• 유체기계공업학회:학술대회논문집
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• 유체기계공업학회 2001년도 유체기계 연구개발 발표회 논문집
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• pp.197-202
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• 2001

The heat produced by the fission in the fuel of HANARO, 30 MW of research reactor, was transferred from the primary cooling water to the secondary cooling water through heat exchangers. The secondary cooling water absorbed the heat was circulated by secondary cooling pumps and cooled through 33 MW of cooling tower. Each capacity of the three secondary cooling pumps was fifty percent ($50\%$) of full load. The two pumps were normally operated and the other pump was standby. One of the secondary cooling pumps has often get troubles by high vibration. To release these troubles the pump shaft has been re-aligned, the pump bearing has been replaced with new one, the shaft sleeve has been replaced with new one, the shaft and the impeller have been re-weight balanced representatively or the vibration of motor has been tested by disconnecting the shaft of pump. But the high vibration of pump cannot be cleared. We find out the weight balance trouble of the assembly that the impeller is installed in the shaft. After clearing the trouble, the high vibration is released and the pump is operated with smooth. In this paper the trouble solution of secondary cooling pump is described including the reason of high vibration.

• 한국에너지공학회:학술대회논문집
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• 한국에너지공학회 1998년도 추계 학술발표회 논문집
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• pp.180-192
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• 1998

One of the conventional gas burners has nowadays been used for ladle preheating. As a ladle is one of the open-type furnaces, however, it causes to consume much fuel because of high temperature of exhaust gas from the ladle and the exhaust gas passing through ladle cover makes it worsen a working environment nearby. Therefore, the objective of this study is to develop the recuperative burner system applying for an existing teeming ladle , which is integrated with burner, recuperator and eductor as one of the new type combustion equipments and has many advantages of simple installation, compactness and easy control, especially a great deal of energy saving through the waste heat recovery from exhaust gas. The contents of the study is to design, manufacture of recuperative burner system and to perform its tests experimentally after applying to the teeming ladle in the capacity of 100 ton. Its heat release rate is 1,700,000 kcal/h with COG(Cokes Oven Gas) as fuel gas. The test items are the temperature distribution inside the ladle and the preheated air temperature change depending upon the exhaust gas. Nox, exhaust gas analysis and noise.

• 대한기계학회논문집B
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• 제25권5호
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• pp.653-659
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• 2001

This paper is concerned with the development of a new method for making and separating ice in-water and saving floated ice by installing an evaporation panel in an ice storage tank. The new method shows very good heat transfer efficiency than that of the convectional method. It is because the evaporation panel is directly contacted with water in the storage tank. The experiments were performed by varying inlet and outlet refrigerant temperatures of its evaporator. From the experimental results, the operating characteristics of in-water harvest-type ice storage system were investigated by measuring temperature and pressure at each point of the ice storage system and power required to operating compressor respect to the changes of the inlet and outlet refrigerant temperature of evaporator. It can be think that defrost frequency decreased and heavy ice created as the refrigerant temperature of evaporator outlet and defrost setting temperature is low so gotten result can effect to release efficiency. Also, consumption power, condensing heat quantity, refrigerating capacity and performance efficiency decreased as time goes by. Therefore, these results provide the basic data for system optimization, performance improvement and the possibility of application to other fields.

• 한국지반공학회논문집
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• 제33권10호
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• pp.25-31
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• 2017

완충재는 고준위폐기물을 처분하기 위한 공학적방벽 시스템에서 중요한 구성요소 중 하나이다. 완충재는 처분공내 사용후핵연료가 담긴 처분용기와 암반사이에 채워지는 물질로써 고준위폐기물의 안전한 처분을 위해 필수적인 요소라고 할 수 있다. 완충재는 지하수 유입으로부터 처분용기를 보호하고, 방사성 핵종 유출을 저지한다. 처분용기로부터 발생하는 고온의 열량은 완충재로 전파되기에 완충재의 열물성은 처분시스템의 안전성 평가에 매우 중요하다고 할 수 있다. 특히, 완충재의 설정온도는 고준위폐기물 처분시설의 설계에 큰 영향을 끼칠 수 있다. 따라서 본 연구에서는 온도변화에 따른 국내 경주산 압축 벤토나이트 완충재에 대한 열물성을 규명하고자 하였다. 열선법과 이중 탐침법을 이용하여 온도변화에 따른 압축 벤토나이트 완충재의 열전도도와 비열을 측정하였다. $22^{\circ}C$와 $110^{\circ}C$ 구간에서는 온도 증가에 따라 포화도가 변화되기에 열전도도와 비열은 급격하게 감소하는 경향을 보였으나 $110^{\circ}C$와 $150^{\circ}C$ 사이의 고온 구간에서는 열전도도와 비열의 추가 변화가 거의 발생하지 않았다.

• 한국화재소방학회:학술대회논문집
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• 한국화재소방학회 2011년도 추계학술논문발표회 논문집
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• pp.478-481
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• 2011

This study is intended to evaluate and optimize the characteristics of smoke spreading and the appropriateness of evacuation time extended by operation of smoke control system during fire within the underground space of the building structured in compliance with the smoke control system performance criteria from the local fire safety standard, which has been currently applied to the buildings in Korea. Using the heat release per unit weight of the combustibles, a numerical analysis both in case of smoke control system in operation and the system not in operation was carried out at the several different shopping malls. From the viewpoint of securing the evacuation time, the results were compared in an attempt to assess the appropriateness of the fire safety criteria.

• 한국가스학회지
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• 제7권1호
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• pp.19-23
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• 2003

최근 국내에서도 정량적 위험성 평가 기법을 위험시설물에 도입하여 위험도를 관리하면서 LPG 저장탱크에 대한 사고후 피해영향평가에 대한 연구는 다각적으로 이루어지고 있으나 BLEVE(Boiling Liquid Expanding Vapor Explosion, BLEVE)의 조건 및 메커니즘 규명에 대한 연구는 별로 이루어지고 있지 않다. 따라서, 본 고에서는 상대적으로 위험성이 큰 지상식 LPG 저장탱크의 BLEVE 가능성에 대해 외국의 Pilot 탱크 시험 결과 및 BLEVE 발생을 위한 소요입열량 계산값을 이용한 연역적 계산방법을 통해 BLEVE 조건 및 가능성을 정량화하여 규명코자 하였다. 또한, 산출된 탱크의 파열압력(burst pressure)과 충전량에 의해 보정된 액 온도를 사용해서 그려진 BLEVE map을 이용하여 BLEVE 조건에서 액위($\%$)가 BLEVE에 어떤 영향을 미칠 것인가를 규명하였다. 계산결과, 탱크 plate 온도가 $600^{\circ}C$이고, 탱크내부 액온도가 $53^{\circ}C$ 일 때 액충전량은 $43.68\%$ 이상일 경우에 BLEVE의 발생이 가능하다는 결과를 얻었다. 또한, 부천 대성에너지 LPG 충전소와 동일한 사양인 15톤 프로판 탱크를 모델로 하여 BLEVE가 발생하기 위한 외부 누출 및 외부화재 조건을 PHAST(Version 6.00) 및 EFFECTS(Version 2.1) 프로그램을 이용해 계산한 결과 액상 누출시 누출상당직경은 7.2mm, 이상 누출시 누출상당직경은 17.6mm 이상일 경우에 BLEVE가 발생 가능한 최소한의 풀화재 생성조건이 되었고, 풀화재의 크기는 최소 직경 3.3m, 높이 10.4m 이상의 풀화재가 전제되어야 한다는 결과를 얻을 수 있었다.

• 한국안전학회지
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• 제30권4호
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• pp.64-72
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• 2015

The purpose of this study is to study the safety of a small LPG storage tank with a capacity less than 3 ton when it is exposed to an external fire. First, simulation studies were carried out using ASPEN Plus and PHAST to demonstrate that overpressurization in the tank can be relieved by discharging the LPG through an adequately sized safety valve, but the release may lead to the secondary risk of fire and explosion around the tank. Next, the temporal variations of the temperatures of the lading and tank wall were obtained using AFFTAC, which showed that the tank wall adjacent to the vapor space could be overheated in about 11 min to such a point that the weakened strength might cause a rupture of the tank and subsequent BLEVE. The consequences of the BLEVE were estimated using PHAST. Finally, several practical measures for preventing the hazards of overheating were suggested, including an anti-explosion device, sprinkling system, insulation, heat-proof coating, and enhanced safety factor for tank fabrication. The effectiveness of these measures were examined by simulations using AFFTAC and ASPEN Plus.

• 한국분무공학회지
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• 제3권1호
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• pp.19-26
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• 1998

The effect of mixture component makes a nelay time and a long total combustion period $\tau_{p\;max}$. The flame propagation delay $\tau_{df}$ was determined by the record of current ion. The pressure release delay $\tau_{dp}$ and $\tau_{p\;max}$ were determined by the indicated pressure diagram in constant volume of the combustion chamber. The results are as follows: 1) The ignition delay $\tau_t$ time takes the minimum value around $\Phi=1.15$. 2) $\tau_{df}$ and $\tau_t$ time increased according to the increases of the concentrated dilution gases, because the adiabatic flame temperature decreased due to the increases of the heat capacity. But dilution gases have little effect on flame nucleus formation delay 3) The relation between $\tau_t$ time and reciprocal laminar burning velocity is almost linear. 4) The increase of the propagation length is accompanied with increased ratio of the $\tau_{df},\;\tau_{dp},\;\tau_{t},\;\tau_{p\;max}$.

• 한국구조물진단유지관리공학회 논문집
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• 제23권1호
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• pp.1-8
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• 2019

스트론튬계 상전이물질은 특정한 온도에서 물질의 상태가 변함에 따라서 열을 흡수하거나 방출하게 된다. 본 연구의 목적은 스트론튬계 상전이물질의 혼입이 플라이애시 치환 모르타르 및 고로슬래그 치환 모르타르의 수화발열 및 역학적 특성에 미치는 영향을 실험적으로 평가하는 것이다. 스트론튬계 상전이물질의 혼입량은 결합재 질량의 1, 2, 3, 4, 5%로 하였다. 총 12개 수준의 모르타르 배합에 대해서 모르타르 흐름성능, 간이수화열온도상승, 압축 및 휨강도 실험을 각각 수행하였다. 실험결과 본 연구에서 사용한 스트론튬계 상전이물질은 모르타르의 수화열 저감 및 수화지연에 효과적인 것으로 판단된다. 특히 플라이애시 치환 모르타르의 최대온도 상승량은 고로슬래그 치환 모르타르의 최대온도 상승량에 비해 낮게 나타났다. 플라이애시 및 고로슬래그 치환 모르타르의 압축강도는 상전이물질 혼입량이 증가함에 따라 감소하는 것으로 나타났다.

• 터널과지하공간
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• 제8권2호
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• pp.107-117
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• 1998

In the case of a fire disaster in a uni-directional road tunnel, it is important to determine the critical ventilation velocity to prevent the backflow travelling toward the tunnel exit where vehicles are stopped. The critical ventilation velocity is horizontal velocity to prevent hot smoke from moving toward the tunnel exit. According to Froude modelling, the model tunnel whcih was 300mm in diameter and 21 m in length was made of acryl tubes. Inner section of acryl tubes was clothed with polycarbonate. 1/20 scaled model vehicles were installed to simulate the situation that vehicles are stopped in the tunnel exit. Methanol in a pool type burner was burned in the middle of tunnel to simulate a fire hazard. In this study, the basis of determining the critical ventilation velocity is the ventilation flow rate that is able to maintain the allowable CO concentration in the tunnel section. We assumed that the allowable CO concentration was backflow dispersion index. Futhermore, We intended to find out CO distribution and temperature distribution according as we changed ventilation velocity. The results of this study were that no backflow happened when ventilation velocity was 0.52 m/s in the case of 5.75 kW. If we adapt these results of a fire disaster releasing 10MW heat capacity in real tunnel which is 400m in length, no backflow happens when ventilation velocity is 2.31m/s. After we figured out dimensionless heat release rate and dimensionless ventilation velocity of model test and those of real test to verify experimental correctness, we tried to find out correlation between experimental results of model tunnel and those of real tunnel.