• 제목/요약/키워드: quasi-CW

검색결과 11건 처리시간 0.038초

고출력 CW Nd:YAG 레이저를 이용한 CSP 1N 박판 절단공정의 열전달 특성 분석 (A Study on Heat Transfer Characteristics of Laser Cutting for the CSP 1N Sheet Using High-power CW Nd:YAG Laser)

  • 안동규;김민수
    • 한국기계가공학회지
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    • 제5권1호
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    • pp.51-58
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    • 2006
  • The objective of this research work is to investigate into heat transfer characteristics of the laser cutting of CSP 1N sheet using high power CW Nd:YAG laser. In order to investigate the heat transfer characteristics, three dimensional quasi stationary and steady-state heat transfer analysis has been carried out. The laser heat source is assumed as a volumetric heat source with a gaussian heat distribution in a plane. Through the comparison of the results of analyses with those of experiments, the proper finite element model has been obtained. In addition, characteristics of the three-dimensional heat transfer and temperature distribution have been estimated by the finite element model. Finally, the minimum temperature at the center for cutting of the material has been estimated.

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비파괴검사를 위한 연속형 테라헤르츠 파 기반의 영상화 기술 (Imaging Technique Based on Continuous Terahertz Waves for Nondestructive Inspection)

  • 오경환;김학성
    • 센서학회지
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    • 제27권5호
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    • pp.328-334
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    • 2018
  • The paper reviews an improved continuous-wave (CW) terahertz (THz) imaging system developed for nondestructive inspection, such as CW-THz quasi-time-domain spectroscopy (QTDS) and interferometry. First, a comparison between CW and pulsed THz imaging systems is reported. The CW-THz imaging system is a simple, fast, compact, and relatively low-cost system. However, it only provides intensity data, without depth and frequency- or time-domain information. The pulsed THz imaging system yields a broader range of information, but it is expensive because of the femtosecond laser. Recently, to overcome the drawbacks of CW-THz imaging systems, many studies have been conducted, including a study on the QTDS system. In this system, an optical delay line is added to the optical arm leading to the detector. Another system studied is a CW-THz interferometric imaging system, which combines the CW-THz imaging system and far-infrared interferometer system. These systems commonly obtain depth information despite the CW-THz system. Reportedly, these systems can be successfully applied to fields where pulsed THz is used. Lastly, the applicability of these systems for nondestructive inspection was confirmed.

고출력 CW Nd:YAG 레이저를 이용한 CSP 1N 냉연강판 절단 공정의 3 차원 열전달 해석 (Three-dimensional heat transfer analysis of laser cutting process for CSP 1N sheet using high power CW Nd:YAG laser)

  • 김민수;안동규;이상훈;유영태;박형준;신호준
    • 한국정밀공학회:학술대회논문집
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    • 한국정밀공학회 2005년도 추계학술대회 논문집
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    • pp.162-165
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    • 2005
  • The objective of this research work is to investigate into the three-dimensional temperature distribution using quasi steady-state heat transfer analysis fur the case of the laser cutting of CSP 1N sheet using high power CW Nd:YAG laser. The laser heat source is assumed as a volumetric heat source with a gaussian heat distribution in a plane. Through the comparison of the results of analyses with those of the experiments, the optimal finite element model is obtained. Finally, characteristics of the three-dimensional heat transfer and temperature distribution have been estimated by the optimal finite element model.

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Effects of Low Incident Energy Levels of Infrared Laser Irradiation on the Proliferation of Candida Albicans Part I : A Long Term Study according to Pulse Type

  • Sam-Kun Kim;Phil-Yeon Lee;Ki-Suk Kim
    • Journal of Oral Medicine and Pain
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    • 제19권1호
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    • pp.9-15
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    • 1994
  • This experiment was performed to confirm the hypothesis that LLLT had biostimulation effect for all kinds of cells and there would be differences in the growth of cells among different types of pulsed laser. 360 samples were used in this study. The samples were randomly divided in 6 groups according to the pulse type : quasi continuous type (CW), pulse 1(P1), pulse 7(P7), pulse 9(P9), pulse 15(P15) and shame-irradiated control(Co) groups. Energy fluences of all experimental groups, P1, P7, P9, P15 and CW were 2.12, 2.12, 6.37, 57.32 and 31.85 mj/cm2 respectively. All samples were irradiated for every 1 minute at 0, 12, 24, 36, 48 and 60 hours. Ten samples of each group were sacrificed at 0 and every 12 hours and then the optical density of all samples was measured with the spectrophotometer. As a result, some types of pulses showed significant differences among groups. The increase of cells were markedly stimulated with laser irradiation in P7 and P9 groups, while inhibited in CW, P1, and P15 groups compared with control group. It is therefore, suggested that specific laser pulse should be recommanded to have the biostimulation effects on the specific tissue or cells, although the biostimulation effect is does dependant.

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Power Characteristics of cw Second-harmonic Generation in Periodically Poled LiNbO3

  • Kang, Bong-Hoon;Joo, Gi-Tae;Rhee, Bum-Ku
    • 한국세라믹학회지
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    • 제47권5호
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    • pp.430-432
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    • 2010
  • We verified through a noncritical phase-matched second-harmonic generation experiment that the periodically-poled $LiNbO_3$ (PPLN) had a large effective nonlinear optical coefficient, demonstrating that the QPM grating was uniform throughout the entire length of PPLN. The quasi-phase matching temperature was $193.4^{\circ}C$. The maximum SHG output power at the fundamental power of 2.0 W was found to be 18.0 mW; generated second-harmonic beam was found to have no photorefractive effect.

첨두 출력 1.5 kW급 준연속 이터븀 첨가 광섬유 레이저 (Quasi-continuous-wave Yb-doped Fiber Lasers with 1.5 kW Peak Power)

  • 전민지;정예지;김지원;정훈
    • 한국광학회지
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    • 제27권3호
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    • pp.95-100
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    • 2016
  • 본 논문에서는 이터븀(Yb)이 첨가된 이중 클래딩 광섬유를 이용한 고출력 고품질 준연속 레이저 시스템에 대한 연구 개발과 레이저 특성에 대해 보고한다. 이론적 수치 모사를 통해 최적화된 준연속 레이저 발진 조건을 찾았고, 그것을 바탕으로 공진기 구조와 MOPA (Master-Oscillator Power-Amplifier) 구조를 가진 광섬유 레이저 시스템을 각각 구축하였다. 두 레이저 시스템 모두 10 Hz 반복률, 10 ms로 작동시킬 때 최고 평균 출력 >150 W, 첨두 출력 >1.5 kW 이상의 준연속 레이저 빔을 발생시키는데 성공하였고, 레이저 발진 특성 및 빔 특성을 각각 비교하였다. 그리고 향후 더 높은 출력을 얻기 위한 방법과 전망에 대해 논의할 것이다.

20W급 AlGaAs 레이저 다이오드 어레이의 제작 (Fabrication of a AlGaAs high power (~20W) laser diode array)

  • 박병훈;손낙진;배정훈;권오대
    • 전자공학회논문지D
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    • 제34D권11호
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    • pp.20-24
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    • 1997
  • We have successfully fabricated high power (~20W) laser diode array, which are useful for pumping Nd:YAG lasers. The laser diode aray has 20 100.mu.m-wide cahnnels of which space was adjusted to 350.mu.m to improve thermal characteristics. And channel width is 100.mu.m. For an uncoated LD array, the output power of 15.66W has been obtained at 41A under quasi-CW operation, which results in about 0.42W/A slope efficiency. After aR(5%) and HR (95%) coatings on both facets, the output power was improved up to 21.18W at 40A under the same operation as above and the slope efficiency was 0.795W/A. On the other hand, by using a near field measurement system consisting of objective lens, eyepiece, CCD camera and image processing board, the typical near field patten of 1*20 LD array was observed.

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자동차용 무침입형 극저탄소강의 파이버 레이저 용접에 대한 연구 (A Study on the Fiber Laser welding of Ultra-Low Carbon Interstitial Free Steel for Automotive)

  • 오용석;신호준;양윤석;황찬연;유영태
    • 한국생산제조학회지
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    • 제20권3호
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    • pp.342-349
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    • 2011
  • The purpose of this paper is to describe experimental results about the butt welding and bead on plate welding of the high power Continuous Wave (CW) Fiber laser for Ultra-low carbon Interstitial Free(IF) steel plate for gear part of car. After being welded of the gear parts by the fiber laser and electron beam Microstructures of melting zone had been mixed acicular, granular bainitic, quasi-polygonal and widmanstatten ferrite because of a radical thermal diffusion after welding, difference of critical volume and grain size. As a result of experiment, when gear parts were welded by the fiber laser and electron beam, the fiber laser welding has been stable properties without internal defects more than the electron beam welding. Therefore it has the very advantages of welding high quality and productivity more than conventional melting method. The optimal welding processing parameters for gear parts were as follows : the laser power and welding speed were 3kWatt, 30mm/sec respectively. At this time heat input was $21.2{\times}10^3J/cm^2$.