• 제목/요약/키워드: Pulse Energy

검색결과 1,310건 처리시간 0.025초

1채널 단일광자검출기를 이용한 낮은 광출력의 SWIR(Short Wave Infrared) 3D 라이다 시스템 개발 (Development of SWIR 3D Lidar System with Low Optical Power Using 1 Channel Single Photon Detector)

  • 권오성;이승필;신승민;박민영;반창우
    • 한국산업융합학회 논문집
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    • 제25권6_3호
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    • pp.1147-1154
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    • 2022
  • Now that the development of autonomous driving is progressing, LiDAR has become an indispensable element. However, LiDAR is a device that uses lasers, and laser side effects may occur. One of them is the much-talked-about eye-safety, and developers have been satisfying this through laser characteristics and operation methods. But eye-safety is just one of the problems lasers pose. For example, irradiating a laser with a specific energy level or higher in a dusty environment can cause deterioration of the dust particles, leading to a sudden explosion. For this reason, the dust ignition proof regulations clearly state that "a source with a pulse period of less than 5 seconds is considered a continuous light source, and the average energy does not exceed 5 mJ/mm 2 or 35 mW" [2]. Energy of output optical power is limited by the law. In this way, the manufacturer cannot define the usage environment of the LiDAR, and the development of a LiDAR that can be used in such an environment can increase the ripple effect in terms of use in application fields using the LiDAR. In this paper, we develop a LiDAR with low optical power that can be used in environments where high power lasers can cause problems, evaluate its performance. Also, we discuss and present one of the directions for the development of LiDAR with laser power limited by dust ignition proof regulations.

중수로형 핵연료 피복관의 자동초음파탐상장치 개발 (Development of the Automated Ultrasonic Flaw Detection System for HWR Nuclear Fuel Cladding Tubes)

  • 최명선;양명승;서경수
    • Nuclear Engineering and Technology
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    • 제20권3호
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    • pp.170-178
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    • 1988
  • 중수로형 핵연료의 피복재로 사용되는 Zircaloy-4관의 결함검사를 위한 자동초음파 탐상 장치가 개발되었다. 이 장치에는 중심진동수가 14 MHz이고 대역폭이 11MHz인 집속 초음파 펄스를 사용한 수침 펄스-에코우 탐상기술과 특별히 고안된 시험수조 이송식 초음파주사 기술이 적용되었다 같은 크기와 방향을 갖는 관내외면 결함들을 같은 높이의 초음파 신호로 검출하기 위한 초음파 빔의 최적입사각은 26도이었다. Zircaloy-4피복관의 최대 허용 결함인, 깊이가 관두께의 10%인 0.04 mm이고, 길이가 0.76 mm인 축방향 및 길이가 0.38 mm인 원주방향 V형 인공결함들이 관내외면에 개재된 표준시험관을 사용하여 이 장치의 성능시험을 수행하였다. 그 결과 인공 표준시험관내의 모든 결함들을 매우 우수한 재현성을 갖고 분당 약 1m의 속도로 검출할 수 있었으며 이때의 신호 대 잡음 비는 축방향 결함에 대해서는 20 dB, 원주방향 결함에 대해서는 12 dB 이상이었다.

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가상 Frisch-그리드를 이용한 CdZnTe 감마선 소자 제작 (Fabrication of Virtual Frisch-Grid CdZnTe ${\gamma}$-Ray Detector)

  • 박찬선;김필수;조평곤;김정민;최종학;김기현
    • 대한방사선기술학회지:방사선기술과학
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    • 제37권4호
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    • pp.253-259
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    • 2014
  • Traveling heater method(THM) 방법을 이용하여 성장시킨 CdZnTe(CZT) 단결정 방사선 소자에 대한 고에너지(high energy) 감마선 에너지 분해능(energy resolution)을 평가하고자 $6{\times}6{\times}12mm^3$ 크기의 CZT 소자를 제작하였다. 두꺼운 방사선 소자의 경우, 전자에 비해 상대적으로 이동속도가 느린 정공(hole)으로 인해 발생하는 hole-tailing 효과가 심화되어 고에너지 영역의 에너지 분해능이 저하되는 현상이 발생한다. 전자(electron)와 정공(hole)의 두 개의 전하 운반자(charge carrier) 중에서 하나의 전하 운반자를 선택적으로 수집하여 에너지 분해능을 높이는 것이 가능하다. 가상 Frisch-그리드(virtual Frisch-grid) 소자는 소자 내부의 가중 퍼텐셜(weighting potential)을 조절하여 전자에 의한 유도전류(induced current)만을 선택적으로 이용하는 방법으로써 제작 과정과 적용이 용이하다. 본 연구에서는 THM 방법으로 성장한 큰 부피의 CZT 방사선 소자의 특성과 가상 Frisch-그리드의 효용성을 평가하였다. 가상 Frisch-그리드의 적절한 위치와 너비는 Maxwell ver.14(ANSYS, 미국)를 이용하여 모의실험으로 정하였다. $^{137}Cs$ 동위원소를 이용한 펄스 높이 스펙트럼(pulse height spectrum) 측정에서 가상 Frisch-그리드를 적용했을 때 662 keV 피크에 대해 2.2%의 에너지 분해능을 확인할 수 있었다.

Nd:YAG레이저조사가 경화상아질에 미치는 영향에 관한 주사전자현미경적 연구 (A Scanning Electron Microscopic Study on the Effect of Nd:YAG Laser Irradiation on the Sclerotic Dentin)

  • 김문현;신금백
    • Journal of Oral Medicine and Pain
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    • 제24권4호
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    • pp.397-410
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    • 1999
  • In order to obtain the basic data concerning the optimal parameters in using Nd:YAG laser as a therapeutic modality to dentinal hypersensitivity, the author prepared 3 sections of sound dentin and 10 sections of sclerotic dentin with thickness of $0.5mm{\pm}0.1mm$ from human extracted teeth of anteriors and premolars, and applied the laser energy from a fiberoptic delivered, free running, pulsed Nd:YAG laser (wavelength 1064nm, pulse duration $120{\mu}sec$, fiber diameter $320{\mu}m$) to surfaces of sound and sclerotic dentin sections for 1 second with contact/unidirectional moving mode of the fiber under speed of 3mm~4mm/sec and parameters of 0.5W/10Hz, 1.0W/10Hz, 1.5W/10Hz, 2.0W/10Hz: $62J/cm^2$, $124J/cm^2$, $187J/cm^2$, $249J/cm^2$. The author comparatively evaluated the characteristics of ultrastructural changes on surfaces of sound and sclerotic dentin sections irradiated by the pulsed Nd:YAG laser using the scanning electron microscopy. A fairly ill-defined bordered surface of partially closed and melted dentinal tubules can be seen on the scanning electron microscopic feature of the sound dentin surface irradiated by the pulsed Nd:YAG laser with energy density of $62J/cm^2$. The physical modification of sound dentin surface extensively occurred depended on the increase of energy density from $62J/cm^2$ to $124J/cm^2$, $187J/cm^2$, $249J/cm^2$. While, a fairly well-defined bordered surface of partially closed and melted dentinal tubules with thickened peritubular dentin can be seen on the scanning electron microscopic feature of the sclerotic dentin surface irradiated by the pulsed Nd:YAG laser with energy density of $62J/cm^2$. The physical modification of sclerotic dentin surface of a fairly rough, shallow depression with many cracks, thickened peritubular dentin and structureless dentinal tubules extensively occurred depended on the increase of energy density from $62J/cm^2$ to $124J/cm^2$, $187J/cm^2$, $249J/cm^2$ compared to those of sound dentin surface irradiated by the pulsed Nd:YAG laser under the same parameters. Therefore, it is recommended that the pulsed Nd:YAG laser as a therapeutic modality to dentinal hypersensitivity should be applied with the less energy density than $62J/cm^2$ on the sound dentin surface, and its energy density on the partially sclerotic dentin surface should be lower than that on the sound dentin surface to preserve tooth from unnecessary excessive structural destruction.

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태양위치 추적 장치를 이용한 집광형 태양광 발전시스템 (The Concentrating Photovoltaic System using a Solar Tracker)

  • 유영태;나승권
    • 한국항행학회논문지
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    • 제21권4호
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    • pp.377-385
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    • 2017
  • 태양광 발전에 있어서 태양전지는 일사량, 온도와 부하에 의해 크게 변동하기 때문에 태양전지에 대한 특성 해석이 필요하다. 또한 태양광 발전에 있어서 가능한 많은 에너지를 얻기 위해서는 환경변화에 따른 태양의 위치추적이 필요하며 태양전지의 출력을 항상 최대로 제어할 필요가 있다. 본 논문에서는 태양광 발전의 효율을 높이기 위하여 센서와 마이크로프로세서를 이용한 태양광 위치추적 장치를 설계하여 고정방식의 태양광 발전과 위치 추적 방식의 태양광 발전에 대하여 비교해 보았으며, 태양전지에 대한 특성 해석과 수학적 모델링을 통한 시뮬레이션을 행하여 태양전지 특성 사양과 비교해 보았다. 또한 전력변환 시스템을 Boost 컨버터와 전압형 인버터로 구성하여 각각에 대하여 실험하였으며, Boost 컨버터 제어에서 최대 전력점 추적을 위해 일정전압 제어법을 사용하였으며 인버터의 제어에서는 SPWM(Sinusoidal Pulse Width Modulation) 제어법을 사용하여 실험해 보았다. 그 결과 태양전지 수학적 모델링 한 것의 시뮬레이션 결과와 태양전지 특성 사양과 비교하였을 때 5%이하의 오차를 보였으며. Boost 컨버터의 승압율은 167%로 시뮬레이션 한 것과 근사적으로 나타났고, 인버터는 시뮬레이션 한 것과 근사적 파형을 얻었으나 손실이 큰 것으로 나타났다.

맥파전달속도를 이용한 내중막 두께 추정에 관한 연구 (A Study on Estimation of Carotid Intima-Media Thickness(IMT) using Pulse Wave Velocity(PWV))

  • 송상하;장승진;김원식;이현숙;윤영로
    • 대한의용생체공학회:의공학회지
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    • 제30권5호
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    • pp.401-411
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    • 2009
  • In this paper, we correct pulse wave velocity(PWV) with heart-rate and derive regression equations to estimate intima-media thickness(IMT). Widely used methods for diagnosis of arteriosclerosis are IMT and PWV. Arterial wall stiffness determines the degree of energy absorbed by the elastic aorta and its recoil in diastole but there is not correlation between sclerosis and IMT in an existing study. In this study, we will correct PWV with heart-rate and get regression equation to estimate IMT using heart-rate correction index(HCI). We executed experiments for this study. Made up question of physical condition and measured electrocardiogram(ECG), photoplethysmogram (PPG) of finger-tip and toe-tip and ultrasound image of carotid artery. Calculated PWV and IMT using ECG, PPG and ultrasound image. We found that every p-value between PWV and IMT is not significant(<0.05). But p-value between IMT and HCI which is a corrected PWV using heart-rate is significant(>0.01). We use HCI and various measured parameter for estimating regression equation and apply backward estimation to select parameters for regression analysis. Result of backward estimation, found that only HCI is possible to derive proper regression equation of IMT. Relationship between PWV and IMT is the second order. Result of regression equation of E-H PWV is $R^2$=0.735, adj $R^2$=0.711. This is the best correlation value. We calculate error of its analysis for verification of earlobe PWV regression equation. Its result is RMSEP=0.0328, MAPE(%) = 4.7622. Like this regression analysis, we know that HCI is useful parameter and relationship between PWV, HCI and IMT. In addition, we are able to suggest possibility which is that we can get different parameter of prediction throughout just one measurement.

PLT(10) 박막의 Switching 특성에 관한 연구 (A Study on the Switching Characteristcs of PLT(10) Thin Films)

  • 강성준;장동훈;윤영섭
    • 전자공학회논문지D
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    • 제36D권11호
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    • pp.63-70
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    • 1999
  • PLT(10) 박막을 $Pt/TiO_2/SiO_2/Si$ 기판 위에 sol-gel법으로 제작하여, 상부전극의 면적과 외부인가 펄스전압 및 부하저항을 변화시켜 가며 비휘발성 메모리 소자에 응용하기 위해 필수적인 switching 특성을 조사하였다. 외부인가 펄스전압이 2V에서 5V 까지 증가함에 따라, switching time은 $0.49{\mu}s$에서 $0.12{\mu}s$로 감소하였으며, 인가된 펄스전압에 대한 switching time의 관계로부터 구한 활성화 에너지 ($E_a$)는 209 kV/cm이었다. 상부전극 면적이 $3.14{\times}10^{-4}cm^2$인 박막에서 이력곡선과 polarization switching 실험으로부터 구한 switched charge density는 5V에서 각각 $11.69{\mu}C/cm^2$$13.02{\mu}C/cm^2$으로 양쪽 값 사이의 오차는 약 10%로 비교적 잘 일치하는 경향을 나타내었다. 상부전극의 면적이 $3.14{\times}10^{-4}cm^2$에서 $5.03{\times}10^{-3}cm^2$으로 증가함에 따라, switching time이 $0.12{\mu}s$에서 $1.88{\mu}s$로 증가하였으며, 부하저항을 50${\Omega}$에서 3.3$k{\Omega}$으로 증가시킴에 따라 switching time은 $0.12{\mu}s$에서 $9.7{\mu}s$로 증가로 증가하였다. 이와 같은 switching 특성에 관한 연구를 통해 PLT(10) 박막이 비휘발성 메모리 소자에 응용될 수 있는 매우 유망한 재료임을 알 수 있다.

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1.57 BRAIN MRI검사에서의 작동제어모드를 통한 두부 SAR측정과 변화인자에 관한 고찰 (Implementation about measurement of the head SAR and variable parameter according to operation control mode in brain MR study with 1.5Tesia)

  • 이규수;심현;문지훈;오재철
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2007년도 심포지엄 논문집 정보 및 제어부문
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    • pp.58-60
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    • 2007
  • Magnetic Resonance Imaging(MRI) has become a very widely used medical procedur e. Clo.sed and open systems are typically used with static magnetic fields at or below 2 Tesla. BWhole body SAR(specific absorbsion rate) is the value of SAR averaged over the entire body of the patient over any period of 15 minutes. Head SAR is the value of SAR averaged over the head of the patient for any period of 10 minutes. SAR is a measure of the absorption of electromagnetic energy in the body' (typically in watts per kilogram (W/kg)). The normal operating mode comprises values of head SAR not higher than 3 W/kg. The second level controlled operating mode comprises values higher than 3 W/kg. Current FDA guidance limits the SAR in the whole body. including the head to a range of 1.5 to 4.0 W/kg, depending on the patient's clinical condition. SAR, limit restrictions are incorporated in all MRI systems. and domestic' s guidance limits the SAR in a part body. including the head to 3.2w/kg and less. The purpose of this study is to evaluate on change of head SAR in using MRI pulse sequence and to check if exceed 3.2(w/kg) level in domestic a part exposure through measured head SAR. 23 patient's the average head SAR of pulse sequence is that T2WI sagittal is 0.5375. T2WI axial(FSE) is 0.4817, T1WI axial(SE) is, 0.8179. FLAIR axial is 0.4580. GRE axial is 0.0077, Diffusion is 0.0824w/kg. The head SAR exposed per patient was proved 2.3845w/kg less than the international standard. Coefficient of correlation for the relations body weight and SAR or for the relations ETL(echo train length) and SAR is 1 value. Coefficient of correlation for the relations between TR(time to repeat) and SAR is -0.602 value. so SAR increased relative to weight body and ETL. But the relations between TR and SAR is negative definite.

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LiMn2O4의 Mn용출 현상 연구를 위한 전기화학적 Mn(II) 정량 분석법 (Electrochemical Quantitative Analysis of Mn(II) for the Study of Mn-Dissolution Behavior of LiMn2O4)

  • 손화영;이민영;고형신;이호춘
    • 전기화학회지
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    • 제14권3호
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    • pp.131-137
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    • 2011
  • [ $LiMn_2O_4$ ] $Mn^{2+}$이온 용출현상 연구를 위한 간단하고 신속한 전기화학적 $Mn^{2+}$이온 분석법을 정립하였다. 이 분석법은 완충용액에서 $Mn^{2+}$이온이 $Mn^{4+}(MnO_2)$로 산화되는 원리를 이용한다. 최적조건 (pH 8.9 0.04 M $NH_3-NH_4Cl$ 완충용액 및 glassy carbon 작업전극)에서, Linear sweep voltammetry(LSV) 측정에 대해 $5{\mu}M-100{\mu}M$ (0.275-5.5 ppm) $Mn^{2+}$이온 범위에서, differential pulse voltammetry (DPV) 측정에 대해 $0.2{\mu}M-10{\mu}M$ (0.011-0.55 ppm) 범위에서 선형적 응답 특성을 확인하였다. 또한, 측정용액에 리튬 이차전지용 전해액 ($LiPF_6$, EC, EMC)이 첨가할 경우, 첨가량에 비례하여 $Mn^{2+}$ 이온의 산화 전류 감소하였는데, 이러한 감소의 주요 원인은 EMC보다는 $LiPF_6$와 EC성분임을 확인하였다.

Bone Mineral Density and Affecting Factors in College Women

  • Na, Hye-Bok;Jung, Shin-Yong
    • Journal of Community Nutrition
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    • 제1권2호
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    • pp.98-107
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    • 1999
  • The purpose of this study was to investigate Bone Mineral Density(BMD) and affecting factors on BMD of college women in Seoul. The subjects were 47 healthy college women aged 18-25 years. Antrophometric and body fat measurements were performed by Bioelectrical Impedance Fatness Analyzer(Tanita TVF 202). Blood pressure and pulse frequency were measured. Dietary intakes and general living habits were examined through questionnaires and nutrient intakes were analyzed by Computer Aided Nutritional Analysis(CAN) program for professional. Serum total cholesterol, TG(triglyceride), HDL-cholesterol, total protein, albumin, GOT, calcium were measured by Spotchem(SP-4410). Serum osteocalcin and alkaline phosphatase(ALP) were measured to monitor bone formation. BMD of lumbar spine(L2-L4), right hip(neck, ward's triangle, trochanter) and right forearm were measured by Dual Energy X-ray Absorptiometry(DEXA). Muscle strength was measured by examining leg flexion strength(right and left), leg extension power(right and left), handgrip power(right and left) and back strength. All data were statistically analyzed by the SAS PC package program. BMD of college women was normal(by WHO, 1994). Their muscle strength was bad(by national fitness guidebook, 1995). Only a mall number of them exercised (32.6% of subjects). There was no significant difference among BMD, muscle strength and % body fat(p<0.05). There were significant differences between BMD and total cholesterol as well as TG and VLDL-cholesterol(p<0.05). Total cholesterol was associated with decreasing BMD of the right forearm(p<0.05). TG and VLDL-cholesterol are associated with increasing BMD of right hip ward's triangle(p<0.05). There were significant differences among BMD, ALP and serum total protein. ALP was associated with decreasing BMD of the right forearm(p<0.05). There were significant differences between BMD and Ca as well as between Na and K intakes (p<0.05). Intakes of Na and K were associated with decreasing BMD of the right forearm (UD)(p<0.05). There were significant differences between in BMD and pulse frequently and serum albumin (p<0.05). Serum albumin is associated with increasing BMD of L3-L4(p<0.05), right hip neck(p<0.05). %Body fat, TG, VLDL-C, Ca intake, pulse frequency and serum albumin were associated with increasing BMD(p<0.05). Intakes of Na and K, ALP, total cholesterol, total cholesterol, total protein and height are associated with decreasing BMD(p<0.05). Overall results indicate that Ca intake but to be moderate in protein and Na intakes in order to increase BMD. Body exercise was recommended to increase BMD as well.

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