• 제목/요약/키워드: Lens power

검색결과 335건 처리시간 0.026초

3차원 패터닝을 위한 레이저 헤드설계 및 열해석 (Laser Head Design and Heat Transfer Analysis for 3D Patterning)

  • 예강현;최해운
    • 한국기계가공학회지
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    • 제15권4호
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    • pp.46-50
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    • 2016
  • A laser head was designed for micro-scale patterning and joining applications. The target feature size of the pattern was $100{\mu}m$, and optics were designed to perform the target. Two singlet lenses were combined to minimize the chromatic aberration, and the geometry of the lenses was calculated by using the raytracing method with a commercial software program. As a restriction of lens design, the focal length was set at 100mm, and the maximum diameter of the lens or beam size was limited to 10mm for the assembly in the limited cage size. The maximum temperatures were calculated to be $1367^{\circ}C$, $1508^{\circ}C$, and $1905^{\circ}C$ for 10, 12, and 15 Watts of power, respectively. A specially designed laser head was used to compensate for the distance between the object and the lens. The detailed design mechanism and 3D data were presented. The optics design and detailed performance of the lens were analyzed by using MTF and spot diagram calculation.

유전체 렌즈를 가진 3~6GHz대용 UWB 시뉴어스 안테나 개발 (Development of UWB Sinuous Antenna with Dielectric Lens for 3~6 GHz Band Application)

  • 이동렬
    • 한국인터넷방송통신학회논문지
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    • 제15권6호
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    • pp.239-244
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    • 2015
  • 최근들어 임펄스 레이더에서 거리를 측정하기위한 센서로서 또는 비 압축 고속 영상데이터의 전송용으로 UWB 기술이 활발히 응용되고 있다. 그러나 UWB 기술은 대역이 옥타브 밴드로 매우 넓어서 시스템을 설계하기가 쉽지 않다. 특히 광대역 임피던스를 정합해야하는 안테나를 비롯한 RF분야에서 더욱 그렇다. 본 연구에서는 이러한 3~6GHz 옥타브 대역에서 사용할 수 있는 시뉴어스 안테나를 설계하고 제작하였다. 그리고 유전체 렌즈를 설계하여 부착하여 이득을 높이는 실험한 결과 3~6GHz 사용대역에서 6~10dBi의 높은 이득을 얻을 수 있었다. 제작된 유전체 부착 시뉴어스 안테나를 HD 비디오 데이터 전송에 사용하였다. 전송 결과 10mW의 무선전력으로 최대 전송 거리는 90m였다.

355nm UV 레이저를 이용한 마이크로 렌즈 어레이 쾌속 제작 (Rapid Fabrication of Micro Lens Array by 355nm UV Laser Irradiation)

  • 제순규;박강수;오재용;김광렬;박상후;고정상;신보성
    • 한국레이저가공학회지
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    • 제11권2호
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    • pp.26-32
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    • 2008
  • Micro lens array (MLA) is widely used in information technology (IT) industry fields, for examples such as a projection display, an optical power regulator, a micro mass spectrometer and for medical appliances. Recently, MLA have been fabricated and developed by using a reflow method, micro etching, electroplating, micromachining and laser local heating. Laser local thermal-expansion (LLTE) technology demonstrates the formation of microdots on the surface of polymer substrate, in this paper. We have also investigated the new direct fabrication method of placing the MLA on the surface of a SU-8 photoresist layer. We have obtained the 3D shape of the micro lens processed by UV laser irradiation and have experimentally verified the optimal process conditions.

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광압을 이용한 입자빔 집속 (Particle Beam Focusing Using Radiation Pressure)

  • 김상복;박형호;김상수
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2004년도 춘계학술대회
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    • pp.1505-1509
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    • 2004
  • A novel technique for fine particle beam focusing under the atmospheric pressure is introduced using a radiation pressure assisted aerodynamic lens. To introduce the radiation pressure in the aerodynamic focusing system, a 25 mm plano-convex lens having 2.5 mm hole at its center is used as an orifice. The particle beam width is measured for various laser power, particle size, and flow velocity. In addition, the effect of the laser characteristics on the beam focusing is evaluated comparing an Ar-Ion continuous wave laser and a pulsed Nd-YAG laser. For the pure aerodynamic focusing system, the particle beam width was decreased as increasing particle size and Reynolds number. For the particle diameter of 0.5 ${\mu}m$, the particle beam was broken due to the secondary flow at Reynolds number of 694. Using the Ar-Ion CW laser, the particle beam width becomes smaller than that of the pure aerodynamic focusing system about 16 %, 11.4 % and 9.6 % for PSL particle size of 2.5 ${\mu}m$, 1.0 ${\mu}m$, and 0.5 ${\mu}m$ respectively at the Reynolds number of 320. Particle beam width was minimized around the laser power of 0.2 W. However, as increasing the laser power higher than 0.4 W, the particle beam width was increased a little and it approached almost a constant value which is still smaller than that of the pure aerodynamic focusing system. The radiation pressure effect on the particle beam width is intensified as Reynolds number decreases or particle size increases relatively. On the other hand, using 30 Hz pulsed Nd-YAG laser, the effect of the radiation pressure on the particle beam width was not distinct unlike Ar-Ion CW laser.

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경남지역 대학생들의 난시 교정용 소프트 콘택트렌즈의 착용에 관한 설문조사 (A Survey about Wearing Soft Contact Lenses for Astigmatism Correction of The Local College Students, Gyeongsangnam-Do, Korea)

  • 김봉환;한선희;김대현;변상현;채정임;김재석;황윤정;김학준
    • 한국임상보건과학회지
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    • 제3권3호
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    • pp.378-389
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    • 2015
  • Purpose. The actual status of wearing toric soft contact lenses was investigated to learn why it is not used although it is required. Materials and Methods. This study has studied 64 contact lens wearing the local college students, Gyeongsangnam-do who are 20.17(${\pm}0.70$)years old, by measuring their refractive power and over-refractive power with auto refractometer(HRK-8000A, Huvitz, Korea). In addition to that, a survey was done to figure out why they do not wear toric soft contact lenses, the purpose of using toric soft contact lenses, whether they have astigmatism or any knowledge about it, the kinds of contact lens, whether they are willing to buy corrective lenses, and how they are satisfied after purchasing them. Results. 17 students (21.9%) said they experienced light-spread; 9 students (14.1%)said that they have dizziness when they wear contact lens all day long. In the survey to see whether they had astigmatism or not, 37 students (57.8%) said they had it. For the reason they do not wear toric soft contact lenses, 33 students (51.6%) said that "they were prescribed regardless of astigmatism in the optometrist." To the question asking if they are willing to buy toric soft contact lenses according to the existence of astigmatism, 51 students (79.6%) answered they are. 31 students (48.4%) said they heard a description about astigmatism at the time of purchase for contact lens. Conclusion. As the ways for any people who need to correct astigmatism to wear corrective lens, enough education about astigmatism and consistent follow-up management are needed, where the role of optometrist is considered important.

Comparison of Intraocular Lens Power Calculation Methods Following Myopic Laser Refractive Surgery: New Options Using a Rotating Scheimpflug Camera

  • Cho, Kyuyeon;Lim, Dong Hui;Yang, Chan-min;Chung, Eui-Sang;Chung, Tae-Young
    • Korean Journal of Ophthalmology
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    • 제32권6호
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    • pp.497-505
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    • 2018
  • Purpose: To evaluate and compare published methods of calculating intraocular lens (IOL) power following myopic laser refractive surgery. Methods: We performed a retrospective review of the medical records of 69 patients (69 eyes) who had undergone myopic laser refractive surgery previously and subsequently underwent cataract surgery at Samsung Medical Center in Seoul, South Korea from January 2010 to June 2016. None of the patients had pre-refractive surgery biometric data available. The Haigis-L, Shammas, Barrett True-K (no history), Wang-Koch-Maloney, Scheimpflug total corneal refractive power (TCRP) 3 and 4 mm (SRK-T and Haigis), Scheimpflug true net power, and Scheimpflug true refractive power (TRP) 3 mm, 4 mm, and 5 mm (SRK-T and Haigis) methods were employed. IOL power required for target refraction was back-calculated using stable post-cataract surgery manifest refraction, and implanted IOL power and formula accuracy were subsequently compared among calculation methods. Results: Haigis-L, Shammas, Barrett True-K (no history), Wang-Koch-Maloney, Scheimpflug TCRP 4 mm (Haigis), Scheimpflug true net power 4 mm (Haigis), and Scheimpflug TRP 4 mm (Haigis) formulae showed high predictability, with mean arithmetic prediction errors and standard deviations of $-0.25{\pm}0.59$, $-0.05{\pm}1.19$, $0.00{\pm}0.88$, $-0.26{\pm}1.17$, $0.00{\pm}1.09$, $-0.71{\pm}1.20$, and $0.03{\pm}1.25$ diopters, respectively. Conclusions: Visual outcomes within 1.0 diopter of target refraction were achieved in 85% of eyes using the calculation methods listed above. Haigis-L, Barrett True-K (no history), and Scheimpflug TCRP 4 mm (Haigis) and TRP 4 mm (Haigis) methods showed comparably low prediction errors, despite the absence of historical patient information.

주문형 렌즈의 규격 비교 연구 (A Comparative Study on Prescription Lenses Standards)

  • 문병연;백선목;유동식
    • 한국안광학회지
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    • 제14권1호
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    • pp.17-21
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    • 2009
  • 목적: 국산 주문용 시력보정 렌즈의 국제규격에 따른 품질을 평가하고, 분석하였다. 방법: 국내시장에서 유통되고 있는 국내 브랜드의 주문용 렌즈들을 대상으로 굴절력, 중심두께, 투과율을 측정하고, 국제규격에 따라 외국브랜드 제품과 비교, 분석하였다. 결과: 국산 제품들 중 국제규격의 허용기준에 맞지 않는 경우가 1제품 있었지만 굴절력, 투과율에서 대부분 우수한 특성을 보였다. 결론: 국내외 시장에서 외국제품들보다 더 높은 선호도를 가지기 위해 렌즈제조업체의 더 강화된 품질관리와 마케팅 전략이 필요하다.

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전면 굴절력과 굴절률이 착락원의 크기에 미치는 영향 (The Influence of the Front Surface Power and the Refraction Index on RMS Spot Diameter)

  • 박성종;신철근;주석희
    • 한국안광학회지
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    • 제8권2호
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    • pp.57-63
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    • 2003
  • 본 연구에서는 안경렌즈의 전면굴절력, 굴절률, 그리고 중심 두께의 변화에 따라 상측정점초점면에 맺는 착락원 직경 변화를 조사하기 위해 Code V와 LOSA 2.0 프로그램을 사용하였으며, 상측정점굴절력이 -4.00D이고 직경이 70 mm인 근시교정용 안경렌즈를 고려하였다. 또한 안경렌즈의 전면 굴절력은 0~10D, 중심 두께는 1.1~2.0mm 그리고 굴절률은 $n_d$ = 1.498, 1.523, 1.586, 1.60인 경우를 각각 고려하였다. 안경렌즈의 전면굴절력이 증가할수록 상측정점초점면에서 맺는 착락원 직경의 크기는 급격하게 증가하였다. 또한 안경렌즈의 굴절률이 증가한 경우에 상측정점초평면에 맺는 착락원 직경의 크기는 감소하였으며, 전면굴절력의 변화에 따른 착락원 직경의 크기 변화는 작았다. 안경렌즈의 중심 두께가 증가할수록 상측정점초평면에 맺는 착락원 직경 크기에는 거의 영향이 없지만 안경렌즈의 가장자리의 두께는 증가하였다. 이러한 결과로부터 구면렌즈의 경우에는 전면굴절력이 작고, 굴절률이 클수록 상측정점초평면에서 더 좋은 결상을 하고 있음을 알 수 있다.

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근시성 난시안에서 구면 RGP 콘택트렌즈의 난시교정 효과 (A Study of a Correction Effect of Astigmatism using Spherical RGP Lens)

  • 주석희;박혜정;신철근;심현석
    • 한국안광학회지
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    • 제8권2호
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    • pp.85-89
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    • 2003
  • 구면 RGP 렌즈는 렌즈 후면과 각막 사이에 눈물이 일정한 두께를 형성하면서 뛰어난 난시교정효과를 나타낸다. 이러한 RGP 렌즈의 난시교정 효과를 체계적으로 연구하여 임상 구면 RGP 렌즈처방에 활용하고자 렌즈착용 전후의 전체난시량 변화 각막난시량의 변화, 잔여난시 변화를 비교, 분석하여 다음과 같은 결론을 얻었다. 1. 구면 RGP 렌즈의 교정 전 후 전체난시량이 2.00D 이하에서는 교정이 거의 모두 이루어졌으나, 전체 난시량이 2.50D 이상에서 미교정된 상태를 보였으며, 특히 3.00D 이상에서는 난시 교정효과가 급격히 감소되는 것으로 나타났다. 2. 구면 RGP 렌즈의 교정 전 후 각막난시량은 2.50D 이하에서 약도의 저교정 상태로 나타났으나, 3.00D이상에서는 전체난시와 마찬가지로 난시 교정효과가 감소되는 것으로 나타났다. 3. 구면 RGP 렌즈 처방시 잔여난시량은 그대로 발현하는 것이 아니고, 잔여난시 도수가 일정부분 감소하여 전체난시 상태로 나타났다.

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CPV모듈의 2차 광학계 특성에 따른 성능분석 (Performance Analysis of CPV Modules for Optimizing Secondary Optical Elements)

  • 박점주;정병호;박주훈;이강연;김효진
    • 한국태양에너지학회 논문집
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    • 제40권5호
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    • pp.23-34
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    • 2020
  • Concentrator photovoltaic (CPV) system consists of high-quality complex optical elements, mechanical devices, and electronics components and can have the advantages of high integration and high-efficiency energy sources. III-V compound semiconductor cells have proven performance based on high reliability in the aerospace field, but have characteristics that require absolute support of the balance of systems (BOS) such as solar position trackers, receivers with heat sinks, and housing instruments. To determine the optimum parameters of secondary optical elements (SOEs) design for CPV systems, we designed three types of CPV modules, classified as non-SOEs type, reflective mirror type, and CPC lens type. We measured the I-V and P-V characteristics of the prototype CPV modules with the angle of inclination varying from 0° to 12° and with a 500-magnification Fresnel lens. The experimental results assumed misalignment of the solar position tracker or module design of pinpoint accuracy. As a result, at the 0° tilt angle, the CPC lens produced lower power due to the quartz transmittance ratio compared to that by other SOEs. However, for tilt angles greater than 3°, the CPC lens type module achieved high efficiency and stability. This study is expected to help design high-performance CPV systems.