• 제목/요약/키워드: orientation target

검색결과 305건 처리시간 0.024초

무인항공 사진측량을 이용한 3D 공간정보 취득 (Acquisition of 3D Spatial Information using UAV Photogrammetric Method)

  • 정성혁;임형민;이재기
    • 한국측량학회지
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    • 제28권1호
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    • pp.161-168
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    • 2010
  • 본 연구에서는 무인항공기로 촬영한 영상을 이용하여 변화가 매우 빈번히 발생하는 도시지역의 3차원 정보를 신속하게 취득하는 기법을 제시하고 처리공정을 개발하였다. 연구에서 제안된 무인항공기를 이용한 사진측량기법은 저가의 무인항공기와 비측량용 카메라를 이용하였으며, 카메라 검정을 통하여 내부표정요소를 취득하였다. 연구 대상지역을 촬영한 영상자료와 기준검측량성과로부터 인공지물의 3차원 모형을 제작하였으며 토목공사로 인하여 변화가 발생한 지형을 대상으로 수치지형모형을 제작하였다. 1/1,000 축척의 수치지도 및 지상 기준점 측량성과와 비교하여 본 기법의 효용성을 분석하였으며 이상과 같은 연구를 통하여 3차원 가상도시 구축, 3D GIS 데이터베이스 갱신, 지형 지물 변화정보 추출 및 수치지도 수시갱신에 활용할 수 있는 가능성을 제시하였다.

Spin and shape analysis for the Mars-crossing asteroid 2078 Nanking

  • Choi, Jung-Yong;Kim, Myung-Jin;Choi, Young-Jun;Yoon, Tae Seog
    • 천문학회보
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    • 제40권1호
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    • pp.85.2-86
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    • 2015
  • The YORP effect is non-gravitational force that changes the spin-status of asteroid. So far this effect has been directly detected only from the Near-Earth asteroids (Taylor et al. 2007; Lowry et al. 2007, 2014; Breiter et al. 2011; Durech et al. 2008, 2012). Pravec at el. 2008 found the evidences for changing spin rate of small asteroids (3 - 15 km) by the YORP effect in the Main-Belt and Mars-crossing asteroids. The Mars-crossing asteroids (1.3 < q < 1.66 AU) are objects that cross orbit of the Mars. The Mars-crossing asteroids are regarded as one of the main sources for the Near-Earth asteroids. We expect that rotation of Mars-crossing asteroids would be influenced by the YORP effect. We try to search observational evidence of the YORP effect for the Mars-crossing asteroid. Our target 2078 Nanking is a population of the Mars-crossing asteroid. First light-curve of 2078 Nanking was obtained from Mohamed et al. 1994, and Warner et al. 2015 recently published new observational data. We observed this asteroid on 26th Nov. 2014 and 17th Jan. 2015 using SOAO (Sobaeksan Optical Astronomy Observatory) 0.61 m telescope with 4K CCD. Using light-curve inversion method (Kaasalainen & Torppa 2001; Kaasalainen et al. 2001), we try to determine the pole orientation and shape model of this asteroid based on the combination of our light-curve and literature photometric data. Knowing spin parameters, such as rotational period and spin axis, are essential for studying the YORP effect. In this presentation, we provide some preliminary results of our recent study: light-curve and processing of shape modeling of 2078 Nanking. We plan to find observational clue for the YORP effect on the Mars-crossing asteroids.

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부동산 유형별 마케팅 전략이 만족도에 미치는 영향요인 분석 (Analysis of Influence Factors of Satisfaction by Marketing Strategic Based on the Type of Real Estate)

  • 김구회;이길재;원유호
    • 지적과 국토정보
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    • 제44권1호
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    • pp.195-212
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    • 2014
  • 본 연구는 부동산 분양 및 개발 사업의 성패에 큰 영향을 미치는 부동산 마케팅 전략의 영향요인을 구축하고, 유형별 만족도의 영향요인을 PLS 회귀분석을 통해 도출하고자 한다. 자료 구축은 부동산 분양 및 개발 사업을 전문으로 하는 집단을 대상으로 실시하였으며, 부동산 유형 분류는 사업적 분류방식에 의해 주거용(residential)과 비주거용(nonresidential)으로 구분한다. 분석결과 주거유형의 경우 브랜드 신뢰, 제휴 및 협력관계 강화, 교통환경, 분양 조건 완화, 사업설명회, 미분양 특전, 납부 조건 완화 요인이 중요하게 도출되었으며, 비주거유형의 경우 납부 조건 완화, 고객지향성, 생활환경, 제휴 및 협력관계 강화, 커뮤니케이션 요인이 만족도에 영향을 주는 것으로 도출되었다.

퍼지시스템과 포텐셜 필드를 이용한 다중 이동로봇의 충돌회피 최적경로 연구 (Study on the Collision Free Optimal Path for Multi Mobile Robots Using Fuzzy system and Potential Field)

  • 이종호;김동원
    • 전자공학회논문지 IE
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    • 제47권2호
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    • pp.66-72
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    • 2010
  • 자율적인 다중이동 로봇환경에서는 현시점에서 목표점까지 장애물과 충돌없이 연결하는 최적 경로를 설정하는 것은 필수불가결하며 매우 중요하다. 실제 많은 이동로봇은 주위 장애물에 대하여 주어진 정보 없이 미지의 환경에서 자율적 이동이 가능해야 한다. 따라서 본 논문에서는 다중이동 로봇환경에 적합한 새로운 형태의 충돌회피 최적경로에 대한 방법을 연구한다. 잘 알려진 포텐셜필드 방법을 이용하여 다중이동 로봇의 전역경로를 계획하고, 퍼지로직 시스템을 이용하여 각 로봇에 근접하는 혹은 경로를 가로막는 장애물과의 충돌을 피하기 위한 지역경로를 계획한다. 제안된 방법의 성능 및 정확성을 검증하기 위해 다양한 모의실험을 진행하여 결과를 검증하고 이의 결과를 토의한다.

Electrical Properties and Microstructures in Ti Films Deposited by TFT dc Sputtering

  • Han, Chang-Suk;Jeon, Seung-Jin
    • 한국재료학회지
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    • 제26권4호
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    • pp.207-211
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    • 2016
  • Ti films were deposited on glass substrates under various preparation conditions in a chamber of two-facing-target type dc sputtering; after deposition, the electric resistivity values were measured using a conventional four-probe method. Crystallographic orientations and microstructures, including the texture and columnar structure, were also investigated for the Ti films. The morphological features, including the columnar structures and surface roughness, are well explained on the basis of Thornton's zone model. The electric resistivity and the thermal coefficient of the resistivity vary with the sputtering gas pressure. The minimum value of resistivity was around 0.4 Pa for both the $0.5{\mu}m$ and $3.0{\mu}m$ thick films; the apparent tendencies are almost the same for the two films, with a small difference in resistivity because of the different film thicknesses. The films deposited at high gas pressures show higher resistivities. The maximum of TCR is also around 0.4 Pa, which is the same as that obtained from the relationship between the resistivity and the gas pressure. The lattice spacing also decreases with increasing sputtering gas pressure for both the $0.5{\mu}m$ and $3.0{\mu}m$ thick films. Because they are strongly related to the sputtering gas pressures for Ti films that have a crystallographic anisotropy that is different from cubic symmetry, these changes are well explained on the basis of the film microstructures. It is shown that resistivity measurement can serve as a promising monitor for microstructures in sputtered Ti films.

기판온도가 ZnO 박막의 특성에 미치는 영향 (Influence of the Substrate Temperature on the Characterization of ZnO Thin Films)

  • 정양희;권오경;강성준
    • 한국정보통신학회논문지
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    • 제10권12호
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    • pp.2251-2257
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    • 2006
  • ZnO 박막을 RF sputtering 법을 이용하여 제작한 후, 기판 온도에 따른 결정성, 표면 형상, c 축 배향성, 박막의 밀도 등을 조사하여 압전 소자로의 적용 가능성을 조사하였다. 본 연구에서는 $Ar/O_2$ 혼합비 70/30, sputtering 파워 125 W, 공정 압력 8 mTorr, 기판 타겟간 거리 70 mm로 공정 변수를 고정시키고, 기판 온도를 상온에서 $400^{\circ}C$까지 변경하면서 ZnO 박막을 증착하였다. 기판온도가 $300^{\circ}C$ 일 때, (002) 피크의 상대 강도비 (I(002)/I(100))가 94%로 가장 크게 나타났으며, 이 때의 반가폭은 $0.571^{\circ}$ 이었다. SEM과 AFM을 통한 표면 형상은 $300^{\circ}C$ 일 때 균일한 입자형태를 띄면서 4.08 nm의 가장 우수한 표면 거칠기를 나타내었다. ZnO 박막의 밀도는 기판 온도가 상온에서부터 $300^{\circ}C$ 까지 상승함에 따라 증가하는 추세를 나타내었으며, 이 후 기판 온도가 $400^{\circ}C$로 증가하면 다시 감소하는 경향을 나타내었다.

X-Ray Absorption Spectroscopic Study of 120 MeV $Ag^{9+}$ Ion-Irradiated N-Doped ZnO Thin Films

  • Gautam, Sanjeev;Lim, Weon Cheol;Kang, Hee Kyung;Lee, Ki Soo;Song, Jaebong;Song, Jonghan;Asokan, K.;Chae, Keun Hwa
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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    • pp.315-315
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    • 2013
  • We report the electronic structure modification in the swift heavy ion (SHI) irradiated N-doped ZnO thin films prepared by RF sputtering from ZnO target in different ratio of Ar/$N_2$ gas mixture using highly pure $N_2$ gas. The different N-ZnO thin lms were then irradiated with 120 MeV Ag ion beam with different doses ranging from $1{\times}10^{11}$ to $5{\times}10^{12}$ ions/$cm^2$ and characterized by XRD and near edge X-ray absorption ne structure (NEXAFS) at N and O K-edges. The NEXAFS measurements provide direct evidence of O 2p and Zn 3d orbital hybridization and also the bonding of N ions with Zn and O ions. The minimum value of resistivity of $790{\Omega}cm$, a Hall mobility of $22cm^2V^-1s^-1$ and the carrier concentration of $3.6{\times}10^{14}cm^{-3}$ were yielded at 75% $N_2$. X-ray diffraction (XRD) measurements revealed that N-doped ZnO films had the preferential orientation of (002) plane for all samples, while crystallinity start decreasing at 32.5% $N_2$. The average crystallite size varies from 5.7 to 8.2 nm for 75% and then decreases to 7.8 nm for 80% $Ar:N_2$ ratio.

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내러티브분석을 통해 본 케이블TV 여성전문채널 뷰티.패션 프로그램 시청자의 소비경험이야기 (Beauty-Fashion Program of CATV Audiences' Consumption Stories by a Narrative Analysis)

  • 유현정;송유진
    • 한국생활과학회지
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    • 제17권1호
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    • pp.57-80
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    • 2008
  • The contemporary consumers have insatiable desires for material and outward appearance. In terms of the desire for outward appearance, people recognize that a beautiful outward appearance can be made by an artificial effort. Subsequently, the interest in a beauty and fashion has been increased. In addition, a cable TV shows a beauty and fashion program targeted for women in 20s to 30s. This study tried to examine the stories on experience of consumption by consumers watching a beauty and fashion program in a women specialized channel of a cable TV. The total number of narrators who participated in this study was 11. Among them, we formed 26 narrative plots on the basis of interviews for 7 persons who could use Labov's structural analysis. The result of analyzing narrators' narrative plots was as follows: First, although narrators received the information on beauty and fashion through a channel which became the target of this study, they applied such information into an ordinary life by transforming such information. Second, narrators thought that their confidence and superiority could be expressed through a beauty and fashion. Third, narrators' consuming life showed a showing off-type consumption and an objective consumption. Fourth, narrators have a gap between the behavior orientation and real actions. And they experiences various trobles on consumption life. Fifth, through the interview for narrators, a trend of reconsidering their consuming life was found out.

입자크기에 따른 SnO2:Ni 가스센서의 감응 특성 (Effect of the Particle Size of SnO2:Ni on Gas Sensing Properties)

  • 이지영;유일
    • 한국재료학회지
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    • 제21권4호
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    • pp.207-211
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    • 2011
  • Ni 8 wt.%-doped tin oxide ($SnO_2$) thick films were fabricated into gas sensors by the method of screen printing onto alumina substrates. The particle size of $SnO_2$ was controlled by changing the ball-mill time between 0~120 h. The structural and morphological properties of these thick films were investigated using X-ray diffraction and scanning electron microscopy. The structural properties of $SnO_2$ powders showed a tetragonal phase with (110) dominant orientation. The particle size of the $SnO_2$:Ni powders after ball-mill of 120 h was about 0.05 ${\mu}m$. The gas sensitivity (S = Rg/Ra) to 5 ppm $CH_4$ gas and $CH_3CH_2CH_3$ gas was measured at room temperature by comparing the resistance in air (Ra) with that of the target gases (Rg). The sensitivity of the $SnO_2$ gas sensors was enhanced by increasing the ball-mill time. There was an association between the sensitivity of both the $CH_4$ gas and the $CH_3CH_2CH_3$ gas and the particle size of the $SnO_2$. $SnO_2$ gas sensors prepared by 72 h ball-mill showed a sensitivity of about 13 to 5 ppm $CH_4$ gas and $CH_3CH_2CH_3$ gas. The response time of the $SnO_2$:Ni gas sensors to the $CH_4$ gas was about 20 seconds.

Trajectory Studies of Methyl Radical Reaction with Iodine Molecule

  • Lee, Sang-Kwon;Ree, Jong-Baik;Kim, Yoo-Hang;Shin, Hyung-Kyu
    • Bulletin of the Korean Chemical Society
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    • 제26권9호
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    • pp.1369-1380
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    • 2005
  • The reaction of methyl radical with iodine molecule on an attractive potential energy surface is studied by classical trajectory procedures. The reaction occurs over a wide range of impact parameters with the majority of reactive events occurring in the backward rebound region on a subpicosecond scale. A small fraction of reactive events take place in the forward hemisphere on a longer time scale. The ensemble average of reaction times is 0.36 ps. The occurrence of reactive events is strongly favored when the incident radical and the target molecule align in the neighborhood of collinear geometry. Since the rotational velocity of I2 is slow, the preferential occurrence of reactive events at the collinear configuration of $CH_3{\ldots}I{\ldots}$I leads to the reaction exhibiting an anisotropic dependence on the orientation of $I_2$. During the collision, there is a rapid flow of energy from the $H_3C{\ldots}$I interaction to the I-I bond. The $CH_3I$ translation and $H_3C$-I vibration share nearly all the energy released in the reaction, and the distribution of the vibrational energy is statistical. The reaction probability is $\cong$0.4 at the $CH_3$ and I2 temperatures maintained at 1000 K and 300 K, respectively. The probability is weakly dependent on the $CH_3\;and\;I_2$ temperatures between 300 K and 1500 K.