• 대한의용생체공학회:의공학회지
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• 제34권2호
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• pp.73-79
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• 2013

Purpose: The purposes of this study were to measure the dose distribution of Photodynamic therapy(PDT) laser with 635 nm wavelength using GafChromic film. Method & Result: We made each output 300 J by changing mW and sec using the laser beam radiation mode such as C.W(Continuous Wave) mode, Pulse mode and Burst Pulse mode and measured the does at 0 mm and 5 mm of distance from optic fiber catheter end to the film, and at 5 mm distance by changing the angle of the end of the optic fiber catheter as $0^{\circ}$ and $0.5^{\circ}$. The radiated film was scanned and OD(Optical Density) was compared. And two-dimensional isodose curves were obtained and the consistency of shapes was compared. It was confirmed that there was consistency between optic density and the dose radiated on the film when we radiated GafChromic film by changing distance and angle of 300 J output in each radiation mode coordinating mW and sec. Conclusion: In this study, we could identify the stability according to changes in laser beam modes, changes in output according to distance, changes in uniformity according to angle, and beam profiles using GafChromic film, and we could also get two-dimensional isodose curve. It was found that small change in the distance and angle that is made when optic fiber catheter was contacted on the treatment area did not make big effects on the output of beam and the uniformity of dose, and it was also found that GafChromic film could be utilized for the purpose of QA of PDT laser beam.

• 설비공학논문집
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• 제7권4호
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• pp.556-565
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• 1995

The physical model of interest is based upon the concentric cylinder, where the outside cylinder is filled with optically thick and high temperature phase change material(PCM). The fluid is flowing through the inside cylinder to transfer the appropriate energy. The fluid is flowing through the inside cylinder to transfer the appropriate energy. The governing equations for the phase change material including internal thermal radiation and for the turbulent transfer fluid have been employed and numerically solved. The optically thick phase change justifies the P-l spherical harmonics approximation, which is believed to be appropriate choice particularly for the much coupled problem like in this study. The solid/liquid interface, temperature distribution within the PCM and the heat flux from the PCM to the transfer fluid have been obtained and compared with those of laminar transfer fluid. The numerical results show that the turbulent transfer fluid accelerates the solid/liquid interface and results in the increase of heat transfer rate from the PCM. The internal thermal radiation within the PCM, however, does not always playa role to increase the heat transfer rate throughout the inside cylinder. It is believed that the combined heat flux has been picked up more in the inflowing area than in the pure conductive phase change material.

• 한국광학회지
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• 제21권4호
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• pp.133-138
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• 2010

모든 복사온도계는 복사원 크기효과(Size-of-Source Effect, SSE)와 자기복사효과를 가지고 있다. 복사원의 직경에 따른 복사온도계의 검출기 신호세기로 정의된 SSE의 주원인은 회절이기 때문에 파장에 크게 좌우된다. 본 논문에서는 중저온영역에서 복사온도의 전달표준기로 많이 사용되고 있는 TRT2(Transfer Radiation Thermometer 2, HEITRONICS)의 SSE와 자기복사 특성을 측정하였다. 측정한 TRT2의 SSE 값을 사용하여 계산한 결과 흑체의 온도가 $300^{\circ}C$ 일 때, 개구 직경이 60 mm인 흑체와 10 mm인 흑체의 복사온도 차이가 저온모드($8-14\;{\mu}m$)에서 $3.5^{\circ}C$, 중온모드($3.9\;{\mu}m$)에서 $0.5^{\circ}C$인 것을 알 수 있었다. 또한, 복사온도계 몸체 온도가 $2.6^{\circ}C$ 변화했을 때 자기복사효과 때문에 흑체의 복사온도는 110 mK 다르게 측정되었다.

• 한국정보통신학회:학술대회논문집
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• 한국정보통신학회 2013년도 춘계학술대회
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• pp.732-735
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• 2013

본 논문에서는 광섬유 브래그 격자 센서를 이용하여 4종류의 단일모드 광섬유에 대한 감마선 조사에 따른 전송손실을 측정하였다. 시험에 사용된 방사선원은 $Co^{60}$ 감마선원으로, 총 2시간동안 0.6 kGy/hr, 1.2 kGy/hr, 2.4 kGy/hr의 선량률로 감마선을 조사하였다. 실험을 통하여 광섬유 종류에 따른 선량률 효과를 확인하였고, 방사선 유입손실 변화를 통한 방사선 민감도를 평가하였다.

• 한국방사선학회논문지
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• 제12권7호
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• pp.845-852
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• 2018

본 연구는 심장 혈관 조영술의 투시 영상과 씨네 영상을 획득하는 데 있어서 초당 프레임 횟수를 변화함에 따라 흡수선량과 획득 영상의 화질의 추이를 살펴보는 것을 목적으로 한다. 또, FOV 확대와 Live Zoom이라는 두 가지 확대 모드에 따른 변화도 고찰 대상으로 한다. 인체모형 팬텀을 심장 혈관 조영장치 위에서 초당 프레임 횟수를 7.5, 15, 30 f/s로 설정하고 두 가지 확대 모드에 대하여 각각 5회씩 촬영하였다. 선량의 척도로서는 흡수선량과 에어 커머가 사용되었고, 화질 평가의 척도로는 잡음의 세기로서의 표준 편차(SD), 신호 대 잡음비(SNR)와 대조도 대 잡음비(CNR) 등을 활용하였다. 초당 프레임 횟수가 30부터 15, 7.5 f/s로 감소되었을 때, DAP와 에어 커머는 동일한 비율로 감소하였으나, 화질의 척도인 SD, SNR과 CNR은 거의 변화가 없었다. 확대 모드에의 의존도에 관해서는, Live Zoom이 FOV 확대와 비교하였을 때, DAP, 에어 커머와 SD에 대해서는 통계적 의미 있는 차이를 보이지 않았으나, SNR과 CNR에 있어서는 통계적 유의미한 개선을 보였다. 이러한 실험 결과에 의하여, 초당 프레임 횟수는 화질의 열화 없이 되도록 낮게 설정하는 것이 가능하며, 확대 모드도 추가적인 선량 없이 실시간 확대가 가능한 Live Zoom 모드를 적극적으로 활용 가능하며 이는 화질의 여러 척도의 저하를 가져오지 않음을 알 수 있었다.

• 한국의학물리학회지:의학물리
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• 제24권4호
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• pp.220-229
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• 2013

Respiratory-induced dynamic tumors render free-breathing cone-beam computed tomography (FBCBCT) images with motion artifacts complicating the task of quantifying the internal target volume (ITV). The purpose of this paper is to study the visibility of the revealed ITV when the imaging dose parameters, such as the kVp and mAs, are varied. The $Trilogy^{TM}$ linear accelerator with an On-Board Imaging ($OBI^{TM}$) system was used to acquire low-imaging-dose-mode (LIDM: 110 kVp, 20 mA, 20 ms/frame) and high-imaging-dose-mode (HIDM: 125 kVp, 80 mA, 25 ms/frame) FBCBCT images of a 3-cm diameter sphere (density=0.855 $g/cm^3$) moving in accordance to various sinusoidal breathing patterns, each with an unique inhalation-to-exhalation (I/E) ratio, amplitude, and period. In terms of image ITV contrast, there was a small overall average change of the ITV contrast when going from HIDM to LIDM of $6.5{\pm}5.1%$ for all breathing patterns. As for the ITV visible volume measurements, there was an insignificant difference between the ITV of both the LIDM- and HIDM-FBCBCT images with an average difference of $0.5{\pm}0.5%$, for all cases, despite the large difference in the imaging dose (approximately five-fold difference of ~0.8 and 4 cGy/scan). That indicates that the ITV visibility is not very sensitive to changes in imaging dose. However, both of the FBCBCT consistently underestimated the true ITV dimensions by up to 34.8% irrespective of the imaging dose mode due to significant motion artifacts, and thus, this imaging technique is not adequate to accurately visualize the ITV for image guidance. Due to the insignificant impact of imaging dose on ITV visibility, a plausible, alternative strategy would be to acquire more X-ray projections at the LIDM setting to allow 4DCBCT imaging to better define the ITV, and at the same time, maintain a reasonable imaging dose, i.e., comparable to a single HIDM-FBCBCT scan.

• 한국의학물리학회지:의학물리
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• 제27권4호
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• pp.196-202
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• 2016

We aim to develop the breast bolus by using a 3D printer to minimize the air-gap, and compare it to commercial bolus used for patients undergoing reconstruction in breast cancer. The bolus-shaped region of interests (ROIs) were contoured at the surface of the intensity-modulated radiation therapy (IMRT) thorax phantom with 5 mm thickness, after which the digital imaging and communications in mdicine (DICOM)-RT structure file was acquired. The intensity-modulated radiation therapy (Tomo-IMRT) and direct mode (Tomo-Direct) using the Tomotherapy were established. The 13 point doses were measured by optically stimulated luminescence (OSLD) dosimetry. The measurement data was analyzed to quantitatively evaluate the applicability of 3D bolus. The percentage change of mean measured dose between the commercial bolus and 3D-bolus was 2.3% and 0.7% for the Tomo-direct and Tomo-IMRT, respectively. For air-gap, range of the commercial bolus was from 0.8 cm to 1.5 cm at the periphery of the right breast. In contrast, the 3D-bolus have occurred the air-gap (i.e., 0 cm). The 3D-bolus for radiation therapy reduces the air-gap on irregular body surface that believed to help in accurate and precise radiation therapy due to better property of adhesion.

• Journal of Radiation Protection and Research
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• 제49권2호
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• pp.68-77
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• 2024

Background: Cone beam computed tomography (CBCT) is essential for correcting and verifying patient position before radiation therapy. However, it poses additional radiation exposure during CBCT scans. Therefore, this study aimed to evaluate radiological safety for the human body through dose assessment for CBCT. Materials and Methods: For CBCT dose assessment, the depth dose was evaluated using a cheese phantom, and the dose in the orbital area was evaluated using a human body phantom self-fabricated with a three-dimensional printer. Results and Discussion: The evaluation of radiation doses revealed maximum doses of 14.14 mGy and minimum doses of 6.12 mGy for pelvic imaging conditions. For chest imaging conditions, the maximum doses were 4.82 mGy, and the minimum doses were 2.35 mGy. Head imaging conditions showed maximum doses of 1.46 mGy and minimum doses of 0.39 mGy. The eyeball doses using a human body phantom model averaged at 2.11 mGy on the left and 2.19 mGy on the right. The depth dose ranged between 0.39 mGy and 14.14 mGy, depending on the change in depth for each imaging mode, and the average dose in the orbit area using a human body phantom was 2.15 mGy. Conclusion: Based on the experimental results, CBCT did not significantly affect the radiation dose. However, it is important to maintain a minimal radiation dose to optimize radiation protection following the as low as reasonable achievable principle.

• 한국정보통신학회논문지
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• 제19권2호
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• pp.486-492
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• 2015

방사선 영상장치는 방사능 누출사고의 조기처리 및 확산 피해 최소화에 필수적인 장비이며, 가까운 미래에 빅마켓으로 성장될 원전폐로 분야에서도 중요한 역할을 담당할 것으로 예상된다. 현재까지 개발된 방사선 영상장치는 방사선 오염원의 위치를 방향 정보만으로 탐지하여 가시화하고 있고 방사선원의 거리 측정은 불가능한 실정이다. 본 논문에서는 스테레오 카메라 원리를 적용하여 방사선원의 3차원 위치정보를 추출할 수 있는 새로운 기법의 방사선 3차원 영상장치의 구현에 대해 연구하였다. 한 대의 방사선 센서와 CCD 카메라, 그리고 팬틸의 컴팩트한 구성으로 설계된 방사선 3차원 영상장치(K3-RIS)는 위치변환 제어에 의한 스테레오 방사선 영상 취득과 연속모드 제어 및 고속 스테레오 영상정보처리 기능이 특징이다. 개발한 장치의 기능검증을 위해 감마 방사선원(Cs-137)을 대상으로 실험을 수행한 결과 선원간의 거리와 무관하게 3% 이하의 거리측정 오차를 확인하였다.

• 한국철도학회:학술대회논문집
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• 한국철도학회 2011년도 정기총회 및 추계학술대회 논문집
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• pp.685-692
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• 2011

DC/DC switching power converters produce DC output voltages from different DC input sources. The converters can be used in regenerative braking of DC motors to return energy back in the supply, resulting in energy savings for the systems containing frequent stops. The current mode DC/DC converter is composed of a PWM (pulse width modulation) controller, a MOSFET, and inductor, etc. Pulse width modulation is applied to control and regulate the total output voltage. It is shown that the variation of threshold voltage at MOSFET and the offset voltage increase caused by radiation effects make the PWM pulse unstable. In the PWM operation, the missing pulses, the changes in pulse width, and a change in the period of the output waveform are studied by simulation program with integrated circuit emphasis (SPICE) and experiments.