• 한국습지학회지
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• 제15권2호
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• pp.251-264
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• 2013

도요 물떼새들은 만조시에 해안 내륙 휴식지에서 휴식을 취하는데, 휴식지를 선택할 때 여러 가지 요소들을 고려한다. 우리는 도요 물떼새 8종(알락꼬리마도요 Numenius madagascariensis, 청다리도요 Tringa nebularia, 큰뒷부리도요 Limosa lapponica, 개꿩 Pluvialis squatarola, 민물도요 Calidris alpine, 중부리도요 Numenius phaeopus, 마도요 Numenius arquata, 뒷부리도요 Xenus cinereus)을 대상으로 휴식지의 시공간적 이용과 그 이용에 영향을 미치는 요인들을 분석하였다. 휴식지 내 고인 물의 면적과 길이, 기온, 풍속, 종별로 이동시기, 방해정도를 변수로 고려하였다. 시공간적으로, 이용하는 종이 달랐으며 개체수 또한 변동을 거듭하였다. 그리고 도요 물떼새의 휴식지 이용에 영향을 미치는 요인은 종-특이적이었다. 연구지역의 휴식지는 폐장한 새우양식장이었으나 조사 기간 중 염생습지에서 자라는 함초 Salicornia herbacea 농장으로 전환하였다. 휴식지가 필요한 상황에서, 도요 물떼새들의 생태를 기초로 해서 기존 휴식지를 관리할 것을 권한다. 더불어, 여름철 가뭄에는 양식장의 수문을 열어주어 도요 물떼새들이 물을 이용해 체온관리를 할 수 있게 해주고, 만조시 도요 물떼새들이 양식장 안으로 날아 들어올 수 있도록 새들이 휴식지를 찾기 시작하는 만조 전네 시간부터는 농장 작업을 안 할 것을 권한다.

• 한국재료학회지
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• 제10권9호
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• pp.629-635
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• 2000

본 논문에서는 Ti-48.5at%Al-0.96at%Mo 조성을 갖는 $\gamma$-TiAl 합금은 항온 단조 및 후속 조직제어 열처리 시 발달하는 집합조직의 변화에 관해 연구하였다. 특히, 동적 재결정 후 조직제어 열처리 온도와 시간의 증가에 따라 발생하는 lamellar volume fraction 과 집합조직 변화에 주목하여 관찰하였다. 동적 재결정 후 집합조직은 ND$\perp${302) 선분과, TD$\perp${100) 및 이에 비해 상대적으로 다소 약한{111) 성분들이 발달하였으며, 열처리 온도와 시간이 증가함에 따라 lameller volume fraction 은 증가했고 동일한 성분의 집합조직도 점차 강하게 발달함을 알 수 있었다. 하지만 상온인장시험 결과는 lameller volume fraction이 증가할수록 낮은 상온 연신을 보였는데, 이는 준 층상조직을 갖는 $\gamma$-TiAl합금의 상온인장특성이 집합조직의 영향보다는 lameller volume fractio과 같은 미세조직 특성에 더욱 강하게 영향을 받기 때문인 것으로 판단된다.

• 한국해양공학회지
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• 제10권3호
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• pp.138-152
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• 1996

Many studies of heat transfer on the swirling flow or unswirled flow in a abrupt pipe expansion are widely carried out. The mechanism is not fully found evidently due to the instabilities of flow in a sudden change of the shape and appearance of turbulent shear layers in a recirculation region and secondary vortex near the corner. The purpose of this study is to obtain data through an experimental study of the swirling flow and heat transfer downstream of an abrupt expansion in a circular pipe with uniform heat flux. Experiments were carried out for the turbulent flow nd heat transfer downstream of an abrupt circular pipe expansion. The uniform heat flux condition was imposed to the downstream of the abrupt expansion by using an electrically heated pipe. Experimental data are presented for local heat transfer rates and local axial velocities in the tube downstream of an abrupt 3:1 & 2:1 expansion. Air was used as the working fluid in the upstream tube, the Reynolds number was varied from 60, 00 to 120, 000 and the swirl number range (based on the swirl chamber geometry, i.e. L/d ratio) in which the experiments were conducted were L/d=0, 8 and 16. Axial velocity increased rapidly at r/R=0.35 in the abrupt concentric expansion turbulent flow through the test tube in unswirled flow. It showed that with increasing axial distance the highest axial velocities move toward the tube wall in the case of the swirling flow abrupt expansion. A uniform wall heat flux boundary condition was employed, which resulted in wall-to-bulk temperatures ranging from 24.deg. C to 71.deg. C. In swirling flow, the wall temperature showed a greater increase at L/d=16 than any other L/d. The bulk temperature showed a minimum value at the pipe inlet, it also exhibited a linear increase with axial distance along the pipe. As swirl intensity increased, the location of peak Nu numbers was observed to shift from 4 to 1 step heights downstream of the expansion. This upstream movement of the maximum Nusselt number was accompanied by an increase in its magnitude from 2.2 to 8.8 times larger than fully developed tube flow values.

• 한국전기전자재료학회논문지
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• 제24권7호
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• pp.574-577
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• 2011

In this study, we use the $2.5cm{\times}7.5cm$ soda lime glass as the substrate. We used the ultrasonicator. Glass was dipped in the acetone, methanol and DI water respectively for 10 minutes. Ar(99.99%)gas was used as the sputtering gas. We varied the RF power between 100~175 W with 25 W steps. Base pressure was kept by turbo molecular pump at $3.0{\times}10^{-6}$ torr. Working pressure was kept by injection of Ar gas. ZnS thin films were deposited with the radio frequency magnetron sputtering technique at various temperatures and sputtering powers. It is also clearly observed that, the intensity of the (111) XRD peak increases with increasing the RF power. Electrical properties were measured by hall effect methods at room temperature. The resistivity, carrier concentration, and hall mobility of ZnS deposited on glass substrate as a function of sputtering power. It can be seen that as the sputtering power increase from 100 to 175 W, the resistivity of the films on glass decreased significantly from $8.1{\times}10^{-2}$ to $1.2{\times}10^{-3}\;{\Omega}{\cdot}cm$. This behavior could be explained by the effect of the sputtering power on the mobility and carrier concentration. When the RF power increases, the carrier concentration increases slightly while the resistivity decreases significantly. These variation originate from improved crystallinity and enhanced substitutional doping as the sputtering power increases.

• 한국재료학회지
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• 제12권6호
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• pp.452-457
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• 2002

Titanium oxide films were prepared by RF reactive magnetron sputtering. The effect of sputtering conditions on structural and optical properties was investigated systemically as a function of sputtering pressure(5~20 mTorr) and $O_2/Ar$ flow ratio(0.08~0.4). The results of the X-ray diffraction showed that all films had only the anatase $TiO_2$ phase. At low sputtering pressure and $O_2/Ar$ flow ratio, the films had preferred orientations along [101] and [200] directions. As the sputtering pressure and $O_2/Ar$ flow ratio increased, the intensity of the 101 and 200 diffraction peaks decreased gradually. The microstructure of the sputtered films showed the fine grain size (20nm~50nm) and columnar microcrystals perpendicular to the substrate. With increasing the sputtering pressure and decreasing $O_2/Ar$ flow ratio, the sputtered films showed the more porous columnar structure. XPS analysis showed that stoichiometric $TiO_2$ films were deposited at 7 mTorr sputtering pressure and 0.2 $O_2/Ar$ flow ratio. The results of the X-ray diffraction showed that all films had only the anatase $TiO_2$ phase. Ellipsometeric analysis showed that the refractive index increased from 2.32 to 2.46 as the sputtering pressure decreased. The packing density calculated using the refractive index varied from 0.923 to 0.976, indicating that $TiO_2$films became denser as the sputtering pressure decreased.

• 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.

• 전자공학회논문지SC
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• 제49권3호
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• pp.53-61
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• 2012

본 논문에서는 스테레오 적외선 카메라를 이용하여 소형 및 고온으로 날아가는 이동체의 거리를 실시간으로 측정하는 시스템을 제안한다. 이동체와 주변 환경의 온도 차이를 측정하고 고속으로 이동하는 소형 이동체의 거리를 자동으로 측정하기 위하여 적외선 스테레오 카메라 시스템을 구축하였다. 우선 적외선 카메라를 이용하여 취득한 고온의 이동체 영상으로부터 주변의 온도분포와 이동체간의 온도차를 이용하여 이동체영역을 검출하고, 이동체의 움직임 정보와 적외선 카메라 영상의 밝기정보를 결합하여 이동체를 추적한다. 좌우 적외선 카메라 영상에 대하여 각각 추출된 이동체 영역을 중심으로 스테레오 정합을 수행하여 시차정보를 추정하고, 카메라 파라미터와 시차정보를 이용하여 실시간으로 이동하는 이동체의 거리를 추정한다. 본 논문에서 제안하는 적외선 스테레오 카메라 시스템을 검증하기 위하여 고온의 이동체를 촬영할 때, 3차원 궤적(x,y,z) 측정기를 함께 가동하여 이동체가 이동하는 거리를 측정하여 이를 기준 거리(ground truth)로 설정하였다. 3차례의 비디오 데이터로부터 실험한 결과, 적외선 스테레오 카메라를 이용한 고온/소형 이동체의 거리오차 측정 결과는 평균적으로 9.68%로 추정되었다. 스테레오 적외선 카메라의 타이밍 문제(jitter)를 고려하면, 실제로 추정 오차는 줄어들 것으로 판단되기 때문에, 향후 적외선 카메라를 이용하는 다양한 이동체의 거리 및 위치를 측정하는데 응용할 수 있을 것으로 기대된다.

• 마이크로전자및패키징학회지
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• 제16권4호
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• pp.33-39
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• 2009

마스크리스 리소그래피(maskless lithography)에 응용하기 위한 마이크로렌즈 어레이(microlens array, MLA)가 석영의 습식 식각과 UV 접착제(UV adhesive)의 코팅을 바탕으로 개발되었다. 제작된 MLA의 초점거리는 ${\sim}45\;{\mu}m$ 정도였으며, 집광되는 광선의 초점은 ${\sim}1\;{\mu}m$로 측정되었다. MLA를 통과하며 초점을 맺은 빔(beam)의 크기 및 세기가 charge coupled device (CCD) 카메라와 빔 프로파일러(beam profiler)를 이용하여 각각 측정되었으며, 일정한 세기의 점들이 초점면에서 고르게 관찰되었다. 초점거리는 코팅된 UV 접착제의 두께에 따라 변화하였으며, UV 접착제의 두께가 두꺼울수록 짧아지는 경향을 보였다. 일반적인 마스크 얼라이너(mask aligner)를 이용한 MLA의 UV 포커싱(UV focusing)이 감광막(photoresist, PR) 상에서 실시되었으며, MLA를 통과한 빛이 감광막 위에 일정하게 집광되었다. 마스크 얼라이너와 MLA 사이의 거리 변화에 따라 감광막에 구현된 패턴 사이즈가 조절 되었다. 고온에서 오랜 시간이 지난 후에도 소자의 특성은 전혀 변함이 없었다.

• 생물환경조절학회지
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• 제4권1호
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• pp.9-16
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• 1995

고추 유묘의 생장, 광합성, 호흡 및 양수분흡수에 미치는 온도 및 주야변온의 영향을 구명하기 위하여 환경조절이 가능한 생장상내에서 실험을 수행한바 얻어진 결과는 다음과 같다. 1. 고추육묘시 적온으로 생각되는 $25^{\circ}C$에 비하여 온도가 12$^{\circ}C$로 저하함에 따라 수분 및 N, P, K 양분흡수에 현저한 감소를 보였으며, 5$^{\circ}C$에는 양수분의 흡수가 거의 이루어지지 않았다. 2. 엽의 광합성은 5$^{\circ}C$에서 $25^{\circ}C$까지는 점차적으로 증가되다가 $25^{\circ}C$에서 최대광합성을 보였으며, 엽과 근의 호흡은 온도가 증가할수록 계속 증가하였다. 3. 지하부 건물중이 가장 높은 적정 주야온도조합은 주간 3$0^{\circ}C$와 야간 $25^{\circ}C$로 나타났고, 주/야 온도 25/$25^{\circ}C$, 30/15$^{\circ}C$, 25/15$^{\circ}C$, 15/$25^{\circ}C$, 10/$25^{\circ}C$ 간에는 큰 차이가 있었으며, 야간온도 5$^{\circ}C$에서는 주간온도에 관계없이 지상부 건물중 증가가 거의 없었다.

• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2002년도 Proceedings
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• pp.400-403
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• 2002

The fundamental experiments for measuring soft x-ray characteristics from the vacuum capillary are described. These experiments were primarily performed in order to generate line spectra such as x-ray lasers. The generator consists of a high-voltage power supply, a polarity-inversion ignitron pulse generator, a turbo-molecular pump, and a radiation tube with a capillary. A high-voltage condenser of 200 nF in the pulse generator is charged up to 20 kV by the power supply, and the electric charges in the condenser are discharged to the capillary in the tube after closing the ignitron. During the discharge, weakly ionized plasma forms on the inner and outer sides of a capillary. In the present work, the pump evacuates air from the tube with a pressure of about 1 mPa, and a demountable capillary was developed in order to measure x-ray spectra according to changes in the capillary length. In this capillary, the anode (target) and cathode elements can be changed corresponding to the objectives. The capillary diameter is 2.0 mm, and the length is adjusted from 1 to 50 mm. When a capillary with aluminum anode and cathode electrodes was employed, both the cathode voltage and the discharge current almost displayed damped oscillations. The peak values of the voltage and current increased when the charging voltage was increased, and their maximum values were -10.8 kV and 4.7 kA, respectively. The x-ray durations observed by a 1.6 ${\mu}$m aluminum filter were less than 30 ${\mu}$s, and we detected the aluminum characteristic x-ray intensity using a 6.8 ${\mu}$m aluminum filter. In the spectrum measurement, two sets of aluminum and titanium electrodes were employed, and we observed multi-line spectra. The line photon energies seldom varied according to changes in the condenser charging voltage and to changes in the electrode element. In the case where the titanium electrode was employed, the line number decreased with corresponding decreases in the capillary length. Compared with incoherent visible light, these rays from the capillary were diffracted and diffused greatly after passing through two slits.