• Nuclear Engineering and Technology
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• 제28권4호
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• pp.349-358
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• 1996

The leaching behavior of uranium from unirradiated CANDU UO$_2$ fuel pellet in the spent fuel wet storage and disposal conditions has been investigated. A modified IAEA leach test method was used, and then the extent of leaching was monitored by analysis for uranium in the leachant. The leach test has been performed in various leachants(demineralized water and boric acid solution at pH=6, synthetic granite groundwater) for a long-term period of 5.4 years, and the effect of temperature on the leach rate of uranium has been analyzed. The leach rates of uranium at $25^{\circ}C$ were dependent on the leachants. Over initial 100 days of leach periods, the leach rate in groundwater was the highest in three leachants and no significant differences of leach rates ore observed in the demineralized oater and boric acid solution. But these leach rates in three leachants around 2,000 days at $25^{\circ}C$ appeared to be reached the steady rates in the range of 1~5$\times$10$^{-8}$ g/$\textrm{cm}^2$ day. The leach rate of uranium in groundwater shooed to be independent of the temperature, but those in both demineralized water and boric acid solution increased with temperature. These results show that the leaching behavior of uranium from UO$_2$ fuel in both the demineralized water ann boric acid may be controlled tv the surface oxidative.dissolution reaction of UO$_2$ and the leach rate of uranium in groundwater at room temperature could mainly be controlled by the complex reaction of dissolved uranyl ions with carbonate ions and no variation of leach rate of UO$_2$ in groundwater with temperature may be due to the local deposition of passivating uranyl phases on the surface.

• Nuclear Engineering and Technology
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• 제35권1호
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• pp.55-63
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• 2003

Threshold porosity above which fission gas release channels would be formed in the rim egion of high burnup UO$_2$ fuel was estimated by the Monte Carlo method and Hoshen-Kopelman algorithm. With the assumption that both rim pore and rim grain can be represented by cube, pore distribution in the rim was simulated 3-dimensionally by the Monte Carlo method according to porosity and pore size distribution. Then, using the Hoshen-Kopelman algorithm, the fraction of open rim pores interlinked to the outer surface of a fuel pellet was derived as a function of rim porosity. The simulation showed that porosity of 24-25% is the threshold above which the number of rim pores forming release channels increases very rapidly. On the other hand, channels would not be formed if the porosity is less than about 23.5%. This is consistent with the observation that, for porosity less than 23.5%, almost no fission gas is released in the rim. However, once the rim porosity reaches beyond 25%, extensive open paths would be developed and considerable fission gas release would start in the rim.

• Nuclear Engineering and Technology
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• 제29권3호
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• pp.201-210
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• 1997

A thermal conductivity correlation has been proposed which can be applied to high turnup fuel by considering both of thermal conductivity with turnup across fuel pellet and additional degradation at pellet rim due to very high porosity. In addition, a correlation has been developed that can estimate the porosity of rim region as a function of rim burnup under the assumptions that all the produced fission gases are retained in the in porosity and threshold pellet average burnup required for the formation of rim region is 40 MWD/㎏U. Rim width is correlated to rim burnup using measured data. For the RISO experimental data obtained at pellet average turnup of 43.5 MWD/㎏U for three linear heat generation rates of 30, 35 and 40 ㎾/m, radial temperature distributions ore calculated using the present correlation and compared with the measured ones. This comparison shows that the present correlation gives the best agreement with the measured data when it is combined with the HALDEN's correlation for thermal conductivity considering its degradation with burnup. Another comparison with the HALDEN's measured fuel centerline temperature as a function of burnup at 25 ㎾/m up to about 44 MWD/㎾U also suggest that the present correlation yields the best agreement when it is combined with the HALDEN's thermal conductivity.

• 한국원자력학회:학술대회논문집
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• 한국원자력학회 2005년도 춘계학술발표회
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• pp.369-370
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• 2005

• 방사성폐기물학회지
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• 제4권3호
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• pp.255-263
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• 2006

$UO_2$ 펠릿 20 kg HM/batch용 분말화 장치는 차세대관리 공정의 금속전환로 안으로 균질화된 분말을 공급하기 위하여 $UO_2$ 펠릿을 산화하여 $U_3O_8$으로 분말화하는 장치이다. 본 연구에는 $UO_2$ 펠릿 20 kg HM/batch용 분말화 장치 설계모델을 제시하고, 실증용 분말화 장치를 제작하여 검증실험을 수행한다. 분말화 장치 설계모델은 내부구조, 성능, 가열로 위치와 크기 등이 고려된다. 실험 방법은 $UO_2$ 펠릿 20 kg HM/batch용 분말화 장치 설계 모델에 따라 기존의 3단 메시 분말화 장치를 이용하여 분말의 메시 투과시험과 온도변화 특성 실험을 하여 장치 내부구조를 결정한다. $UO_2$ 펠릿 20 kg HM/batch의 산화 반응도 실험과 가열로 위치별 온도 분포를 측정하고 장치의 성능과 가열로의 영 역 위치를 결정한다. 장치 크기를 결정하기 위하여 산화전의 20kg의 $UO_2$ 펠릿과 산화후의 $U_3O_8$ 부피를 측정한다. 이상의 결과를 토대로 실증용 분말화 장치를 설계. 제작하고, 검증을 위하여 산화도, 분말특성 및 분석 등을 수행하였다. 산화반응 실험결과 에서 기존장치에 비하여 분말의 메시 투과율이 향상되었으며, 기존의 3단 메시 장치의 $UO_2$ 펠릿산화시간이 13시간 소요된 것에 비하여 8시간으로 단축되었다. $U_3O_8$ 분말 특성 분석결과, 평균 입도가 $40{\mu}m$이었다. 제작된 $UO_2$ 펠릿 20 kg HM/batch용 분말화 장치 성능과 설계모델 예측 값은 대체로 잘 일치되었다.

• 한국재료학회지
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• 제8권9호
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• pp.783-790
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• 1998

용융점 및 물리.화학적 특성이 $\textrm{UO}_{2}$와 비슷한 yttria-stabilized-zirconia ($\textrm{ZrO}_{2}$-$\textrm{Y}_{2}\textrm{O}_{3}$)분말을 유도플라즈마(induction plasma)로 용융 침적시켜 원자력발전용 핵연료펠렛 제조공정에 응용하고자 하였다. 분말의 용융정도는 플라즈마동력 및 분말의 크기에 영향을 받는 것으로 나타났으며, 쉬스가스 조성, 분말분사관 위치, 입자크기 및 분사거리 등을 최적화 하여 Ar/$\textrm{H}_{2}$유량120/20$\ell$/min, 플리즈마 동력 80KW, 분사관의위치 8cm , 챔버압력 200Torr, 분사거리 18cm에서 이론밀도의 97.91%, 침적속도 20mm/min의 최적조건을 도출하였다. 침적시험에서 도출된 최적조건으로 펠렛몰더에서 제조한 펠렛은 96.5%의 밀도를 나타내었으며, 균일도 및 외곤도 우수하여 신기술에 의한 핵연료의 제조가능성을 확인하였다. 고밀도 침적에 영향을 미치는 각 변수들의 영향과 이들 변수들의 상호영향은 ANOVA(Analysis of Variance)을 이용하여 분석하였다.

• Nuclear Engineering and Technology
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• 제41권4호
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• pp.493-520
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• 2009

During the last four decades, 16 Pressurized Water Reactors (PWR) and 4 Pressurized Heavy Water Reactors (PHWR) have been constructed and operated in Korea, and nuclear fuel technology has been developed to a self-reliant state. At first, the PWR fuel design and manufacturing technology was acquired through international cooperation with a foreign partner. Then, the PWR fuel R&D by Korea Atomic Energy Research Institute (KAERI) has improved fuel technology to a self-reliant state in terms of fuel elements, which includes a new cladding material, a large-grained $UO_2$ pellet, a high performance spacer grid, a fuel rod performance code, and fuel assembly test facility. The MOX fuel performance analysis code was developed and validated using the in-reactor test data. MOX fuel test rods were fabricated and their irradiation test was completed by an international program. At the same time, the PWR fuel development by Korea Nuclear Fuel (KNF) has produced new fuel assemblies such as PLUS7 and ACE7. During this process, the design and test technology of fuel assemblies was developed to a self-reliant state. The PHWR fuel manufacturing technology was developed and manufacturing facility was set up by KAERI, independently from the foreign technology. Then, the advanced PHWR fuel, CANFLEX(CANDU Flexible Fuelling), was developed, and an irradiation test was completed in a PHWR. The development of the CANFLEX fuel included a new design of fuel rods and bundles.. The nuclear fuel technology in Korea has been steadily developed in many national R&D programs, and this advanced fuel technology is expected to contribute to a worldwide nuclear renaissance that can create solutions to global warming.

• Nuclear Engineering and Technology
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• 제42권1호
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• pp.79-88
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• 2010

Spent $UO_2$ nuclear fuel discharged from a nuclear power plant (NPP) contains fission products, U, Pu, and other actinides. Due to neutron capture by $^{238}U$ in the rim region and a temperature gradient between the center and the rim of a fuel pellet, a considerable increase in the concentration of fission products, Pu, and other actinides are expected in the pellet periphery of high burnup fuel. The characterization of the radial profiles of the various isotopic concentrations is our main concern. For an analysis, spent nuclear fuels originating from the Yeonggwang-2 pressurized water reactor (PWR) were chosen as the test specimens. In this work, the distributions of some actinide isotopes were measured from center to rim of the spent fuel specimens by a radiation shielded laser ablation inductively coupled plasma mass spectrometer (LA-ICP-MS) system. Sampling was performed along the diameter of the specimen by reducing the sampling intervals from 500 ${\mu}m$ in the center to 100 ${\mu}m$ in the pellet periphery region. It was observed that the isotopic concentration ratios for minor actinides in the center of the specimen remain almost constant and increase near the pellet periphery due to the rim effect apart from the $^{236}U$ to $^{235}U$ ratio, which remains approximately constant. In addition, the distributions of local burnup were derived from the measured isotope ratios by applying the relationship between burnup and isotopic ratio for plutonium and minor actinides calculated by the ORIGEN2 code.

• Nuclear Engineering and Technology
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• 제26권3호
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• pp.374-380
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• 1994

결정립계에 존재하는 핵분열기체의 기포가 소결체의 외부와 연결되는 정도를 모사할 수 있는 방법을 개발하였다. $UO_2$ 결정립의 형상을 TKD로 취급할 때, 결정립 Corner에서 자유 공간과 연결되는 핵분열 기체의 기포 비율을 결정립 Corner에 형성된 기포 반경의 함수로서 몬테 카를로 방법을 이용하여 계산하였다. 2차원적인 분석에도 불구하고, 본 방법은 모든 기포가 자유 공간과 완전히 연결된 순간에서 예측된 핵연료 팽윤과 측정된 핵연료 팽윤이 비교적 잘 일치함을 보였다. 그러나 핵분열기체 기포가 외부와 상호 연결된 정도를 좀 더 사실적으로 모사하려면 결정립 Corner의 기포를 3차원적으로 취급해야 한다.

• Nuclear Engineering and Technology
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• 제41권2호
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• pp.187-198
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• 2009

In this paper, three power ramp tests performed on high burn-up Re-crystallized Zircaloy2 - UO2 BWR fuel rods (56 to 63 MWd/kgU) within the SCIP project are simulated with METEOR and ALCYONE 3D. Two of the ramp tests are of staircase type up to Linear Heat Rates of 420 and 520 W/cm and with long holding periods. Failure of the 420 W/cm fuel rod was observed after 40 minutes. The third ramp test consisted of a more standard ramp test with a constant power rate of 80 W/cm/min up to 410 W/cm with a short holding time. The tests were first simulated with the METEOR 1D fuel rod code, which gave accurate results in terms of profilometry and fission gas releases. The behaviour of a fuel pellet fragment and of the cladding piece on top of it was then investigated with ALCYONE 3D. The size and the main characteristics of the ridges after base irradiation and power ramp testing were recovered. Finally, the failure criteria validated for PWR conditions and fuel rods with low-to-medium burn-ups were used to analyze the failure probability of the KKL rodlets during ramp testing.