• Title/Summary/Keyword: P-V 선도

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Effect of an Acrylic Plate and SSD on Dose Profile and Depth Dose Distribution of 9 MeV Electron Beams (에너지 저하체로서 아크릴과 SSD 가 9MeV 전자선의 측방 및 깊이선량분포에 미치는 효과)

  • 강위생
    • Progress in Medical Physics
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    • v.9 no.2
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    • pp.65-71
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    • 1998
  • The aims are to evaluate the effects of an 1.0 cm acrylic plate and SSD on the dose profile and depth dose distribution of 9 MeV electron beam and to analyse adequacy for using an acrylic plate to reduce energy of electron beams. An acrylic plate of 1.0 cm thickness was used to reduce energy of 9 MeV electron beam to 7 MeV. The plate was put on an electron applicator at 65.4 cm distance from x-ray target. The size of the applicator was 10${\times}$l0cm at 100 cm SSD. For 100cm, l05cm and 110cm SSD, depth dose on beam axis and dose profiles at d$\_$max/ on two principal axes were measured using a 3D water phantom. From depth dose distributions, d$\_$max/, d$\_$85/, d$\_$50/ and R$\_$p/, surface dose, and mean energy and peak energy at surface were compared. From dose profiles flatness, penumbra width and actual field size were compared. For comparison, 9 MeV electron beams were measured. Surface dose of 7 MeV electron beams was changed from 85.5% to 82.2% increasing SSD from 100 cm to 110 cm, and except for dose buildup region, depth dose distributions were independent of SSD. Flatness of 7 MeV ranged from 4.7% to 10.4% increasing SSD, comparing 1.4% to 3.5% for 9 MeV. Penumbra width of 7 MeV ranged from 1.52 cm to 3.03 cm, comparing 1.14 cm to 1.63 cm for 9 MeV. Actual field size increased from 10.75 cm to 12.85 cm with SSD, comparing 10.32 cm to 11.46 cm for 9 MeV. Virtual SSD's of 7 and 9 MeV were respectively 49.8 cm and 88.5cm. In using energy reducer in electron therapy, depth dose distribution were independent of SSD except for buildup region as well as open field. In case of using energy reducer, increasing SSD made flatness to deteriorate more severely, penumbra width more wide, field size to increase more rapidly and virtual SSD more short comparing with original electron beam. In conclusion, it is desirable to use no energy reducer for electron beam, especially for long SSD.

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DNA Damage by X-ray and Low Energy Electron Beam Irradiation (X선과 저에너지 전자선에 의한 DNA 손상)

  • Park, Yeun-Soo;Noh, Hyung-Ah;Cho, Hyuck;Dumont, Ariane;Ptasinska, Sylwia;Bass, Andrew D.;Sanche, Leon
    • Journal of Radiation Protection and Research
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    • v.33 no.2
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    • pp.53-59
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    • 2008
  • We observed DNA damages as a function of mean absorbed dose to identify the indirect effect of high-energy radiation such as x-ray. Monolayer films of lyophilized pGEM-3Zf(-) plasmid DNA deposited on tantalum foils were exposed to Al $K{\alpha}$ X-ray (1.5 keV) for 0, 3, 7 and 10 min, respectively, in a condition of ultrahigh vacuum state. We compared DNA damages by X-ray irradiation with those by 3 eV electron irradiation. X-ray photons produced low-energy electrons (mainly below 20 eV) from the tantalum foils and DNA damage was induced chiefly by these electrons. For electron beam irradiation, DNA damage was directly caused by 3 eV electrons. Irradiated DNA was analyzed by agarose gel electrophoresis and quantified by ImagaQuant program. The quantities of remained supercoiled DNA after irradiation were linearly decreased as a function of mean absorbed dose. On the other hand, the yields of nicked circular (single strand break, SSB) and interduplex crosslinked form 1 DNA were linearly increased as a function of mean absorbed dose. From this study, it was confirmed that DNA damage was also induced by low energy electrons ($0{\sim}10\;eV$) even below threshold energies for the ionization of DNA.

A Development of Home Automation Using Power Line Carrier (전력선 반송방식을 이용한 Home Automation 개발)

  • 박충규;오상기;나채동
    • The Proceedings of the Korean Institute of Illuminating and Electrical Installation Engineers
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    • v.5 no.4
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    • pp.43-51
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    • 1991
  • 본 논문에서는 전력선 반송통신을 이용한 가정내 전기기기의 감시제어 시스템인 "전동선 HMCS"를 개발했다. 통신방식은 양방향으로서 반송파 주파수 125[kHz]의 FSK디지탈 신호를 전등선에 중첩시키는 방식이며, 제어방식은 Polling 방식을 채용했다. 그리고 시스템의 송신출력은 4Vp-p이고, 수신감도는 CISPR 잡음 규제등을 고려하여 10[mV] 이상으로 설계하였다. 개발 시스템의 성능은 58[dB] 시스템 여유도와 1.78$\times$10-7의 에러확률을 갖는다.에러확률을 갖는다.

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Structural dependences of the extinction in an 1.55 $1.55{\mu}m$ InGaAsP/InGaAsP multiple-quantum-well electro-absorption modulator (1.55 $1.55{\mu}m$ InGaAsP/InGaAsP MQW 광흡수 변조기에서 구조변수가 소광특성에 미치는 영향)

  • 민영선;심종인;어영선
    • Korean Journal of Optics and Photonics
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    • v.12 no.1
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    • pp.40-47
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    • 2001
  • The structural dependence of the performance of an 1.55 $1.55{\mu}m$ InGaAsPIInGaAsP MQW electro-absorption modulator for highspeed digital fiber communication was systematically investigated. The effects of n-doped SCH region length $t_n$ as well as the general structure parameters including quantum well number $N_w$, well-thickness $t_w$, detuning wavelength $\Delta\lambda$, and device length L were thoroughly analyzed. Thereby, a high-pelfoIDlance electro-absorption modulator with device length L of $100{\mu}m$ was successfully designed. The designed structure showed excellent characteristics that have residual loss less than -1.5 dB, operational voltage from 0 V to -2V, and extinction ratios of -2.92 dB at $V_{\alpha}$=-1 V and -10 dB at $V_{\alpha}$=-2V.X>=-2V.

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A Study on the Measurement of the Relative Nuclear Reaction Cross-Section of the natW(p,xn)176Re Reaction using 100 MeV Proton (100 MeV 양성자를 이용한 natW(p,xn)176Re 핵반응의 상대 핵반응단면적 측정에 대한 연구)

  • Lee, Samyol
    • Journal of the Korean Society of Radiology
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    • v.15 no.2
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    • pp.257-263
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    • 2021
  • This study derives the relative cross-section for the natW(p,xn)176Re nuclear reaction by measuring the gamma rays generated from the nuclear reaction with natural tungsten using a 100 MeV linear accelerator of the Korea Multi-purpose Accelerator Complex in the Korea Atomic Energy Research Institute. In general, research on isotopes with a short half-life always shows a tendency that the intensity of radioactivity decreases rapidly within a short period of time, making it very difficult to measure itself. In particular, 176Re is one of the relatively short radionuclides with a half-life of 5.3 minutes. In this study, 109.08 keV gamma rays generated from the 176Re isotope having such a short half-life were measured using a high-purity Ge detector(HPGe detector). The obtained relative measurements were the results in the 8 to 14 MeV proton energy domain published by Richard G. in 1967, and the TENDL-2019 value, which was the result of A. J. Koning in 2019, which evaluated the nuclear reaction cross-section by calculation based on this comparative analysis was performed. The results of this study are expected to be usefully applied to the design of nuclear fusion reactor which is known as future energy sources, elements ratio for the nuclear synthesis of astrophysics.

A Study on the Stability Control Method of Soft and Polluted Silt Soils (연약한 실트지반과 오염된 실트지반의 안정관리 방법에 관한 연구)

  • Ahn, Jong-Pil;Park, Sang-Bum
    • Journal of the Korean Geotechnical Society
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    • v.24 no.6
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    • pp.5-16
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    • 2008
  • This study investigated the existing theoretical backgrounds in order to examine the stability control method of lateral flow caused by the Plasticity of soils when unsymmetrical surcharge works on polluted soils and then compared and analyzed the results measured through model tests. Ultimate bearing power of ML and $ML_{p1}$ and $ML_{p2}$ obtained at surcharge(q)-settlement$(S_v)$ curve showed similar trends to ultimate bearing power obtained from control chart of deflection $(S_v-Y_m)$ by Tominaga.Hashimoto, that of $S_v-(Y_m/S_v)$ by Matsuo.Kawamura and that of $(q/Y_m)-q$ by Shibata.Sekiguchi and so it is considered that it has no problem in actual applicability. ${S_v-(Y_m/S_v)}$ of control chart of $ML_{p1}$ by Matsuo.Kawamura showed smaller value than ultimate bearing capacity value from surcharge-settlement curve $(q-S_v)$. Expression of ML of fracture baseline at stability control charge by Matsuo Kawamura is ${S_v=3.21exp}\{-0.48(Y_m/S_v)\}$ and expression of $ML_{p1}$ is ${S_v=3.26exp}\{-0.96(Y_m/S_v)\}$ and expression of $ML_{p2}$ is ${S_v=6.33exp}\{-0.45(Y_m/S_v)\}$.

Eu을 도핑한 ZnS 나노선의 온도변화에 따른 광발광 감쇄

  • Sin, Yong-Ho;Kim, Yong-Min;Kim, Sang-Dan;Ju, Sang-Hyeon
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.08a
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    • pp.416-416
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    • 2012
  • Eu이 도핑된 ZnS 나노선을 제작하여 온도변화에 따른 광발광 변화를 측정하였다. ESR 측정을 통하여 제작된 시료의 도펀트가 Eu2+ 상태임을 확인하였다. Au-catalyst와 Eu 도펀트 관련전이(Fig. 1, P2)와 표면 상태와 관련된 exciton (P1)의 온도변화에 대한 발광특성들이 100 meV 내외의 매우 큰 활성화 에너지를 가짐을 알 수 있었다. 이들 나노선들이 상온에서도 매우 강하게 발광하는 특성이 첨가된 도펀트와 강하게 관련이 있음을 알 수 있었으며, 이 실험을 통하여 Eu을 도핑한 ZnS 나노선들이 발광 소자로 이용 가능성함을 확인하였다.

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Overvoltage Analysis for One Side Energization of 765kV Line (765kV 선로 편단가압 시 전압상승 분석)

  • Seo, H.C.;Yeo, S.M.;Kim, C.H.;Yoo, Y.S.;Jo, B.S.
    • Proceedings of the KIEE Conference
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    • 2007.07a
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    • pp.608-609
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    • 2007
  • 본 논문에서는 765kV 선로의 편단가압 시 기존 운전중인 선로에서의 전압상승에 대하여 분석하였다. EMTP-RV를 이용하여 당진T/P$\sim$신서산S/S$\sim$신안성S/S의 실계통 모델을 구현하여, 선로길이 및 전원용량을 변경시키면서 시뮬레이션 하였으며 그 결과를 분석하였다.

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A study on the transmission system realization using residential power line carrier (전등선 반송방식 통신시스템 실현에 관한 연구)

  • Kim, In-Soo;Oh, Won-Rock;Kim, Kwan-Ho;Oh, Sang-Ki
    • Proceedings of the KIEE Conference
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    • 1989.07a
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    • pp.707-711
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    • 1989
  • This system exchange half-duplex serial data at 1200 baud by FSK modulating a carrier frequency at 200KHz over the 110V A.C. power line. Transmitter output voltage to A.C. line is 4V p-p and line sensitivity is selected 2.54mV because CISPR Noise limitation is $66dB{\mu}V$ at 150 ${\sim}$ 500KHz. The designed and realized system has abtained system margin of 58 dB and probability of error, Pe = $1.78{\times}10^{-7}$ was obtained

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Response Function of HPGe Detector using $^{23}Na$(p, $\gamma$)$^{24}Mg$ and $^{27}Al$(p, $\gamma$)$^{28}Si$ Reaction ($^{23}Na$(p, $\gamma$)$^{24}Mg$$^{27}Al$(p, $\gamma$)$^{28}Si$반응을 이용한 HPGe 검출기의 응답함수)

  • Park, Sang-Tae
    • Journal of Radiation Protection and Research
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    • v.35 no.2
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    • pp.85-90
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    • 2010
  • In the present work, peak relative efficiency for the energy was obtained and response function was worked out. This study was carried out using the high resolution high efficiency HPGe detector(diameter 78.7 mm, length 86.5 mm) and NaI(Tl) detector for anti-compton. The anti-coincidence of the signals from the two detectors could be used to lessen the Compton effect signal; thus, the $\gamma$-ray energy resolution could be improved. The $\gamma$-ray spectrum was measured at $55^{\circ}$ to the direction of the incident proton beam. Reaction spectrum was obtained from the $^{23}Na$(p, $\gamma$)$^{24}Mg$ reaction at $E_p$ = 1424 keV and $^{27}Al$(p, $\gamma$)$^{28}Si$ reaction at $E_p$ = 992 keV. To accelerate the incident proton which creates the (p, $\gamma$) capture reaction, the 3 MeV Pelletron accelerator at the Tokyo Institute of Technology was used. Response function was worked out by a noble technique. We worked out a response function from 1.2 to 9.4 MeV at intervals of 0.75 MeV.