• 제목/요약/키워드: Focal length

검색결과 372건 처리시간 0.038초

Liquid Crystal Lens Array with Thermally Controllable Focal Length and Electrically Convertible Lens Type

  • Heo, Kyong Chan;Kwon, Jin Hyuk;Gwag, Jin Seog
    • Journal of the Optical Society of Korea
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    • 제19권1호
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    • pp.88-94
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    • 2015
  • This paper reports the fabrication of a lenticular liquid crystal (LC) lens array with thermally tunable focus and with the function of a convertible lens type, using the surface structure of a UV-curable polymer and a twisted-nematic (TN) LC cell. The TN LC cell makes the LC lenticular lens function as a converging or diverging lens by controlling electrically the polarization of input light. Therefore, the focal lengths for both the converging and diverging lenses, which can be switched from the TN cell, can be tuned by changing the effective refractive index of the LC by Joule heating of the transparent electrode. As a result, the focal length of the lens with the E7 LC was changed continuously from 8.7 to 31.2 mm for the converging lens type and from -9.8 to -14.2 mm for the diverging lens when the temperature was increased from 25 to $56^{\circ}C$.

비접촉 센서를 이용한 레이저 자동 포커싱 (Laser Auto Focus Using Non-Touch Sensor)

  • 장정원;김재구;신보성;장원석;최지연
    • 한국정밀공학회:학술대회논문집
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    • 한국정밀공학회 2003년도 춘계학술대회 논문집
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    • pp.280-283
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    • 2003
  • In this paper, there was finding laser beam focal length using the camera at the work with laser preprocess. A process have some similarity that the laser direct writing was condition of unused other light source in order to a partical object of working substrate, so we worked finding focal length using yellow light. As we found focal lengths from three points of substrate edges, The focal length of all substrates was able to be computed by calculating a plane equation using these three point. Also we make a device and software that can automatically perform all of the processes.

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공구날 특이길이의 물리적 적합성 고찰 (Physically Compatible Characteristic Length of Cutting Edge Geometry)

  • 안일혁;김익현;황지홍
    • 한국정밀공학회지
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    • 제29권3호
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    • pp.279-288
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    • 2012
  • The material removal mechanism in machining is significantly affected by the cutting edge geometry. Its effect becomes even more substantial when the depth of cut is relatively small as compared to the characteristic length which represents the shape and size of the cutting edge. Conventionally, radius or focal length has been employed as the characteristic length with the assumption that the shape of cutting edge is round or parabolic. However, in reality, there could be various ways to determine the radius or focal length even for the same tool edge profile, depending on the region to be considered as cutting edge in the measured profile and the constraints to be set in constructing the best fitted circle or parabola. In this regard, the present study proposes various models to determine the characteristic length in terms of radius or focal length. Their physical compatibility are validated by carrying out 2D orthogonal cutting experiments using inserts with a wide range of characteristic length ($30{\sim}180\;{\mu}m$ in terms of radius) and then by investigating the correlation between the characteristic length and the cutting forces. Such validation is based on the common belief that the larger the characteristic length is, the blunter the cutting edge is and the higher the cutting forces are. Interestingly, the results showed that the correlation is higher for the radius or focal length obtained with a constraint that the center of best fitted circle or the focus of the best fitted parabola should be on the bisectional line of the wedge angle of tool.

The Compound Refractive Lens for Hard X-ray Focusing

  • Choi, J.;Jung, J.;Park, S.;Kwon, T.
    • Journal of the Optical Society of Korea
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    • 제11권2호
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    • pp.76-81
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    • 2007
  • The compound refractive X-ray lens (CRL) for focusing hard X-rays is investigated to determine the parameters such as the focal length, the focal spot size, and spatial distribution at the focal spot using a simple theoretical calculations and CRLs fabricated by the self-assembly method. The number of individual compound lenses are defined for the given focal length of 1 m. The X-ray energy of 1 to 40 keV is used in the calculations. The CRL for focusing hard X-rays which generated from the X-ray tube is fabricated by nanoparticle-polymer composite in the form of circular concaves. The self-assembly method is applied to form the nanoaluminum-poly (methly meth-acrylate) composite and carbon-polymer composite CRL lenses. Aluminum nanoparticles of 100 nm and carbon microparticles are diffused in the polymer solution then the high gravity up to 6000G is applied in it to form the concave lens shape. X-ray energy at 8 keV is used for characterization of the composite CRLs. The FWHM of intensity for the fabricated nanoaluminium composite CRL system, N=10 is measured as 1.8 mm, which would give about $70{\mu}m$ in FWHM at 1 m of the focal length.

Virtual portraits from rotating selfies

  • Yongsik Lee;Jinhyuk Jang;SeungjoonYang
    • ETRI Journal
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    • 제45권2호
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    • pp.291-303
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    • 2023
  • Selfies are a popular form of photography. However, due to physical constraints, the compositions of selfies are limited. We present algorithms for creating virtual portraits with interesting compositions from a set of selfies. The selfies are taken at the same location while the user spins around. The scene is analyzed using multiple selfies to determine the locations of the camera, subject, and background. Then, a view from a virtual camera is synthesized. We present two use cases. After rearranging the distances between the camera, subject, and background, we render a virtual view from a camera with a longer focal length. Following that, changes in perspective and lens characteristics caused by new compositions and focal lengths are simulated. Second, a virtual panoramic view with a larger field of view is rendered, with the user's image placed in a preferred location. In our experiments, virtual portraits with a wide range of focal lengths were obtained using a device equipped with a lens that has only one focal length. The rendered portraits included compositions that would be photographed with actual lenses. Our proposed algorithms can provide new use cases in which selfie compositions are not limited by a camera's focal length or distance from the camera.

초점 조절이 가능한 디지털 유체 렌즈 (Digital Variable Focal Liquid Lens)

  • 이동우;조영호
    • 대한기계학회논문집A
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    • 제34권5호
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    • pp.557-560
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    • 2010
  • 본 논문에서는 4 비트 디지털구동기를 가변초점 유체렌즈에 적용하였다. 4 비트 디지털구동기는 총 16 단계로 렌즈곡면을 조절하여 렌즈의 초점을 변화시킨다. 본 가변초점 유체렌즈는 별도의 정밀 압력 및 유체량 제어기 없이 디지털구동기의 On/Off 제어만으로 렌즈곡면을 ${\pm}200nm$ 의 정밀도로 제어하여 초점거리를 3.63mm에서 38.6mm 까지 조절할 수 있다.

원거리 입체촬영용 카메라 축간거리 조절을 위한 퍼지추론 시스템 (Design of Fuzzy Inference System for Cameras Inter-Axial Distance Control of Remote Stereoscopic Photographs)

  • 변기식;오세웅;김관형;김민;김현조
    • 한국정보통신학회논문지
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    • 제19권1호
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    • pp.41-49
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    • 2015
  • 일반적으로 원거리 피사체를 입체로 촬영할 경우 두 대의 카메라를 교차하기 보다는 평행으로 놓고 좌우 영상을 획득한다. 이를 위해서 특정거리 피사체에 대하여 축간거리와 렌즈의 초점거리를 다양하게 변화시켜가면서 좌우영상들의 깊이총량을 분석하였다. 이들 분석 작업을 통하여 시각적 피로와 시각적 불안정을 주지 않는 축간거리와 렌즈의 초점거리에 대한 데이터를 선택하고, 이들 데이터를 통하여 퍼지제어기를 설계하였다. 피사체에 대한 입체영상을 획득하기 위하여 설계한 퍼지제어기로 축간거리와 렌즈의 최대초점거리를 추론하여 안정된 입체영상임을 확인하였다. 설계된 퍼지제어기는 원거리 피사체의 거리만 입력되면 카메라의 축간거리와 카메라 최대 초점거리 범위가 설정되는 동적 시스템 설계에 활용될 수 있음을 확인하였다.

태양열 집광기의 플럭스 밀도 분포 특성에 관한 연구 (An Experimental Study on the Characteristics of Flux Density Distributions produced by Solar Concentrating System)

  • 강명철;강용혁;윤환기;유창균
    • 한국신재생에너지학회:학술대회논문집
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    • 한국신재생에너지학회 2005년도 춘계학술대회
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    • pp.422-426
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    • 2005
  • This experimental study represents the results of an analysis on the characteristics of flux density distribution in the focal region of solar concentrator. The characteristics of flux density distributions are investigated to optimally design and position a cavity receiver. This was deemed very useful to find and correct various errors associated with a dish concentrator. We estimated the flux density distribution on the target placed along with focal lengths from the dish vertex to experimentally determine the focal length. It is observed that the actual focal point exists when the focal length is 2.17m. The total integrated power and percent power was 2467W and $85.8\%$, respectively, in the case of small dish, and also 2095W and $79\%$, respectively, in the case of KIERDISH II. As a result of the percent power within radius, approximately $90\%$ of the incident radiation is intercepted by about 0.06 m radius. The minimum radius of receiver in KIERDISH II is found to be 0.15m and approximately $90\%$ of the incident radiation is intercepted by receiver aperture.

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FIB 가공 공정 특성 분석 (The analysis of sputtering characteristics using Focused Ion Beam according to Focal Length)

  • 최병열;최우천;강은구;홍원표;이석우;최헌종
    • 한국정밀공학회:학술대회논문집
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    • 한국정밀공학회 2005년도 춘계학술대회 논문집
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    • pp.1518-1521
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    • 2005
  • The application of focused ion beam (FIB) technology in micro/nano machining has become increasingly popular. Its usage in micro/nano machining has advantages over contemporary photolithography or other micro/nano machining technologies such as small feature resolution, the ability to process without masks and being accommodating for a variety of materials and geometries This paper focus to apply the sputtering technology accumulated by experiments to 3d structure fabrication with high resolution. Therefore some verifications and discussions of the characteristics of FIB sputtering results according to focal length were described in this paper. And we suggested the definition of rectangular pattern profile and made the verifications of sputtering results based on definition of it.

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마이크로 유체렌즈를 이용한 마이크로 PIV 측정에 관한 실험적 연구 (Experimental Study on Micro PIV Measurement using a Micro Liquid Lens)

  • 정성룡;당중덩;최진호;김규만;박철우
    • 한국가시화정보학회지
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    • 제8권3호
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    • pp.22-28
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    • 2010
  • In the present study, we performed the velocity field measurement in a microchannel using a focal length variable micro liquid lens. The liquid lens is used as a beam expander in a micro-PIV system to acquire the scatter image of the seeded particle. A thin film-type micro liquid lens was made of PDMS material and it was attached on top of the 700-micron-wide working fluid supply channel trench. As a result, the focal length and contact angle of the liquid lens changed with variations in applied pressure.