. The joint stiffness classifications were compared and a supplement stiffness classification method was proposed, and the energy dissipation ability of different class connections were compared and discussed. Results indicated that the main deformation pattern of unstiffened blind bolt endplate connections was the local bending of end plate. The vertical stiffeners can effectively alleviate the local bending deformation of end plate. And influence of stiffeners in thin endplate and thick endplate was different. Based on the stiffness of external diaphragm welded connection, a more detailed rigidity classification was proposed which included the pin, semi-rigid, quasi-rigid and rigid connection. Beam was the main energy dissipation source for rigid connection. For the semi-rigid and quasi-rigid connection, the extended endplate, stiffeners and steel beam would all participate in the energy dissipation.