• 제목/요약/키워드: beam profile

검색결과 469건 처리시간 0.028초

금속 표면경화용 고출력 다이오드 레이저 개발 프로세스 (Development Process for High Power Diode Laser for Metal Surface Hardening)

  • 장동환
    • 한국기계가공학회지
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    • 제21권2호
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    • pp.11-22
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    • 2022
  • This paper presents the development process for a high-power diode laser for metal surface hardening. To combine the emissions from several laser bars, it is necessary to collimate the emitted light using an optical lens. Thus, to achieve a suitable power density and uniform beam profile, several optical layouts were proposed. To estimate the laser beam for a flat-top distribution, a numerical analysis was performed using the ZEMAX software, and the results were compared with the experimental results. With a focal lens assembled in a serial diode stack source, the design can utilize the advantage of compacting the overall beam size. Experimental results for a robotic system demonstrated the processing ability of this diode laser module in industrial laser hardening.

전극 구조 변화에 따른 Cold Hollow Cathode Ion Source의 특성 변화 (Characterization of Cold Hollow Cathode Ion Source by Modification of Electrode Structure)

  • 석진우;;한성;백영환;고석근;윤기현
    • 한국세라믹학회지
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    • 제40권10호
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    • pp.967-972
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    • 2003
  • 직경 5 cm cold hollow cathode 이온원을 박막의 이온보조증착법 또는 이온보조반응법에 사용하기에 적합한 이온빔으로 넓은 면적을 균일하게 조사할 수 있는 이온원을 설계, 제작하기 위한 방안으로 연구하게 되었다. 이온원은 글로우 방전을 위한 음극과 이온화 효율의 증가를 위한 자석, 플라즈마 챔버, 그리드 전극으로 이루어진 이온광학시스템, 직류전원공급장치로 이루어진다. 전자인출전극의 구조 및 형태로 구분하여 한개의 노즐로 이루어진 (I) 형태와 복수개의 노즐로 변형된 (II) 형태로 제작하였다. 서로 다른 구조의 전자인출전극 (I)형태와 (II) 형태를 부착한 이온원에 beam profile을 측정한 결과 (I) 형태의 전자인출전극을 부착한 경우에는 이온원의 중심에서 140 $\mu\textrm{A}$/$\textrm{cm}^2$으로 측정되어 졌으며, 외곽으로 멀어질수록 급격히 전류밀도가 감소하여 균일한 영역(최대값의 90%)은 직경 5 cm로 측정되어졌다. (II) 형태로 변형되어진 이온원의 경우 중심에서 65 $\mu\textrm{A}$/$\textrm{cm}^2$으로 (I) 형태와 비교하여 상대적으로 낮은 전류밀도가 측정되었지만 외각으로 멀어졌을 경우에도 전류밀도는 완만하게 감소하여 균일한 영역은 직경 20 cm로 측정되었으며, 본 연구목적에 부합되는 특성이 측정되었다. 이온빔 균일도가 증가한 (II) 형태의 전자인출전극을 부착한 이온원으로 주입하는 아르곤 가스량의 변화, 이온광학시스템의 플라즈마 그리드 전극과 가속 그리드 전극 간격의 조절, 이온빔 에너지 변화에 따른 beam profile 및 특성을 괸찰하였다.

An AFM-based Edge Profile Measuring Instrument for Diamond Cutting Tools

  • Asai, Takemi;Motoki, Takenori;Gao, Wei;Ju, Bing-Feng;Kiyono, Satoshi
    • International Journal of Precision Engineering and Manufacturing
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    • 제8권2호
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    • pp.54-58
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    • 2007
  • This paper describes an atomic force microscope (AFM)-based instrument for measuring the nanoscale cutting edge profiles of diamond cutting tools. The instrument consists of a combined AFM unit and an optical sensor to align the AFM tip with the top of the diamond cutting tool edge over a submicron range. In the optical sensor, a aser beam is emitted from a laser diode along the Y-axis and focused to a small beam spot with a diameter of approximately $10{\mu}m$ at the beam waist, which is then received by a photodiode. The top of the tool edge is first brought into the center of the beam waist by adjusting it in the X-Z-plane while monitoring the variation in the photodiode output. The cutting tool is then withdrawn and its top edge position at the beam center is recorded. The AFM tip can also be positioned at the beam center in a similar manner to align it with the top of the cutting edge. To reduce electronic noise interference on the photodiode output and thereby enhance the alignment accuracy, a technique is applied that can modulate the photodiode output to an AC signal by driving the laser diode with a sinusoidal current. Alignment experiments and edge profile measurements of a diamond cutting tool were carried out to verify the performance of the proposed system.

Dosimetric Impact of Ti Mesh on Proton Beam Therapy

  • Cho, Shinhaeng;Goh, Youngmoon;Kim, Chankyu;Kim, Haksoo;Jeong, Jong Hwi;Lim, Young Kyung;Lee, Se Byeong;Shin, Dongho
    • 한국의학물리학회지:의학물리
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    • 제28권4호
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    • pp.144-148
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    • 2017
  • When a high density metallic implant is placed in the path of the proton beam, spatial heterogeneity can be caused due to artifacts in three dimensional (3D) computed tomography (CT) scans. These artifacts result in range uncertainty in dose calculation in treatment planning system (TPS). And this uncertainty may cause significant underdosing to the target volume or overdosing to normal tissue beyond the target. In clinical cases, metal implants must be placed in the beam path in order to preserve organ at risk (OARs) and increase target coverage for tumors. So we should introduce Ti-mesh. In this paper, we measured the lateral dose profile for proton beam using an EBT3 film to confirm dosimetric impact of Ti-mesh when the Ti-mesh plate was placed in the proton beam pathway. The effect of Ti-mesh on the proton beam was investigated by comparing the lateral dose profile calculated from TPS with the film-measured value under the same conditions.

Optimum design of steel floor system: effect of floor division number, deck thickness and castellated beams

  • Kaveh, A.;Ghafari, M.H.
    • Structural Engineering and Mechanics
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    • 제59권5호
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    • pp.933-950
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    • 2016
  • Decks, interior beams, edge beams and girders are the parts of a steel floor system. If the deck is optimized without considering beam optimization, finding best result is simple. However, a deck with higher cost may increase the composite action of the beams and decrease the beam cost reducing the total cost. Also different number of floor divisions can improve the total floor cost. Increasing beam capacity by using castellated beams is other efficient method to save the costs. In this study, floor optimization is performed and these three issues are discussed. Floor division number and deck sections are some of the variables. Also for each beam, profile section of the beam, beam cutting depth, cutting angle, spacing between holes and number of filled holes at the ends of castellated beams are other variables. Constraints include the application of stress, stability, deflection and vibration limitations according to the load and resistance factor (LRFD) design. Objective function is the total cost of the floor consisting of the steel profile cost, cutting and welding cost, concrete cost, steel deck cost, shear stud cost and construction costs. Optimization is performed by enhanced colliding body optimization (ECBO), Results show that using castellated beams, selecting a deck with higher price and considering different number of floor divisions can decrease the total cost of the floor.

6MV Photon Beam Commissioning in Varian 2300C/D with BEAM/EGS4 Monte Carlo Code

  • Kim, Sangroh;Jason W. Sohn;Cho, Byung-Chul;Suh, Tae-Suk;Choe, Bo-Yong;Lee, Hyoung-Koo
    • 한국의학물리학회:학술대회논문집
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    • 한국의학물리학회 2002년도 Proceedings
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    • pp.113-115
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    • 2002
  • The Monte Carlo simulation method is a numerical solution to a problem that models objects interacting with other objects or their environment based upon simple object-object or object-environment relationships. In spite of its great accuracy, It was turned away because of long calculation time to simulate a model. But, it is used to simulate a linear accelerator frequently with the advance of computer technology. To simulate linear accelerator in Monte Carlo simulations, there are many parameters needed to input to Monte Carlo code. These data can be supported by a linear accelerator manufacturer. Although the model of a linear accelerator is the same, a different characteristic property can be found. Thus, we performed a commissioning process of 6MV photon beam in Varian 2300C/D model with BEAM/EGS4 Monte Carlo code. The head geometry data were put into BEAM/EGS4 data. The mean energy and energy spread of the electron beam incident on the target were varied to match Monte Carlo simulations to measurements. TLDs (thermoluminescent dosimeter) and radiochromic films were employed to measure the absorbed dose in a water phantom. Beam profile was obtained in 40cm${\times}$40cm field size and Depth dose was in 10cm${\times}$10cm. At first, we compared the depth dose between measurements and Monte Carlo simulations varying the mean energy of an incident electron beam. Then, we compared the beam profile with adjusting the beam radius of the incident electron beam in Monte Carlo simulation. The results were found that the optimal mean energy was 6MV and beam radius of 0.1mm was well matched to measurements.

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T형 모듈단면 합성 프로파일보의 거동에 관한 실험적 연구 (An Experimental Study on the Behavior of T-type Modular Composite profiled Beams)

  • 안형준;이성원;류수현
    • 한국강구조학회 논문집
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    • 제20권4호
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    • pp.539-548
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    • 2008
  • 본 연구는 기존에 발표한 T형 모듈단면 프로파일보의 적용가능성을 확인하기 위해 실험체를 제작하고 전단보강 유무에 따른 휨 및 전단거동을 측정하여 그 결과를 소성이론식과 비교 분석하였다. 모듈단면 프로파일보는 프로파일이 거푸집기능에 추가하여 휨 및 전단저항성능에 기여하고 모듈개념을 통해 성형성능을 향상시킨다. 실험결과 전단보강을 실시한 TS계열 실험체가 전단보강이 없는 T계열 실험체에 비해 우수한 휨저항 능력을 나타내 사용된 전단보강재는 적절하게 전단력을 분담하고 있는 것으로 파악되었으나 T1-1실험체를 제외한 모든 실험체에서 볼트의 전단파괴에 의한 모듈간 슬립현상이 발생되어 휨저항 성능이 충분히 발휘되지 못한 것으로 판단된다. 추후 전단연결재를 변수로 한 T형 모듈단면 프로파일보에 관한 연구를 통해 적절한 모듈간 접합방법이 연구 되어져야 할 것으로 판단된다.

Structural performance of GFRP-concrete composite beams

  • Yang, Yong;Xue, Yicong;Zhang, Tao;Tian, Jing
    • Structural Engineering and Mechanics
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    • 제68권4호
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    • pp.485-495
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    • 2018
  • This paper presents the results of an experimental study on the structural performance of an innovative GFRP-concrete composite beam construction, which is reinforced with longitudinal GFRP pultruded box-profile and transverse steel stirrups. GFRP perfobond (PBL) shear connectors are employed to enhance the bonding performance between the GFRP profile and the concrete portion. To investigate the shear and flexural performance of this composite system, eight specimens were designed and tested under three-point and four-point bending. The main variables were the height of the composite beam and the shear span-to-depth ratio. The test results indicated that bonding cracks did not occur at the interface between the GFRP profile and the concrete until the final stage of the test. This shows that the specimens performed well as composite beams during the test and that the GFRP PBL connectors were reliable. Based on the test results, two calculation methods were used to determine the flexural and shear capacity of the composite beams. A comparative study of the test and theoretical results suggests that the proposed methods can reasonably predict both the flexural and shear capacities of the specimens, whereas the provisions of ACI 440 are relatively conservative on both counts.

응력측정 구조를 이용한 $p^+$ 박막의 응력분포 추정 (Estimation of the Stress Profile of $p^+$ Silicon Films Using Stress Measurement Structures)

  • 양의혁;양상식;박응준;유승현
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1994년도 추계학술대회 논문집 학회본부
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    • pp.413-415
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    • 1994
  • In this paper, a new technique for quantitative estimation of the stress profile along the depth of $p^+$ silicon films is presented. The $p^+$ silicon cantilevers with various beam thickness and a rotating beam supported by two cantilevers are used for estimating the stress profile of the films. The average of the residual stress distribution is estimated to be 50MPa. Most of $p^+$ silicon films are subjected to the tensile stress, except the region near the frontside.

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흡수 선량 분포의 수송방정식을 이용한 10 MV X-선의 모델 (High Energy Photon Beam Modeling Using Transport Theory for Calculation of Absorbed Dose Distribution)

  • 최동락;전하정;이명자
    • Radiation Oncology Journal
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    • 제10권1호
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    • pp.115-120
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    • 1992
  • 물팬톰내에 조사된 10 MV X-선의 심부율을 입자의 수송이론을 근거로 한 1차원적인 모델을 이용하여 계산하였다. 계산된 이론식의 매개상수는 9개로 줄일 수 있었으며 실측치를 이용하여 비선형 회귀분석 방법으로 얻을 수 있다. 조사면과 선원간의 거리 및 깊이에따른 3차원적인 흡수선량분포의 계산식은 고에너지 광자선이 조사된 물팬톰내에서의 Beam Profile에 대한 시도함수를 이용하여 수송이론에의한 심부율계산을 3차원적으로 확장하였으며 흡수 선량 분포는 3차원적 위치의 함수로 널리 계산할 수 있다. 이 모델을 사용하여 계산된 이론값은 실험값과 $\pm12\%$ 이내의 만족할만큼 잘 일치하였다.

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