• Title/Summary/Keyword: 조사면 크기

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The Physical Penumbra of the 6MV X-ray (6MV 방사선의 물리학적 Penumbra)

  • Cho Moon-June;Kang Wee-Saing
    • Radiation Oncology Journal
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    • v.9 no.2
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    • pp.333-336
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    • 1991
  • High energy Photon beam has a sharp beam margin due to a less side scatter and the other things. But there still remains a penumbra where the dose changes rapidly in the region near the edge of a radiation beam, although it is short in width. It is suggested that the width of the penumbra depends on the source size, distance from source to diaphragm, source to skin distance, and depth in tissue. However, it is also supposed that the other factors influence the penumbra width. In this paper, we investigate changes of the physical penumbra widths according to various field sizes and depths, by using the three dimensional dosimetry system. As a result, we found that as field size and depth increase, the physical penumbra width also increases.

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Evaluation of Dosimetric Characteristics of Small Field in Cone Versus Square Fields Based on Linear Accelerators(LINAC) for Stereotactic Radiosugery(SRS) (선형가속기를 기반으로 한 뇌정위 방사선 수술 시 전용 콘과 정방형 소조사면의 선량 특성에 관한 고찰)

  • Yoon, Joon;Lee, Gui-Won;Park, Byung-Moon
    • Journal of radiological science and technology
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    • v.33 no.1
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    • pp.61-66
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    • 2010
  • In this paper we evaluated small field dose characteristics of exclusive cone fields versus square fields for stereotactic radiosugery (SRS) which is based on linear accelerators (LINAC). For this test, we used a small beam detector (stereotactic fields detector : SFD) with a 6 MV photon beam and a water phantom system (IBA, Germany). Percentage depth dose (PDD) was measured for different field sets (cones : ${\Phi}1\;cm$, ${\Phi}2\;cm$, ${\Phi}3\;cm$ ; square fields : $1{\times}1\;cm^2$, $2{\times}2\;cm^2$, $3{\times}3\;cm^2$) at a source skin distance (SSD) of 100 cm. We measured the point depths at 1.5 cm, 5 cm, 10 cm, 20 cm, and 30 cm. The output factors were measured under the same geometrical conditions of the PDD and normalized at the maximum dose depth. To analyze the penumbra, we measured the dose profile with 95 cm of SSD, 5 cm of depth for each field sizes (${\Phi}1\;cm$, ${\Phi}3\;cm$, $1{\times}1\;cm^2$, and $3{\times}3\;cm^2$) using SFD. We obtained the values for every 1 mm interval in the physical field (90%) and 0.5 mm interval in the penumbra region (20 to 80%). The PDD variation of exclusive cones and square fields were 4.3 to 7.9% lesser than the standard field size ($10{\times}10\;cm^2$. The variation of PDD was reduced while the field size was increased. To compare the beam quality, we analyzed the $PDD_{20,10}$ and the results showed under the 1% of variations for all experiments except for ${\Phi}1\;cm$ cone and $1{\times}1\;cm^2$ fields. Output factors of exclusive cone were increased 3.1~4.6% than the square fields, and the penumbra region of exclusive cone was reduced 20% as compared to the square fields. As the previous researches report, it is very important for SRS and SFD that precise dosimetry in small beam fields. In this paper, we showed the effectiveness of exclusive cone, compared to square field. And we will study on the various detector characteristics for small beam fields.

Perforated Plates Design Effective Shielding (효율적 전자파 차폐를 위한 개구면 설계)

  • 양승인;명노훈
    • The Proceeding of the Korean Institute of Electromagnetic Engineering and Science
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    • v.2 no.3
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    • pp.60-66
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    • 1991
  • In this paper, circula and rectangular apertures arranged with triangular and rectangular lattices and having a certain thickness are considered for eddective electromagnctic wave shielding when the plane wave is incident normally to the perfectly conductingmaterrial. The shielding effectiveness is represented by the transmitted power which can be obtained by reflection and transmission coefficients using Floquet mode representation.

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Thermal Performance of PV Cells Exposed to Irradiation by a Parabolic Trough Concentrator (PTC형 태양열 집열기로 조사되는 PV cell의 열적 성능)

  • Hwang, Seon Yeob;Kang, Tae Gon;Boo, Joon Hong
    • 한국신재생에너지학회:학술대회논문집
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    • 2011.05a
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    • pp.68-68
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    • 2011
  • 본 연구에서는 PV cell이 직달 일사에 노출되는 경우와 집광된 태양광에 조사되는 경우의 성능을 비교하는 한편 집광기의 형태에 따른 열적 성능을 검토하고자 하였다. PV cell은 본질적으로 반도체의 특성을 가지므로 작동온도의 상승에 따라 성능이 저하된다는 사실이 알려져 있으며, 태양조사의 강도 및 밀도 등 특성에 따라서도 성능의 변화를 예상할 수 있다. 그러나 이러한 성능변화에 관련된 인자들과 그 영향의 크기에 대한 정량적인 기술자료가 부족하므로 설치와 이용에 한계가 있는 것이 현실이다. 인공태양 장치(solar simulator)를 이용하여 0.7에서 1.2 sun 범위의 태양 조사 환경에서 결정질 실리콘계 PV cell과 집광형 PV cell의 성능을 검토하였다. 집광에 사용한 PTC는 집광면적의 폭이 500 mm이며, 집광 조사면적이 최소 10 mm인 경우 이론적 최대 집광비가 50이었다. PTC의 축방향으로는 균일한 태양조사가 있게된다는 것을 가정하여 모델의 길이는 간편한 실험을 위해 150에서 500 mm의 범위에서 제작하였다. 수평으로 놓인 PTC의 상부 초점 위치로부터 집광면이 아래 쪽에 위치할수록 집광 조사 면적이 증가하므로 PV cell의 크기에 따라 PTC 초점의 위치로부터 거리를 결정하였다. 한편, PTC 자체의 성능도 촛점거리와 집광면 폭의 비에 따라 달라질 수 있다는 가정 하에, 포물면의 최저 위치로부터 촛점거리는 각각 300, 400 및 500 mm가 되도록 세가지 형태를 제작하여 사용하였다. 동일한 형태의 PTC에서 PV cell의 동일한 설치 위치에서도 최고 $110^{\circ}C$ 범위의 PV cell의 작동 (표면) 온도에 따른 성능의 차이를 관찰하기 위해 셀의 후면을 냉각시키는 경우와 그렇지 않은 경우를 비교하였다. PV cell의 표면 온도 측정을 위해서, 후면의 온도와 같이 광선 차단 효과의 우려가 없는 경우에는 열전대를 설치하였으며, 셀의 전면 온도 측정을 위해서는 비접촉식 적외선 온도계를 사용하였다. 냉각 방법으로는 공기를 이용한 자연대류와 액체를 사용하는 강제대류의 경우를 고려하였으며, 필요에 따라 적절히 설계된 히트싱크를 설치하여 비교 실험을 진행하였다. 강제대류 냉각의 경우는 항온조를 사용하여 순환하는 냉각수의 유량과 공급온도를 변화시킴으로써 PV cell의 작동온도를 조절하고, 이에 따른 발전 성능의 변화를 관찰하였다. 본 연구에서 도출한 실험 및 분석 결과는 PV cell의 설치 환경과 작동온도의 변화에 따라 그 성능 변화를 예측할 수 있는 기술적 자료를 제공함으로써 에너지 이용의 합리화를 도모하는데 기여할 수 있을 것이다.

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Calculation of Dose Distribution for SBRT Patient Using Geant4 Simulation Code (Geant4 전산모사 코드를 이용한 SBRT 환자의 선량분포 계산)

  • Kang, Jeongku;Lee, Jeongok;Lee, Dong Joon
    • Progress in Medical Physics
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    • v.26 no.1
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    • pp.36-41
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    • 2015
  • The Monte Carlo based dose calculation program for stereotactic body radiotherapy was developed in this study. The Geant4 toolkit widely used in the radiotherapy was used for this study. The photon energy spectrum of the medical linac studied in the previous research was applied for the patient dose calculations. The geometry of the radiation fields defined by multi-leaf collimators were taken into account in the PrimaryGeneratorAction class of the Geant4 code. The total of 8 fields were demonstrated in the patient dose calculations, where rotation matrix as a function of gantry angle was used for the determination of the source positions. The DicomHandler class converted the binary file format of the DICOM data containing the matrix number, pixel size, endian type, HU number, bit size, padding value and high bits order to the ASCII file format. The patient phantom was constructed using the converted ASCII file. The EGSnrc code was used to compare the calculation efficiency of the material data.

Physical Characteristics Comparison of Virtual Wedge Device with Physical Wedge (가상쐐기와 기존쐐기의 물리적 특성 비교)

  • Choi Dong-Rak;Shin Kyung Hwan;Lee Kyu Chan;Kim Dae Yong;Ahn Yong Chan;Lim Do Hoon;Kim Moon Kyun;Huh Seung Jae
    • Radiation Oncology Journal
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    • v.17 no.1
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    • pp.78-83
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    • 1999
  • Purpose : We have compared the characteristics of Siemens virtual wedge device with physical wedges for clinical application. Materials and Methods : We investigated the characteristics of virtual and physical wedges for various wedge angles (15, 30, 45, and 60$^{\circ}$) using 6- and 15MV photon beams. Wedge factors were measured in water using an ion chamber for various field sizes and depths. In case of virtual wedge device, as upper jaw moves during irradiation, wedge angles were estimated by accumulated doses. These measurements were performed at off-axis points perpendicular to the beam central axis in water for a 15cm${\times}$20cm radiation field size at the depth of loom. Surface doses without and with virtual or physical wedges were measured using a parallel plate ion chamber at surface. Field size was 15cm H20cm and a polystyrene phantom was used. Results : For various field sizes, virtual and physical wedge factors were changed by maximum 2.1% and 3.9%) , respectively. For various depths, virtual and physical wedge factors were changed by maximum 1.9% and 2.9%, respectively. No major difference was found between the virtual and physical wedge angles and the difference was within 0.5$^{\circ}$ . Suface dose with physical wedge was reduced by maximum 20% (x-ray beam :6 MV, wedge angle:45$^{\circ}$, 550: 80 cm) relative to one with virtual wedge or without wedge. Conclusions : Comparison of the characteristics of Siemens virtual wedge device with physical wedges was performed. Depth dependence of virtual wedge factor was smaller than that of physical wedge factor. Virtual and physical wedge factors were nearly independent of field sizes. The accuracy of virtual and physical wedge angles was excellent. Surface dose was found to be reduced using physical wedge.

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Application of the Equivalent-Field Method for Output Calculation: Is it safe for elongated x-ray fields\ulcorner (출력인자 계산에 이용되는 등가면법의 타당성 연구 : 장방형 X-선 조사면에 대해서 안전한가\ulcorner)

  • Kim, Chang-Seon;Kim, Chul-Yong;Park, Myung-Sun
    • Progress in Medical Physics
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    • v.9 no.4
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    • pp.195-200
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    • 1998
  • Purpose: When an elongated x-ray field is used for treating a patient, the equivalent- field method is commonly used for the output calculation. This study is intended for investigating potential factors such as, beam quality, field elongation ratio, and depth of measurement, which might effect on the applicability of the equivalent square technique for output calculation. The derivation of a 'rule of thumb' for the application criteria of the equivalent-field method is also aimed. Materials and Methods: Three x-ray beams, 4-, 6- and 10-MV, were employed for this study. Width of the rectangular field was ranged from 5-40 cm and the elongation ratio (length/width) 1:0 to 10:0. An elongation effect was measured in a water phantom at three different depths, dmax, 5-cm, and 10-cm. For an elongated field and its equivalent square field, the output factor was measured and the difference in the output factor were examined between two fields. Results and Discussions: As the elongation ratio increases, a larger discrepancy in outputs is observed between the elongated rectangular field and its corresponding equivalent square field. Output was measured larger for an elongated field than for its corresponding equivalent square field and the maximal difference over 10 % was found. The difference was found larger for the smaller field with the same elongation ratio. The effect of the beam quality and the depth of measurement on the output difference was minimal. Conclusion: Based on the study, there is criteria for the application of the method for output calculation. For the combination of long axis and elongation ratio whose relationship satisfies Elongation ratio < (0.48) (Long axis) - 0.5, the equivalent-field method is valid for output calculation within 2 % for the field whose long axis < 25-cm. For other combinations, instead of using the equivalent-field method, direct output measurement is recommended. This criteria can be applied for 4-10 MV x-ray beams up to 10-cm depth.

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A DESCRIPTIVE STUDY OF KOREAN NURSING STUDENTS생 ATTITUDES TOWARD MENTAL ILLNESS (정신질환에 대한 간호학생의 태도 연구)

  • Chu, Myung-Soon
    • Journal of Korean Academy of Nursing
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    • v.4 no.3
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    • pp.13-32
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    • 1974
  • 본 연구는 한국의 학사과정에 등록한 간호학생의 정신질환에 대한 태도를 조사 연구하는데 주목적이 있고, 연구 결과에 의한 학생들의 태도와 학생들의 종교, 지역사회의 크기, 장래에 정신과 간호를 그들의 근무영역으로 삼을 것인가에 대한 관련도를 조사하는데 두번째의 목적이 있고, 세번째의 목적은 미국에서 발표된 정신질환에 대한 태도 연구와 본 연구의 결과에서 나타나는 한국 학생들과의 태도를 비교해 보는 데에 있겠다. 본 연구의 대상은 서울대학교 의과대학 간호학과 4학년생(1972년도) 이었으며, 미국과외 비교 연구를 위해서 Morris의 간호학생 태도 연구를 사용했다. 본 연구에 사용된 도구는 Cohen과 Straining이 발달시킨 51항으로 구성된 Opinions About Mental Illness (O.M.I) Scale이며, 학생들로부터 개인적인 자료를 얻기 위 해 4항이 더 첨 가되었다. 연구 결과를 보면 간호학생들의 정신질환에 대한 부정적인 태도가 보여졌다. 즉, 높은 권위의식 (요소, A)과 사회적 제한성 (요소, D)을 표현했고, 자비심 (요소, B)은 낮게 표현되었으니. 이는 정신질환에 대한 부정적인 태도를 보여주었다. 또한 본 연구에서 학생들의 종교와 졸업 후 정신과 간호 영역에서 근무할 취향이 O.M.I.에서 보여지는 태도면에 영향을 줌이 밝혀졌다. 즉 기독교인과 졸업 후 정신과간호원 지망생이 비 기독교인과 비 정신과간호원 지망생보다 정신질환에 대한 태도에 보다 긍정적인 반응을 보였다. 학생들이 살고있는 지역 사회의 크기와 O,M,I. 척도에서 보여지는 태도 면에 통계학적인 유의의 차이는 없었다. 본 연구의 결과로 보여진 정신질환에 대한 간호학생들의 부정적 인 태도는 간호교육의 단면적인 평가도 되겠지만 정신과 간호교육과정이나 다른 교육과정의 내용 면의 재 고려와 아울러 긍정적인 방향으로의 태도변화를 위해 보다 많은 연구가 필요하겠다.

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Distribution and Ecology of Genus Corbicula in the North Kyungsang Province I. Distribution and Classification of Genus Corbicula in the North Kyungsang Province (경상북도 재첩자원 분포 및 생태 조사 1.경상북도산 재첩선(Corbicula) 이매패류)

  • 주문규;변경숙;장명호
    • Journal of Aquaculture
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    • v.11 no.4
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    • pp.581-592
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    • 1998
  • To know on the distribution and ecological characteristics of genus Corbicula field survey made from August 1997 to July 1998 in the North Kyungsang Province. Three species, i.e. Corbicula japonica, C. leand and C. papyracea, were inhabited in the North Kyungsang Provice. C. japonica was dioecious and oviparous species and C. leana and C. papyracea were monoecious and viviparous species.

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The characteristics on dose distribution of a large field (넓은 광자선 조사면($40{\times}40cm^2$ 이상)의 선량분포 특성)

  • Lee Sang Rok;Jeong Deok Yang;Lee Byoung Koo;Kwon Young Ho
    • The Journal of Korean Society for Radiation Therapy
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    • v.15 no.1
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    • pp.19-27
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    • 2003
  • I. Purpose In special cases of Total Body Irradiation(TBI), Half Body Irradiation(HBI), Non-Hodgkin's lymphoma, E-Wing's sarcoma, lymphosarcoma and neuroblastoma a large field can be used clinically. The dose distribution of a large field can use the measurement result which gets from dose distribution of a small field (standard SSD 100cm, size of field under $40{\times}40cm2$) in the substitution which always measures in practice and it will be able to calibrate. With only the method of simple calculation, it is difficult to know the dose and its uniformity of actual body region by various factor of scatter radiation. II. Method & Materials In this study, using Multidata Water Phantom from standard SSD 100cm according to the size change of field, it measures the basic parameter (PDD,TMR,Output,Sc,Sp) From SSD 180cm (phantom is to the bottom vertically) according to increasing of a field, it measures a basic parameter. From SSD 350cm (phantom is to the surface of a wall, using small water phantom. which includes mylar capable of horizontal beam's measurement) it measured with the same method and compared with each other. III. Results & Conclusion In comparison with the standard dose data, parameter which measures between SSD 180cm and 350cm, it turned out there was little difference. The error range is not up to extent of the experimental error. In order to get the accurate data, it dose measures from anthropomorphous phantom or for this objective the dose measurement which is the possibility of getting the absolute value which uses the unlimited phantom that is devised especially is demanded. Additionally, it needs to consider ionization chamber use of small volume and stem effect of cable by a large field.

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