• 상하수도학회지
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• 제18권3호
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• pp.377-384
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• 2004

In the present study, a feasibility of an advanced oxidation process using UV/Hydrogen peroxide($H_2O_2$) system equipped with a medium pressure lamp for secondary effluent reclamation was investigated. Initial concentration of $H_2O_2$ and pH were changed to determine the optimum operation condition for the system. The removal efficiency of color was than 80% with 14.3mg/L of initial $H_2O_2$ and 5 minute of contact time in the UV/$H_2O_2$ system. The color removal was analyzed using first-order reaction equation. The dependence of rate constant (k) on initial $H_2O_2$ represented the rational relationship with maximum value. Residual $H_2O_2$ caused increase of effluent COD, since analyzing agent, dichromate, reacted with $H_2O_2$ in the sample. Therefore, excess initial concentration of $H_2O_2$ would significantly affect effluent COD measurement. At pH variation experiment, both residual $H_2O_2$ and color showed peak in the neutral pH range with the same pattern. Effect of $H_2O_2$ dose also enhanced color removal but raised residual $H_2O_2$ problem in the continuous operation UV system. In conclusion, these results indicated that medium pressure UV/$H_2O_2$ system could be used to control color in the secondary effluent for reclamation and reuse.

• 대한방사선치료학회지
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• 제26권2호
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• pp.265-272
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• 2014

목 적 : 전뇌 방사선 치료 시 산란선으로 인하여 영향을 받는 갑상선의 피폭선량을 감소시키기 위해 차폐체를 사용하여 갑상선의 차폐 효과를 평가하고자 한다. 대상 및 방법 : 갑상선의 피폭선량을 측정하기 위해 선형가속기(Clinac iX. VARIAN, USA)를 이용하여 6 MV X선, 300 cGy를 인체모형팬텀에 대향 2문 조사하였다. 갑상선의 입사표면선량을 측정하기 위해 인체모형팬텀의 10번째 슬라이스 표면에 유리선량계 다섯 개를 1.5 cm 간격으로 위치시킨 후 차폐체 미사용, bismuth 차폐체 사용, 0.5 mmPb 차폐체 사용, 자체 제작한 1.0 mmPb 차폐체를 사용하여 각각 5회씩 측정하여 평균값을 산출하였다. 또한, 같은 위치에서 갑상선 심부선량을 측정하기 위해서 인체모형팬텀의 10번째 슬라이스 2.5 cm 깊이에서 유리선량계 다섯 개를 1.5 cm 간격으로 위치시킨 후 차폐체 미사용, bismuth 차폐체 사용, 0.5 mmPb 차폐체 사용, 자체 제작한 1.0 mmPb 차폐체를 사용하여 각각 5회씩 측정하여 평균값을 산출하였다. 결 과 : 갑상선의 입사표면선량은 차폐체 미사용 시 44.89 mGy로 측정되었고, bismuth 차폐체는 36.03 mGy, 0.5 mmPb 차폐체는 31.03 mGy, 자체 제작한 1.0 mmPb 차폐체는 23.21 mGy로 측정되었다. 또한, 갑상선의 심부선량은 차폐체 미사용 시 36.10 mGy로 측정되었고, bismuth 차폐체는 34.52 mGy, 0.5 mmPb 차폐체는 32.28 mGy, 자체 제작한 1.0 mmPb 차폐체는 25.50 mGy로 측정되었다. 결 론 : 전뇌 방사선 치료 시 방사선 조사면 밖의 영역에서 발생하는 이차 산란 및 누출 선량에 의해 영향을 받는 갑상선에 대하여 차폐체를 사용했을 때 갑상선 심부는 약 11~30%, 갑상선 표면은 약 20~48% 정도의 피폭선량 감소 효과가 나타났다. 따라서 전뇌 방사선 치료 시 갑상선 차폐체를 사용함으로써 갑상선을 효과적으로 보호하며 치료를 시행할 수 있을 것으로 사료된다.

• Journal of Korean Neurosurgical Society
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• 제42권3호
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• pp.200-204
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• 2007

Objective : Radiation therapy is an important treatment for brain tumor. However, serious complications such as radiation necrosis can occur and it may be secondary to the expression of acute phase genes, like cytokines. In particular, inflammatory cytokines (IL-$1{\beta}$, TNF-${\alpha}$) and other immunomodulatory cytokines (TNF-${\alpha}$, TGF-${\beta}1$) might be changed after irradiation (high single dose irradiation). Although it has been reported that IL-1 level is remarkably elevated within 8 week after the irradiation to the rat brain. the change of cytokines levels at acute phase (within 24 hours) has not been reported. In the present study, we examined TNF-${\alpha}$, TGF-${\beta}1$, and IL-$1{\beta}$ levels in acute phase to clarify the early effect of cytokines on the radiation-induced brain damage. Methods : Fifty Sprague-Dawley rats were used and these were divided into irradiation group and control group. After a burr-hole trephination on the right parietal area using a drill, a single 10Gy was irradiated at the trephined site. Their forebrains were extirpated at 30 min, 2 hr, 8 hr, 12 hr and 24 hr, respectively and examined for the expression of TNF-${\alpha}$, TGF-${\beta}1$, and IL-$1{\beta}$. Results : The expression of TNF-${\alpha}$ and TGF-${\beta}1$ were decreased until 12 hr after irradiation but elevated thereafter. The expression of IL-1 was peak at 8 hr and then decreased until 12 hr but elevated after this time window. The present study indicated that expression of cytokines (TNF-${\alpha}$, TGF-${\beta}1$ and IL-$1{\beta}$) were increased at 24 hr after the irradiation to the rat brain. IL-$1{\beta}$ level, on the other hand. reached peak at 8 hr after radiation injury. Conclusion : These findings indicate that IL-1, among various cytokines, may have a more important role in the inflammatory reaction by radiation injury at acute phase and provide some clues for better understanding of the pathogenesis of radiation injury.

• Radiation Oncology Journal
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• 제31권4호
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• pp.206-215
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• 2013

Purpose: Re-irradiation (re-RT) is considered a treatment option for inoperable locoregionally recurrent head and neck cancer (HNC) after prior radiotherapy. We evaluated the efficacy and safety of re-RT using Helical Tomotherapy as image-guided intensity-modulated radiotherapy in recurrent HNC. Materials and Methods: Patients diagnosed with recurrent HNC and received re-RT were retrospectively reviewed. Primary endpoint was overall survival (OS) and secondary endpoints were locoregional control and toxicities. Results: The median follow-up period of total 9 patients was 18.7 months (range, 4.1 to 76 months) and that of 3 alive patients was 49 months (range, 47 to 76 months). Median dose of first radiotherapy and re-RT was 64.8 and 47.5 $Gy_{10}$. Median cumulative dose of the two courses of radiotherapy was 116.3 $Gy_{10}$ (range, 91.8 to 128.9 $Gy_{10}$) while the median interval between the two courses of radiation was 25 months (range, 4 to 137 months). The response rate after re-RT of the evaluated 8 patients was 75% (complete response, 4; partial response, 2). Median locoregional relapse-free survival after re-RT was 11.9 months (range, 3.4 to 75.1 months) and 5 patients eventually presented with treatment failure (in-field failure, 2; in- and out-field failure, 2; out-field failure, 1). Median OS of the 8 patients was 20.3 months (range, 4.1 to 75.1 months). One- and two-year OS rates were 62.5% and 50%, respectively. Grade 3 leucopenia developed in one patient as acute toxicity, and grade 2 osteonecrosis and trismus as chronic toxicity in another patient. Conclusion: Re-RT using Helical Tomotherapy for previously irradiated patients with unresectable locoregionally recurrent HNC may be a feasible treatment option with long-term survival and acceptable toxicities.

• 한국측량학회지
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• 제35권1호
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• pp.55-62
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• 2017

The SRP (Solar Radiation Pressure) model has always been an issue in the dynamic GPS (Global Positioning System) orbit determination. The widely used CODE (Center for Orbit Determination in Europe) model and its variants have nine parameters to estimate the solar radiation pressure from the Sun and to absorb the remaining forces. However, these parameters show a very high correlation with each other and, therefore, only several of them are estimated at most of the IGS (International GNSS Service) analysis centers. In this study, we attempted to numerically verify the correlation between the parameters. For this purpose, a bi-directional, multi-step numerical integrator was developed. The correlation between the SRP parameters was analyzed in terms of post-fit residuals of the orbit. The integrated orbit was fitted to the IGS final orbit as external observations. On top of the parametric analysis of the SRP parameters, we also verified the capabilities of orbit prediction at later time epochs. As a secondary criterion for orbit quality, the positional discontinuity of the daily arcs was also analyzed. The resulting post-fit RMSE (Root-Mean-Squared Error) shows a level of 4.8 mm on average and there is no significant difference between block types. Since the once-per-revolution parameters in the Y-axis are highly correlated with those in the B-axis, the periodic terms in the D- and Y-axis are constrained to zero in order to resolve the correlations. The 6-hr predicted orbit based on the previous day yields about 3 cm or less compared to the IGS final orbit for a week, and reaches up to 6 cm for 24 hours (except for one day). The mean positional discontinuity at the boundary of two 1-day arcs is on the level of 1.4 cm for all non-eclipsing satellites. The developed orbit integrator shows a high performance in statistics of RMSE and positional discontinuity, as well as the separations of the dynamic parameters. In further research, additional verification of the reference frame for the estimated orbit using SLR is necessary to confirm the consistency of the orbit frames.

• 한국전자파학회논문지
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• 제20권12호
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• pp.1233-1242
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• 2009

본 논문에서는 도체 판 대신 인공 자기 도체를 반사판으로 이용하여 방사 특성이 개선되고 두께를 줄인 PCS용 기지국 안테나 구조를 제안하였다. 반사판으로 도체 판을 사용하는 기존 기지국 안테나의 경우, 도체 판 끝부분에서 기생 방사가 발생하고 이는 안테나의 후방사를 증가시켜 기지국 안테나의 방사 특성을 악화시킨다. 하지만 인공 자기 도체를 사용하면 표면에서의 높은 임피던스에 의해 표면파가 억압되어 후방사를 크게 줄일 수 있다. 그리고 부엽 특성도 개선되어 서비스 지역이 겹치는 문제를 막을 수 있다. 뿐만 아니라, 인공 자기 도체 표면에서의 $0^{\circ}$ 반사 위상에 의해 기지국 안테나의 두께를 또한 줄일 수 있다.

• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2002년도 Proceedings
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• pp.241-243
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• 2002

New types of protocols have been recently in development, all based on an absorbed dose-to-water with the aim of improving the accuracy of measurements of absorbed dose to water. IAEA TRS-277, the air-kerma standard-based present protocol, and IAEA TRS-398 and AAPM TG-51, the absorbed dose-to-water standard-based new one, were studied and compared theoretically and experimentally for photon beams of 6, 10, and 15 MV. NE 2571 and 3 Farmer types of ionization chambers in widely commercial use were used to determine an absorbed dose to water at the reference depth in water. Two different kinds of calibration factors were given respectively for every chamber calibrated in $\^$60/CO gamma ray beams from a Korean Secondary Standard Dosimetry Laboratory (KFDA). This work shows that there is around 1 % of difference of absorbed doses measured between two different types of calibration systems owing to different physical parameters and reference conditions used. We hope this work to help form the basis on development of new type of protocol in Korea.

• 대한방사선기술학회지:방사선기술과학
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• 제38권4호
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• pp.477-482
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• 2015

핵의학과에 근무하는 방사선작업종사자들은 방사성동위원소의 생산, 분배, 조제, 주입 등의 업무를 진행하며, 이러한 과정에서 손에 대한 방사선 피폭이 높게 발생한다. 이에 본 연구에서는 핵의학과에서 이용되는 방사성동위원소의 에너지로서 140 keV와 511 keV의 ${\gamma}$선에 대한 차폐효과를 몬테카를로 모의 모사를 통해 분석하였다. 모의실험 결과 140 keV ${\gamma}$선은 차폐체에 두께와 상관없이 모두 방사선에 대한 차폐효과가 발생되었으며, 511 keV의 ${\gamma}$선에서는 1.1 mm 이상에서 차폐효과가 발생되었다. 그러나 1.1 mm 미만에서는 2차적으로 발생된 산란선으로 인하여 차폐효과가 없었으며, 오히려 방사성동위원소의 피폭선량이 증가되었다. 따라서 효율적인 방사선 방어를 위해서는 핵종별 에너지에 따른 납 차폐체의 두께를 고려하여야 할 것이다.

• Nuclear Engineering and Technology
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• 제54권9호
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• pp.3317-3323
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• 2022

Half Value Layer calculations theoretically need prior specification of linear attenuation calculations, since the HVL value is derived by dividing ln(2) by the linear attenuation coefficient. The purpose of this study was to establish a direct computational model for determining HVL, a vital parameter in nuclear radiation safety studies and shielding material design. Accordingly, a typical gamma-ray transmission setup has been modeled using MCNPX (version 2.4.0) general-purpose Monte Carlo code. The MCNPX code's INPUT file was designed with two detection locations for primary and secondary gamma-rays, as well as attenuator material between those detectors. Next, Half Value Layer values of some well-known gamma-ray shielding materials such as lead and ordinary concrete have been calculated throughout a broad gamma-ray energy range. The outcomes were then compared to data from the National Institute of Standards and Technology. The Half Value Layer values obtained from MCNPX were reported to be highly compatible with the HVL values obtained from the NIST standard database. Our results indicate that the developed INPUT file may be utilized for direct computations of Half Value Layer values for nuclear safety assessments as well as medical radiation applications. In conclusion, advanced simulation methods such as the Monte Carlo code are very powerful and useful instruments that should be considered for daily radiation safety measures. The modeled MCNPX input file will be provided to the scientific community upon reasonable request.

• 대한방사선치료학회지
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• 제31권1호
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• pp.51-56
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• 2019

목 적: 수술 후 유방암 환자의 1차 방사선치료 후 2차 방사선치료 시 단일전자선을 사용하는 것과 서로 다른 에너지의 전자선을 혼합하여 사용하는 방법에 대해 유용성을 평가하고자 한다. 대상 및 방법: 본 연구에서는 2018년 1월부터 10월까지 본원 유방암 방사선 치료 환자를 대상으로 하였으며, 혼합 전자선을 사용하여 2차 치료를 진행한 환자 59명 중 에너지 6 MeV, 9 MeV를 혼합 사용한 환자 40명(A그룹)과 9 MeV, 12 MeV를 혼합 사용한 환자 19명(B그룹)을 대상으로 진행하였다. 각 그룹의 환자마다 6 MeV, 9 MeV, Combine(6 MeV / 9 MeV)와 9 MeV, 12 MeV, Combine(9 MeV / 12 MeV) 각기 다른 방법으로 세 가지 치료계획을 세우고, 원발병소에 전달되는 최대선량, D95, D5과 폐의 전달되는 최대선량, 평균선량, $V_3$, $V_5$, $V_{10}$을 비교 분석하였다. 결 과: A그룹 치료계획의 D95 평균값은 6 MeV에서 $785.33{\pm}225.37cGy$, 9 MeV에서 $1121.79{\pm}87.02cGy$, SUM(6 MeV / 9 MeV)에서 $1010.98{\pm}111.17cGy$였으며, 6 MeV / 9 MeV에서의 평균값이 처방 선량에 가장 적합했다. 치료하는 유방 방향의 폐의 저선량 영역 $V_3$,$V_5$의 평균값은 6 MeV / 9 MeV에서 $3.24{\pm}3.49%$, $0.72{\pm}1.55%$였고, 9 MeV에서 $7.25{\pm}4.59%$, $3.07{\pm}2.64%$로 가장 높은 값을 보였고, 6 MeV에서 $0.21{\pm}0.45%$, $0.03{\pm}0.07%$로 가장 낮은 값을 보였다. 폐의 최대선량과 평균선량은 6 MeV / 9 MeV에서 $727.78{\pm}137.27cGy$, $49.16{\pm}24.44cGy$였으며, 9 MeV에서 $998.97{\pm}114.35cGy$, $85.33{\pm}41.18cGy$로 가장 높았고, 6 MeV에서 $387.78{\pm}208.88cGy$, $9.27{\pm}6.60cGy$로 가장 낮았다. $V_{10}$의 값은 모두 0에 가까웠다. B그룹도 A그룹의 패턴으로 나타났다. 결 론: 폐의 $V_3$, $V_5$의 저선량 영역에서 상대적인 차이가 나타났으며, 혼합 에너지 적용 시 원발병소의 선량 전달에 있어서 가장 효과적임을 알 수 있었다. 유방암 추가 방사선 치료 시 전자선 에너지를 combine하여 사용하는 방법이 에너지 재원으로부터 제한되는 에너지의 효과를 좀 더 효과적으로 사용할 수 있는 방법이라고 사료되며 비록 작은 선량차이이기 때문에 간과하고 넘어갈 수 있는 부분들도 다시 한번 생각해본다면 조금 더 환자에게 도움이 되는 방사선 치료가 될 수 있을 것으로 사료된다.