• Proceedings of the Korean Radioactive Waste Society Conference
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• 2006.06a
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• pp.251-252
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• 2006

원자력발전소는 기체폐기물의 90% 이상을 계획예방정비기간 중에 방출한다. 기체 폐기물 방출은 filter를 거치지 않고 대량 방출하는 고체적 방출과,filter를 거쳐 방출하는 저체적 방출이 있다. 고체적 방출은 방출농도계수가 5842, 저체적 방출은 계수가 183052로 이 이하로 방출만 하면 발전소제한구역(EPB Emergency Planning Zone)에서의 법적허용치 농도 ECL(environmental Control Limit)를 초과하지 않게 된다. 원전에서는 현재 기체방출 시 이 기준치(농도계수)의 1/10을 자체관리 기준치로 하여 적용하고 있다. 실제 울진3호기 4차O/H 시 그 실적을 파악해 본 결과 고체적 방출 시 방출농도계수가 최대 312, 저체적 방출 시는 최대 707을 넘지 않아 허용방출 농도계수와 비교하면 비교가 되지 않을 정도로 낮게 방출하였음을 확인하였다

• Proceedings of the Korean Society of Propulsion Engineers Conference
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• 2004.10a
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• pp.121-125
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• 2004

The effectiveness of the pogo suppression device (PSD) installed at the piping system simulating the fuel supply lines of the rocket engines was investigated. The system response defined as the ratio of the flow rate to the pressure in the main tube was obtained for various PSD gas volumes $(0,\;0.5,\;1,\;2\times10^{-6}\;m^3)$. Existence of a gas volume in the PSD reduced the system resonance frequency. With a larger gas volume, the resonance frequency became lower, but only slightly, though the fluctuations of the main tube pressure and the flow rate damped down considerably

• Journal of the Korean Society of Propulsion Engineers
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• v.9 no.2
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• pp.32-39
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• 2005

The effectiveness of the pogo suppression device (PSD) on the response of the piping system simulating the fuel (or oxidizer) supply lines of the rocket engines was investigated. The system response defined as the ratio of the flow rate to the pressure in the main tube was obtained for various PSD gas volumes $((0\~2)\times10^{-3}m^3)$ and three different baffle hole diameters (5, 50, 115mm). Existence of a gas volume in the PSD reduced the system resonance frequency. With a larger gas volume, the resonance frequency became lower, but only slightly, while the fluctuations of the main tube pressure and the flow rate damped down considerably. The resonance frequency decreased with the increase of the PSD inlet restriction (or the decrease of the baffle hole diameter), though slightly. However, with a larger inlet restriction, the PSD pressure wave showed a delayed response with the smaller amplitude compared to the pressure variation in the main tube.

• Journal of the Korean Vacuum Society
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• v.15 no.5
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• pp.465-474
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• 2006

A gas fueling system composed of a gas reservoir, an on-off valve, and a gas transferring tube, which is the simplest construction for the pre-programmed gas puffing, was simulated by numerically solving the time-dependent one-dimensional gas flow equation. The purpose of the simulation is to establish the relationship between the gas flow pattern (the elapsed time to the maximum flow, the maximum flow rate, the gas pulse duration) and the system parameters (the filling pressure and the volume of the gas reservoir, and the length and the diameter of the gas transferring tube).

• Transactions of the Korean Society of Mechanical Engineers A
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• v.39 no.4
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• pp.429-435
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• 2015

A bellows is an important temperature control component in a Joule-Thomson micro-cryocooler. It is designed using a very thin shell, and the inside of the bellows is filled with nitrogen gas. The bellows is made of a nickel-cobalt alloy that maintains its strength and elastic properties in a wide range of temperatures from cryogenic to $300^{\circ}C$. The pressure of the gas and the volume within the bellows vary according to the temperature of the gas. As a result, the bellows contracts or expands in the axial direction like a spring. To explore this phenomenon, the deformation of the bellows and its internal volume must be calculated iteratively under a modified pressure until the state equation of the gas is satisfied at a given temperature. In this paper, the modified Benedict-Webb-Rubin state equation is adopted to describe the temperature-volume-pressure relations of the gas. Experiments were performed to validate the proposed method. The results of a numerical analysis and the experiments showed good agreement.

• Proceedings of the Korean Nuclear Society Conference
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• 2002.10a
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• pp.110-110
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• 2002

• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.169-169
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• 2011

진공펌프의 성능을 나타내는 여러 파라미터가 있지만 가장 중요한 성능지표는 역시 배기속도라고 할 수 있다. 배기속도는 물리적으로 체적유량(volume flow rate, L/s 또는 m3/hr) 즉 단위시간당 펌프 흡기구에 들어오는 기체의 체적을 가리킨다. 펌프 흡기구 단면을 지나가는 체적을 직접 측정하는 것은 거의 불가능하므로 진공 전문가들은 흡기구로 들어가는 기체 유량(flow rate, mbar${\cdot}$L/s 또는 Pa${\cdot}$m3/s)과 흡기구 압력(mbar 또는 Pa)을 측정한 후 유량을 압력으로 나누어 주는 방식으로 배기속도를 측정한다. 유량은 표면 기체 방출을 고려하더라도 실용적인 측면에서 보면 위치에 상관없이 불변하는 값으로 볼 수 있어서 유량을 어떻게 정밀하게 잴 것인가 하는 방법만 있으면 편리한 위치에서 측정하면 된다. 반면에 압력을 정밀하게 측정하는 방식은 확립되어 있지만 막상 어디서 측정하는 것이 옳은가 하는 것은 의외로 쉽지 않다. 펌프의 배기속도를 측정하는 상황을 몇 가지로 가정해 보면, 규격에 입각한 표준용기에 달아 정식으로 재는 것, 게이지가 부착된 마구리판을 달고 간이로 재는 것, 펌프가 사용되고 있는 시스템 현장에서 재는 것이 있을 수 있고 펌프가 달려 있는 상태도 직접 용기에 달거나, 도관 또는 어댑터 및 밸브를 통해 달리는 경우가 있다. 앞에서 펌프 배기속도 계산 시 사용하는 흡기구 압력이란 엄밀히 말하면 흡기구를 바라보는 방향으로 가해지는 압력을 말하는데 이는 진공 게이지를 펌프 흡기구 면에서 상류를 향하도록 놓을 때 얻을 수 있는 값으로 막상 실행하는 것은 어렵다. 표준용기의 구조는 진공 게이지를 특정 위치에 달 때 마치 흡기구 면에 놓인 게이지처럼 흡기구 압력을 정확하게 측정할 수 있도록 고안된 것이지만 때에 따라서는 여러 변형된 측정 방식을 사용할 수밖에 없는 상황이 만들어지므로 어떤 보정을 거치면 올바른 배기속도 값을 구할 수 있는지 살펴볼 필요가 있다.

• KOREAN JOURNAL OF CROP SCIENCE
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• v.33 no.4
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• pp.353-359
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• 1988

Variations in photosynthetic capacities of leaves differing in thickness were explained on the basis of relationships between gas exchange and internal leaf structure. The relative importance of gas diffusion and of biochemical processes as limiting for leaf photosynthesis was also determined. Mesophyll cell surface was considered to be the limiting internal site for gas diffusion. and cell volume to be indicative of the sink capacity for CO$_2$ fixation. Increases in cell surface area were assumed to reduce proportionately mesophyll resistance to the liquid phase diffusion of CO$_2$. Increased cell volume was thought to account for a proportional increase in reaction rates for carboxylation, oxygenation. and dark respiration. This assumption was tested using chamber-grown Glycine max (L.) Merr. cv. Amsoy plants. Plants were grown under 200, 400, and 600 ${\mu}$mol photons m$\^$-2/ s$\^$-1/ of PAR to induce development of various leaf thickness. Photosynthetic CO$_2$ uptake rates were measured on the 3rd and 4th trifoliolate leaves under 1000 ${\mu}$mol photons m$\^$-2/ s$\^$-1/ of PAR and at the air temperature of 28 C. A pseudo -mechanistic photosynthesis model was modified to accommodate the concept of cell surface area as well as both cell volume and surface area. Both versions were used to simulate leaf photosynthesis. Computations based on volume and surface area showed slightly better agreement with experimental data than did those based on the surface area only. This implies that any single factor, whether it is photosynthetic model utilized in this study was suitable for relating leaf thickness to leaf productivity.

• Journal of Power System Engineering
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• v.12 no.1
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• pp.28-34
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• 2008

가스-액체 이젝터에 관한 수치해석은 3차원 CFD 모델로 수행하였다. 본 논문에서는 이젝터의 유동특성과 질량전달특성에 대한 작동조건과 이젝터의 기하학적 모형의 영향에 관한 연구를 수행하고자 한다. CFD 결과 실험 데이터에 의하여 검증되었으며, 유동 분석과 이젝터 성능의 예측 또한 실행되었다. 작동상태의 변화는 0.2 $\sim$ 1.2 범위에서 가스-액체 유량비를 변화시킴으로서 주어진다. 혼합관의 $L_M/D_M$이 4 $\sim$ 10의 범위에서 변화를 주었다. CFD 연구는 길이와 직경비가 5.5일 때 체적 유량전달계수는 가스 유량이 증가함에 따라 증가한다는 것을 나타낸다. 동시에 $L_M/D_M$가 4일 때 체적유량전달계수는 기체-액체 유량비가 0.6에서 최대치에 도달한다. 또한, 체적 유량전달계수는 혼합 튜브길이가 증가함에 따라 감소한다.

• Journal of the Korean Society of Propulsion Engineers
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• v.12 no.1
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• pp.16-22
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• 2008

The effect of two-phase spray injected into subsonic cross-flow was studied experimentally. External-mixing of two-phase spray from orifice nozzle with L/d of 3 was tested with various air-liquid ratio that ranges from 0 to 59.4%. Trajectory of spray and breakup phenomena were investigated by shadowgraph photography. Detailed spray structure was characterized in terms of SMD, droplet velocity, and volume flux using PDPA. Experimental results indicate that penetration length was increased and collision point of liquid jets approached to nozzle exit and distributions of mist-like spray were obtained by increasing air-liquid ratio.