• Title/Summary/Keyword: $^60$Co ${\gamma}$-rays

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Measurements of the Direction and Polarization Correlation for Cascade Gamma-rays of Co-60 and Cs-134 (Co-60과 Cs-134의 연발감마선에 대한 방향 및 편극상관 측정)

  • Hyung-Ju Woo;Kie-Hyung Chung;Hae-Ill Bak
    • Nuclear Engineering and Technology
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    • v.14 no.2
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    • pp.64-69
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    • 1982
  • Directional correlation measurements for the Co-60 and Cs-134 cascade gamma-rays have been performed in the angular range from 90$^{\circ}$ to 180$^{\circ}$ by use of the fast coincidence scintillation spectrometer incorporated with a gamma-ray polarimeter based on the Compton scattering effect to determine the polarization correlations. The experimental method together with the theoretical background is described, and the results are shown graphically to represent the consistency of the measurement with approximate theoretical estimates.

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$\gamma$-선 Radiography에 있어서의 피사체 산란선에 관한 연구

  • 허남;야고이명
    • Nuclear Engineering and Technology
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    • v.4 no.3
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    • pp.223-228
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    • 1972
  • In the radiography, of thick materials the scattered rays from an object are one of major causes to reduce the quality of the radiographic image on the film. To determine the rate of scattering of incident gamma rays by an objective specimen, film blacknesses are measured for various slit widths. For each measurement, the changes of a penetrameter's sensitivity are also evaluated. It is observed that the fault-detectability can be improved by reducing the slit width when the fault detectability deteriorates due to the increase in scattered gamma rays by thicker samples. This experiment has been carried out with the iron specimens and $^{60}$ Co source.

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Electrical conduction phenomena of OPP film irradiated by $Co^60-\gamma$ rays ($Co^60-\gamma$선으로 조사된 이축 연신 폴리프로필렌 필름의 전기전도 현상)

  • 박승협;박영제;이준웅
    • Electrical & Electronic Materials
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    • v.4 no.2
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    • pp.132-142
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    • 1991
  • 본 연구에서는 유기절연재료의 재방사선 재료개발을 위한다는 측면에서 두께 15[.mu.m]의 이축 연신 폴리프로필렌 필름을 시료로 선정하여 Co$^{60}$-.gamma.으로 조사시켜 온도 25-55[.deg.C], 전계 10-250[MV/m]사이에서 방사선 조사량 변화에 따른 전기전도현상을 연구하였다. 조사된 시료의 전기전도는 온도에 크게 의존하여 전계의 증가와 더불어 각기 다른 전도기구 특성을 갖는 4개의 영역으로 구분되었는데 각 영역별로 조사선량 변화에 따른 하전입자들의 거동상황을 규명하고 기초적인 제 물성정수를 결정하였다.

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Exposure Measurements of Co-60 Gamma rays (Co-60 감마선의 조사선량 측정)

  • Hah, Suck-Ho;Kim, Hyun-Moon
    • Journal of Radiation Protection and Research
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    • v.16 no.2
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    • pp.7-16
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    • 1991
  • Measurement of Co-60 gamma rays has been made for establishment of exposure standard and analyze it's overall uncertainties. Exposure rate determined by the charge mode method using vibrating reed amplifier with cylinderical type cavity chamber. The values of a variety of physical constants and the correction factors are evaluated. The resulting exposure rate is 690.81 R/h at the distance of 1m from the source and the related uncertainties is ${\pm}0.8%$

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Observation Systems of Cherenkov Radiation from Water Phantom Irradiated with Co-60 Gamma-rays

  • Tabushi, Katsuyoshi;Koyama, Shuji;Homma, Mitsuhiko;Tamiya, Tadashi;Yajima, Mihoko;Imai, Kuniharu;Obata, Yasunori
    • Proceedings of the Korean Society of Medical Physics Conference
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    • 2002.09a
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    • pp.123-125
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    • 2002
  • Blue light of Cherenkov radiation generated by electrons in transparent substances such as water and acrylic resin is well known generally. If students can easily observe the blue light at school, they may be impressed by the fascinating radiation. Four years ago, management of the Co-60 unit for radiotherapy was transferred to Nagoya University School of Health Sciences from a related hospital. We have examined whether or not the Cherenkov radiation in water from secondary electrons generated by Co-60 gamma-rays can be safely observed by eyes and photographs. First, the Cherenkov radiation in the water tank was led to the corridor outside the irradiation room by a mirror, and observed directly without any effect of the radiation exposure. Second, photographs of the Cherenkov radiation were taken under the conditions consisted of several irradiation fields and pass lengths of gamma-rays in water.

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Synthesis of PVA/PVP Hydrogel by Irradiation Crosslinking (방사선 가교에 의한 PVA/PVP 하이드로겔 제조 및 드레싱에의 응용)

  • 김태훈;노영창
    • Polymer(Korea)
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    • v.25 no.2
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    • pp.270-278
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    • 2001
  • Hydrogels for wound dressing were manufactured using poly(vinylalcohol)(PVA) and poly(N-vinylpyrrolidone)(PVP). The hydrogels were obtained by exposing to $^{60}$ Co${\gamma}$-rays after freezing and thawing of aqueous solutions of PVA and PVP to improve mechanical strength. Mechanical properties such as gelation, water absorptivity and gel strength were examined after repeating the \"freezing and thawing\" of PVA/PVP hydrogels, and then irradiating them at 40 kGy. The PVA/PVP ratio was in the range of 30:70 ~ 100:0, and the solid concentration of PVA/PVP was 20 wt%. The gelation and strength of hydrogels were much higher when \"freezing and thawing\" and the irradiation process were used than when only the irradiation process was utilized. In addition, the mechanical properties of PVA/PVP hydrogels after repetition of \"freezing and thawing\" are discussed. thawing\" are discussed.ssed.

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Plastic scintillator beta ray scanner for in-situ discrimination of beta ray and gamma ray radioactivity in soil

  • Bae, Jun Woo;Kim, Hee Reyoung
    • Nuclear Engineering and Technology
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    • v.52 no.6
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    • pp.1259-1265
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    • 2020
  • A beta ray scanner was proposed for in-situ discrimination of beta and gamma ray radioactivity. This scanner is based on the principle that gamma and beta rays experience different changes in detection efficiency in scintillators with different geometries, especially with regard to the scintillator thickness. The ratios of the counting rates of gamma rays (Rgamma), beta rays (Rbeta), and sample measurements (Rtotal) in a thick scintillator to those in a thin one are reported. The parameter Xthick, which represents the counting rate contributed by beta rays to the total counting rate in the thick scintillator, was derived as a function of those ratios. The values of Rgamma and Rbeta for 60Co and 90Sr sources were estimated as 3.2 ± 0.057 and 0.99 ± 0.0049, respectively. The estimated beta ray contributions had relative standard deviations of 2.05-4.96%. The estimated range of the beta rays emitted from 90Sr was 19 mm as per the Monte Carlo N-Particle simulation, and this value was experimentally verified. Homogeneous and surface contaminations of 60Co and 90Sr-90Y were simulated for application of the proposed method. The counting rate contributed by the beta rays was derived and found to be proportional to the concentration of 90Sr-90Y contamination.

Comparison of Skin Injury Induced by β- and γ-irradiation in the Minipig Model

  • Kim, Joong-Sun;Jang, Hyosun;Bae, Min-Ji;Shim, Sehwan;Jang, Won-Seok;Lee, Sun-Joo;Park, Sunhoo;Lee, Seung-Sook
    • Journal of Radiation Protection and Research
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    • v.42 no.4
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    • pp.189-196
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    • 2017
  • Background: The effects of radiation on tissues vary depending on the radiation type. In this study, a minipig model was used to compare the effects of ${\beta}$-rays from $^{166}Ho$ and ${\gamma}$-rays from $^{60}Co$ on the skin. Materials and Methods: In this study, the detrimental effects of ${\beta}$- and ${\gamma}$-irradiation on the skin were assessed in minipigs. The histopathological changes in the skin from 1 to 12 weeks after exposure to 50 Gy of either ${\beta}$- (using $^{166}Ho$ patches) or ${\gamma}$- (using $^{60}Co$) irradiation were assessed. Results and Discussion: The skin irradiated by ${\beta}$-rays was shown to exhibit more severe skin injury than that irradiated by ${\gamma}$-rays at 1-3 weeks post-exposure; however, while the skin lesions caused by ${\beta}$-rays recovered after 8 weeks, the ${\gamma}$-irradiated skin lesions were not repaired after this time. The observed histopathological changes corresponded with gross appearance scores. Seven days post-irradiation, apoptotic cells in the basal layer were detected more frequently in ${\beta}$-irradiated skin than in ${\gamma}$-irradiated skin. The basal cell density and skin thickness gradually decreased until 4 weeks after ${\gamma}$- and ${\beta}$- irradiation. In ${\beta}$-irradiated skin lesions, and the density and thickness increased sharply back to control levels by 6-9 weeks. However, this was not the case in ${\gamma}$-irradiated skin lesions. In ${\gamma}$-irradiated skin, cyclooxygenase-2 (COX-2) was shown to be expressed in the epidermis, endothelial cells of vessels, and fibroblasts, while ${\beta}$-irradiated lesions exhibited COX-2 expression that was mostly limited to the epidermis. Conclusion: In this study, ${\beta}$-rays were shown to induce more severe skin injury than ${\gamma}$-rays; however, the ${\beta}$-rays-induced injury was largely repaired over time, while the ${\gamma}$-rays-induced injury was not repaired and instead progressed to necrosis. These findings reveal the differential effects of ${\gamma}$- and ${\beta}$-irradiation on skin and demonstrate the use of minipigs as a beneficial experimental model for studying irradiation-induced skin damage.