• Title/Summary/Keyword: C3 pre-cooled system

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Exergy Analysis and Optimization of Chiller System in Hydrogen Fueling Station Using R290 Refrigerant (R290 냉매를 이용한 수소 충전소 냉각시스템 엑서지 분석 및 공정 최적화)

  • HYEON, SOOBIN;CHOI, JUNGHO
    • Journal of Hydrogen and New Energy
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    • v.32 no.5
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    • pp.356-364
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    • 2021
  • During the hydrogen fueling process, hydrogen temperature inside the compressed tank were limited below 85℃ due to the allowable pressure of tank material. The chiller system to cool compressed hydrogen used R407C, greenhouse gas with a high global warming potential (GWP), as a refrigerant. To reduce greehouse gas emission, it should be replaced by refrigerant with a low GWP. This study proposes a chiller system for fueling hydrogen with R290, consisted in propane, by applying the C3 pre-cooled system use d in the LNG liquefaction process. The proposed system consisted of hydrogen compression and cooling sections and optimized the operating pressure through exergy analysis. It was also compared to the exergy efficiency with the existing system at the optimal operating pressure. The result showed that the optimal operating pressure is 700 kPa in 2-stage, 840 kPa/490 kPa in 3-stage, and the exergy efficiency increased by 17%.

Analysis of Pure Refrigerant Cycle Design on C3MR Process through Driver Selection (동력 공급 장치 선택을 통한 C3MR 공정의 순수냉매 사이클 설계 분석)

  • Lee, Inkyu;Tak, Kyungjae;Lim, Wonsub;Moon, Il;Kim, Haksung;Choi, Kwangho
    • Journal of the Korean Institute of Gas
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    • v.17 no.3
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    • pp.27-32
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    • 2013
  • Natural gas liquefaction process which is operated under cryogenic condition spends large amount of energy. Most of energy in the natural gas liquefaction process is consumed by compressors. Therefore, minimizing energy consumption of compressors is an important issue in process design and operation. Among various natural gas liquefaction processes, propane pre-cooled mixed refrigerant (C3MR) process consists of mixed refrigerant system and pure refrigerant system. In this study, to find the optimal design of pure refrigerant system, pure refrigerant cycle is simulated on different number of pressure levels and the necessary energy of each design is compared. After that, the driver selection model is applied to analyse each processes, which has different number of equipments, in terms of cost. As the result, the design using many equipments spends lower energy. Using this result, this study suggests standard of process design selection by the cost term.

The Magnetic Characteristics and Microstructure of Mn-A1 System Alloys(1st Report) -Focused on the Mn-A1 Alloys- (Mn-Al계 합금의 열처리에 따른 미세조직 변화와 지기적 특성(제1보) -Mn-Al-Cu 합금을 중심으로-)

  • Pang, Man-Gyu;Yang, Hyun-Soo;Kwak, Chang-Sup
    • Journal of the Korean Society for Precision Engineering
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    • v.5 no.4
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    • pp.48-58
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    • 1988
  • This study was undertaken to observe the formation behavior of ferro- magnetic phase in Mn-Al-Cu Alloys. The alloy selected for this investigation was 70% Mn-29% Al-1% Cu. This pre-allyed pig was prepared to the cylinderical castings using an Induction furnace after homogenizing at $1100^{\circ}C$ for 2hr, the specimens were cooled by cooling methods. Subwequent isothermal heat treatments were followed at $550^{\circ}C$ for various periods of time at predetermined(1-1000min). The formation behavior of ferromagnetic phase was investigated by measurements of magnetic properties of the specimens at each stage of heat treatment, and optical microscopic esamination and X-Ray diffraction analyses were also employed. By this basic experimental results, the conclusions are as follows 1) In order to obtain much amount of ferromagnetic phase, the optimum average cooling rate was about 7.35-$16.4^{\circ}C$/sec($1100^{\circ}C$-$600^{\circ}C$). 2) We verified the decomposition of {\tau} phase to {\beta} -Mn and {\gamma} , as the specimens were homogenized at $1100^{\circ}C$ for 12hr, then heat-treased at $550^{\circ}C$ for 1-1000min. 3) A condition of optimum heat treatments in Mn-Al-Cu permanent mag-netic alloys showed that after homogenizing at $1100^{\circ}C$ for 2hr, the speciments were cooled in air or furnace(A) and subsequent heat treatments at $550^{\circ}C$ for 1-30min. The maximum magnetic properties were measured as follows: Air cooling; Br=1200(Gause), bHc=100(oe), (BH)max=0.07(MGOe) Furnace cooling(A);Br=950(Gauss), bhe=80(Oe), (BH)max=0.05(MGOe)

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