• 자원환경지질
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• 제33권3호
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• pp.195-204
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• 2000

order to investigate physical characteristics and element concentrations of sediments, coastal bottom sediments were collected at 20 stations in the vicinity of Youngkwang Nuclear Power Plant. After air drying of samples in the laboratory. article size distribution was examined by Master sizer (X-350F), radio-activity by HPGe ${\gamma}$-spectrphotometer, and element concentrations by ICP-AES and AAS. According to particle size analysis , sediments are mainly composed of silt fraction weith 23% of sand, 65% of silt and 12% of clay on average. Most sediments are derived from muddy environment that silt dominates with the characteristics of 5.3${\varsigma}$ mean particle size, poorly sorted, very fine skewed and lepto-kurtic. Only two sediments are well sorted with sandy silt owing to wind, winnowing action, tide and current andits complex reactions. Element concentrations in the coastal bottom sediments are relatively high at finer sediment and show significant relationship with grain size. Index of geoaccumulation by heavy metals at every sampling station is classified as practically unpolluted. The radioactivities of the sediments were measured for 15 isotope elements, and 2 elements of K-40 and Cs-137 were detected in most sediments. The K-40 is the natural nuclide and the artificial nuclide of Cs-137 was thought to be derived from the fallout of past nuclear weapon test. The results of correlation coefficient between grain size and radioactivity shows that the activity of Cs-137 significantly increases in finer grain.

• Nuclear Engineering and Technology
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• 제45권1호
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• pp.61-66
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• 2013

Among the radioactive wastes generated from the nuclear power plant, a radioactive nuclide such as $^{129}I$ is classified as a difficult-to-measure (DTM) nuclide, owing to its low specific activity. Therefore, the establishment of an analytical procedure, including a chemical separation for $^{129}I$ as a representative DTM, becomes essential. In this report, the adsorption and recovery rate were measured by adding $^{125}I$ as a radio-isotopic tracer ($t_{1/2}$ = 60.14 d) to the simulation sample, in order to measure the activity concentration of $^{129}I$ in a pressurized-water reactor primary coolant. The optimum condition for the maximum recovery yield of iodine on the anion exchange resins (AG1 x2, 50-100 mesh, $Cl^-$ form) was found to be at pH 7. In this report, the effect of the boron content in a pressurized-water reactor primary coolant on the separation process of $^{129}I$ was examined, as was the effect of $^3H$ on the measurement of the activity of iodine. As a result, no influence of the boron content and of the simultaneous $^3H$ presence was found with activity concentrations of $^3H$ lower than 50 Bq/mL, and with a boron concentration of less than 2,000 ${\mu}g/mL$.

• Journal of Radiation Protection and Research
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• 제47권4호
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• pp.237-245
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• 2022

Background: The current study reports measurements of activity concentrations of radon (²²⁰Rn) and thoron (²²⁰Rn) in dwellings, followed by inhalation dose assessment of the public, and then by the development of regulation and the national radon action plan (NRAP) in Cameroon. Materials and Methods: Radon, thoron, and thoron progeny measurements were carried out from 2014 to 2017 using radon-thoron discriminative detectors (commercially RADUET) in 450 dwellings and thoron progeny monitors in 350 dwellings. From 2019 to 2020, radon track detectors (commercially RADTRAK) were deployed in 1,400 dwellings. It was found that activity concentrations of radon range in 1,850 houses from 10 to 2,620 Bq/㎥ with a geometric mean of 76 Bq/㎥. Results and Discussion: Activity concentrations of thoron range from 20 to 700 Bq/㎥ with a geometric mean of 107 Bq/㎥. Thoron equilibrium factor ranges from 0.01 to 0.6, with an arithmetic mean of 0.09 that is higher than the default value of 0.02 given by UNSCEAR. On average, 49%, 9%, and 2% of all surveyed houses have radon concentrations above 100, 200, and 300 Bq/㎥, respectively. The average contribution of thoron to the inhalation dose due to radon and thoron exposure is about 40%. Thus, thoron cannot be neglected in dose assessment to avoid biased results in radio-epidemiological studies. Only radon was considered in the drafted regulation and in the NRAP adopted in October 2020. Reference levels of 300 Bq/㎥ and 1,000 Bq/㎥ were recommended for dwellings and workplaces. Conclusion: Priority actions for the coming years include the following: radon risk mapping, promotion of a protection policy against radon in buildings, integration of the radon prevention and mitigation into the training of construction specialists, mitigation of dwellings and workplaces with high radon levels, increased public awareness of the health risks associated with radon, and development of programs on the scientific and technical aspects.

• Archives of Pharmacal Research
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• 제11권2호
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• pp.93-98
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• 1988

To elucidate the reaction mechanism of ginseng protein on its antiradiation activity, its effects were studied on sister chromatid exchanges (SCE) induced by UV irradiation in CHO-KI cells. When cells were irradiated with 254 nm UV light at the dose of 0 to 8erg$\textrm{mm}^2$, the frequencies of CSE were increased more than two fold. However, when radio protective ginseng protein was added to the cells before the after UV irradiation, SCE frequencies were decreased significantly at all UV doses in both cases with no significant differences. As the amount of ginseng protein was varied from 100 to 500 .mu.g/ml, with UV irradiation at 60 erg$\textrm{mm}^2$, SCE frequencies dropped sharply at the first two concentrations and then reached a sort of plateau in both cases of pre-and post-treatment. When the ginseng protein was treated alone without UV irradiation, there were no changes in SCE frequencies no matter when the protein was added. There results suggest that the ginseng protein could reduced DNA damages, which may play an important role in the reaction mechanism of radioprotective activity of the protein.

• 방사선산업학회지
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• 제5권1호
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• pp.15-20
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• 2011

Protein kinases are the most important drug targets for the treatment of numerous diseases. The involvement of protein kinase C (PKC) in many biological processes such as development, memory, cell differentiation, and proliferation has been demonstrated. PKC is recognized as an important player in carcinogenesis. Thus, a variety of PKC inhibitors have been investigated. Among them, flavonoids have been demonstrated to affect the activity of many mammalian in vitro enzyme systems. The recent investigation was performed to evaluate the inhibitory effects of hesperidin, which is a flavonoid, on the proliferation and carcinogenesis of many cancers. In this study, an efficient kinase assay based on a biochip using radio-phosphorylation was established and performed for an examination of the inhibitory effects of hesperidin on PKC activity at different concentrations of 50, 200, 500 nM. It was found that hesperidin shows inhibitory potency on PKC, and that the biochip can be used to rapidly screen kinase inhibitors resulting in the therapeutic agents.

• Journal of Radiation Protection and Research
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• 제19권3호
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• pp.179-188
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• 1994

생쥐의 난소에 미치는 방사선의 조직학적 및 기능적 영향을 조사하기 위하여 2.88Gy 및 7.2Gy의 방사선(Co-60)을 전신조사하였다. $7{\mu}m$ 두께의 조직절편을 제작하여 조직학적 관찰을 하였고, 방사면역측정 법을 이용하여 난소마쇄현탁액내 프로게스테론, 테스토스테론 및 에스트라디올을 정량하였다. 방사선조사로 유강소난포 및 무강소난포가 공히 높은 폐쇄율을 보였고, 난포내 프로게스테론의 농도가 증가되었으며 테스토스테론 및 에스트라디올의 농도는 감소되었다. 즉, 방사선을 조사함으로써 난소내 난포세포인 협막세포에 영향이 미친 결과 $3{\beta}-HSD(3{\beta}-hydroxysteroid\;dehydrogenase) $ 및 isomerase의 활성이 억제 혹은 둔화되어 테스토스테론 및 에스트라디올의 합성이 저하되었고 그 결과 난포의 폐쇄가 가속화되었다고 사료된다.

• Journal of the korean society of oceanography
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• 제35권1호
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• pp.16-33
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• 2000

In order to measure the vertical fluxes of particles and reactive radionuclides such as thorium and polonium isotopes, Dunbar-type sediment traps were freely deployed at the Ulleung Basin and in warm and cold water masses around the polar front of the East Sea. We estimated the ratios of the catched (F) to the predicted $^234$Th fluxes (P) using natural tracers pair $^234$Th-$^238$U. The F/P ratios are decreased with increasing water depth. Whereas the concentrations of suspended particles are homogeneous in water column, the mass fluxes are also decreased with increasing water depth like the F/P ratios. These facts indicate that organic matters of settling particles are destructed within the euphotic layer due to decomposition. Whereas regenerations of sinking particles are negligible in the cold water mass, about 80% of them are regenerated in the warm water mass during falling of large particles. These downward mass fluxes are closely correlated with their primary productions in euphotic zone. The activities of $^234$Th, $^228$Th and $^210$Po in the sinking material were increased with water depth. Because $^234$Th steadily produced in the water column are cumulatively adsorbed on the surface of sinking particles, vertical $^234$Th fluxes were observed to increase with water depth. Therefore, these sinking particles play important roles in transporting the particle reactive elements like thorium from surface to the deep sea. The scavenging processes including adsorption and settling reactions generate radio-disequilibrium between daughter and parent nuclides in water column. The activity ratios of $^234$Th/$^238$U and $^228$Th/$^228$Ra were observed to be < 1.0 in the surface water and approached to be equilibrium below the thermocline. The extent of the deficiency of daughter nuclides compared to the parents nuclide was highly correlated with the vertical particle flux. Because most of the $^210$Po in the surface water are scavenged on a labile phase and are recycled at sub-surface depths (< 200 m), the $^210$Po are always observed to be excess activities compared to $^226$Ra in surface water.

• 핵의학기술
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• 제14권2호
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• pp.172-176
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• 2010

PET/CT 검사에서 발생하는 환자의 움직임은 감쇠보정의 불일치를 초래하여 정량평가에 영향을 주게 되어 결과의 정확도를 저하시키게 된다. 본 연구에서는 PET/CT 3D 영상촬영에서 투과촬영 후 방출촬영의 위치변화에 따른 감쇠보정 불일치 시 감쇠보정 위치 변화 방법을 이용한 영상재구성법의 유용성에 대하여 평가하였다. GE Discovery STE16 장비에 스티로폼($20{\times}20{\times}10$ cm)의 중심점을 기준으로 x, y축 방향으로 ${\pm}2$, 6, 10 cm까지 1 mL 주사기 삽입 공간을 제작하였다. $^{18}F$-FDG 5 kBq/mL의 주사기를 중심점에서 투과촬영한 후 위치를 변화하여 방출촬영하고 위치 변화에 따른 감쇠보정 방법을 사용하여 영상을 얻었다. 재구성 방법은 반복영상 재구성법으로 반복횟수 2회, 부분집합 수 20을 적용하였으며 모든 방출촬영 데이터는 시간경과에 따른 붕괴보정을 적용하였다. 또한 주사기 위치에 관심영역을 설정한 후 방사능 값(kBq/mL)과 중심점에 대한 각 위치에서의 백분율 오차를 비교하였다. 방출영상의 중심점의 방사능 값은 2.30 kBq/mL이며, +x축 1.95, 1.82, 1.75 kBq/mL, -x축 2.07, 1.75, 1.65 kBq/mL, +y축 2.07, 1.87, 1.90 kBq/mL, -y축 2.17, 1.85, 1.67 kBq/mL로 나타났고, 백분율 오차는 +x축 15, 20, 23%, -x축 9, 23, 28%, +y축 12, 21, 20%, -y축 8, 22, 29%로 산출 되었다. 그리고 방출 영상에서 감쇠보정 위치변화 방법을 사용 하였을 경우 +x축 2.00, 1.95, 1.80 kBq/mL, -x축 2.25, 2.15, 1.90 kBq/mL, +y축 2.07, 1.90, 1.90 kBq/mL, -y축 2.10, 2.02, 1.72 kBq/mL로 나타났으며, 백분율 오차는 +x축 13, 15, 21%, -x축 2, 6, 17%, +y축 9, 17, 17%, -y축 8, 12, 25%로 산출 되었다. 감쇠보정 불일치 시 감쇠보정 위치변화 방법을 사용한 경우의 방사능 농도 값은 x, y축에서 평균 0.14, 0.03 kBq/mL 증가 하였고, 백분율 오차는 6.1, 4.2% 향상되었다. 또한 중심으로부터 멀어질수록 공간분해능이 저하되는 특성상 중심에서 먼 위치일수록 방사능 값의 저하현상은 커짐을 알 수 있었다. 그러나 실제 임상에서는 감약 정도가 더 커지기 때문에 이러한 불일치 시 그 오차는 더 클 것으로 사료된다. 따라서 감쇠보정이 일치하지 않는 부분의 병변에서는 감쇠보정 위치변화 방법을 적용하여 방사능 값의 오차를 감소시킬수 있을 것이다.

• 핵의학기술
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• 제16권1호
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• pp.102-107
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• 2012

단 반감기 핵종을 이용한 PET검사는 방사성동위원소의 빠른 물리적 붕괴로 인하여 영상 획득을 위한 계수검출이 제한적이다. 이러한 이유로 비교적 낮은 감도의 검사에서는 보다 정확한 정량적 평가를 위하여 긴 시간동안 영상 획득을 적용하기도 한다. 본 연구에서는 $^{11}C$와 $^{18}F$를 이용한 PET 검사 시 영상 획득 시간에 따른 차이를 평가하여 합리적인 영상 획득 시간에 관하여 알아보고자 한다. 1994 NEMA Phantom에 $^{11}C$은 $30.08{\pm}4.22MBq$, $^{18}F$은 $40.08{\pm}8.29MBq$을 증류수에 희석하여 채운 후 $^{11}C$은 동적영상 1분씩 20회, 정적 영상 20분, $^{18}F$은 동적영상 2분30초씩 20회, 정적영상 50분을 획득하였다. 모든 데이터는 동일한 재구성법을 적용하였으며, 시간의 경과에 따른 붕괴보정을 적용하였다. 방출영상에 관심영역을 설정하고 최대 방사능 농도값(kBq/mL)을 비교하였으며, 각각의 동적영상을 영상 획득 시간의 증가에 따라 1개씩 증가시켜 영상 합산(Image summation) 후 영상의 관심 영역 내에서의 최대 방사능 농도값(kBq/mL)을 평가하였다. $^{11}C$ 동적영상의 시간 경과에 따른 최대 방사능 농도값은 $3.85{\pm}0.45{\sim}5.15{\pm}0.50kBq/mL$, 정적영상은 $2.15{\pm}0.26kBq/mL$였다. $^{18}F$ 동적영상은 $9.09{\pm}0.42{\sim}9.48{\pm}0.31kBq/mL$, 정적영상은 $7.24{\pm}0.14kBq/mL$였다. $^{11}C$의 동적영상 합산에서 영상 획득 시간의 합이 5, 10, 15, 20분으로 증가할수록 $2.47{\pm}0.4$, $2.22{\pm}0.37$, $2.08{\pm}0.42$, $1.95{\pm}0.55kBq/mL$으로 감소하였으며, $^{18}F$의 경우 합산된 영상 획득 시간의 합이 12분 30초, 25분, 37분 30초, 50분으로 증가할수록 $7.89{\pm}0.27$, $7.61{\pm}0.23$, $7.36{\pm}0.21$, $7.31{\pm}0.23kBq/mL$으로 감소하였다. 영상의 질을 평가 하는 SNR에서는 $^{11}C$과 $^{18}F$ 모두 동적영상획득 방법에서는 주사 후 시간이 흐를수록 SNR가 저하 되었으나, 영상 합산획득 방법에서는 합산 횟수가 증가 할수록 SNR가 향상 되는 것을 알 수 있었다. 동적영상에서 시간 경과에 따른 최대 방사능 농도값은 $^{11}C$과 $^{18}F$에서 증가하였고, 동적영상 합산의 경우는 합산수가 증가함에 따라 최대 방사능 농도값은 $^{11}C$과 $^{18}F$ 감소함을 보였다. $^{18}F$을 이용할 경우에는 시간 경과에 따른 정량평가의 오차를 크게 고려하지 않아도 될 것으로 사료되고, $^{11}C$를 이용한 PET 검사는 시간경과에 따른 감쇠 보정의 오차를 감안하여 추가의 감쇠 보정법을 적용하거나 30%정도의 오차를 적용하여 정적영상 획득시간을 반감기의 25% 이내인 5분 내외로 설정해야 할 것이다.