• Title/Summary/Keyword: 증기유량분포

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Analysis of Characteristics on Small Air Conditioning Type Condenser (소형 공조용 응축기의 특성 해석)

  • 김재돌;장재은;윤정인
    • Journal of Energy Engineering
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    • v.8 no.1
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    • pp.14-22
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    • 1999
  • 본 연구는 일반적으로 소·중용량의 냉동·공조기에 많이 사용되고 있는 플레이트 핀 코일형 공냉응축기를 대상으로 수치해석에 의해 응축기의 특성을 파악하였다. 해석에서는 응축기를 과열증기영역, 2상영역 및 과냉각액영역으로 구분하여 공냉 응축기의 성능에 큰 영향을 미치고 있는 공기온도, 공기측열전달률, 입구 냉매온도, 응축온도 및 질량유량 등을 파라메터로하여 이들의 상호관계와 이들이 응축완료점까지의 거리 및 방열량 등에 미치는 영향을 파악하였다. 해석결과로는 해석모델로부터 각 영역의 냉매 상태량, 온도분포 및 열전달률을 구할 수 있었고, 일반적으로 응축기의 성능에 많은 영향을 미치는 각종 파라메터들을 중심으로 광범위한 동작조건에서 이들의 상관관계 및 특성을 파악하므로서 응축기 설계를 위한 기초 자료 및 설치장소나 주위환경 등에 따라 서로간에 다양한 영향을 미치는 실제장치의 동적특성 해석을 위한 자료를 얻을 수 있었다.

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Pressure Distribution over Tube Surfaces of Tube Bundle Subjected to Two-Phase Cross-Flow (이상 유동에 놓인 관군의 표면에 작용하는 압력 분포)

  • Sim, Woo Gun
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.37 no.1
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    • pp.9-18
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    • 2013
  • Two-phase vapor-liquid flows exist in many shell and tube heat exchangers such as condensers, evaporators, and nuclear steam generators. To understand the fluid dynamic forces acting on a structure subjected to a two-phase flow, it is essential to obtain detailed information about the characteristics of a two-phase flow. The characteristics of a two-phase flow and the flow parameters were introduced, and then, an experiment was performed to evaluate the pressure loss in the tube bundles and the fluid-dynamic force acting on the cylinder owing to the pressure distribution. A two-phase flow was pre-mixed at the entrance of the test section, and the experiments were undertaken using a normal triangular array of cylinders subjected to a two-phase cross-flow. The pressure loss along the flow direction in the tube bundles was measured to calculate the two-phase friction multiplier, and the multiplier was compared with the analytical value. Furthermore, the circular distributions of the pressure on the cylinders were measured. Based on the distribution and the fundamental theory of two-phase flow, the effects of the void fraction and mass flux per unit area on the pressure coefficient and the drag coefficient were evaluated. The drag coefficient was calculated by integrating the measured pressure on the tube by a numerical method. It was found that for low mass fluxes, the measured two-phase friction multipliers agree well with the analytical results, and good agreement for the effect of the void fraction on the drag coefficients, as calculated by the measured pressure distributions, is shown qualitatively, as compared to the existing experimental results.

New Seat Design and Finite Element Analysis for Anti-Leakage of Globe Valve (글로브 밸브의 누설방지를 위한 시트 설계 및 유한요소해석)

  • Lee, Sung Ho;Kang, Gyeong Ah;Kwak, Jae-Seob;An, Ju Eun;Jin, Dong Hyun;Kim, Byung Tak
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.40 no.1
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    • pp.81-86
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    • 2016
  • The valves used to control or shut off the flow through a pipeline can be divided into many different types, including gate valves, globe valves, and check valves. Globe valves, in particular, have excellent properties, and because they can easily control the flow under high-pressure conditions, they are generally used in LNG ship and steam pipelines. In this paper, a method for changing the shape of a seat was suggested to solve the valve leakage problem from a structural perspective. In addition, the stress distribution and directional deformation were compared for each model. The suggested models were thus validated, and the optimized seat structure, which includes a self-supporting capability for decreasing the amount of leakage, was determined.

Fabrication and Charactreistics of MOCVD Cu Thin Films Using (hfac)Cu(VTMOS) ((hfac)Cu(VTMOS)를 이용한 Thermal CVD Cu 박막의 제조 및 그 특성)

  • 이현종;최시영
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.36D no.3
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    • pp.59-65
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    • 1999
  • In this paper, we had studied the possibility of application as Cu thin films from (hfac)Cu(VTMOS) which is very stable. Cu thin films had been studied as a function of deposition temperature. Substrates used in the experiment were PVD TiN on Si wafer. Deposition conditions were as follow : deposition temperature $50^{\circ}C$. Cu thin films were analyzed by AES, four point probe, XRD and SEM. All of deposited films were very pure and some favoring of <111> planes perpendicular to the substrate surface were observed. Cu thin films had two distinct growth rates at various deposition temperature. One is the surface reaction limited region below $200^{\circ}C$, and the other is the mass transport limited region above $200^{\circ}C$. The resistivity of deposited Cu thin films under the optimum deposition condition is $2.5mu\Omega.cm$ Thus, properties of deposited Cu thin films using (hfac)Cu(VTMOS) didn't show difference with Cu thin films from other precursors.

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Preparation of Asymmetric Membranes by Addition of Nonsolvent (비용매 첨가제를 이용한 비대칭막의 제조)

  • Kim, Nowon
    • Membrane Journal
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    • v.25 no.1
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    • pp.32-41
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    • 2015
  • High performance polysulfone microfiltration membranes with a high were successfully prepared by vapor induced phase separation (VIPS) coupled with non-solvent induced phase separation (NIPS) process. Asymmetric Membranes were prepared with PSF/DMF/PVP/PEG/DMSO/water mixed solutions and water/IPA coagulant. PSF, DMF, PVP, PEG, DMSO, water was used as a membrane polymer, a solvent, a hydrophilic polymer additive, a polar protic liquid polymer, a polar aprotic nonsolvent, and a polar protic nonsolvent in the casting solution, respectively. The addition of polar aprotic nonsolvents, and polar protic nonsolvents is a convenient and effective method to control membrane structure. In order to control the morphology of polymeric membranes, the spontaneous emulsification induced by drawing water vapor into the exposed casting solution surface has been used. Control of the internal morphology of polymeric membranes by using mixed coagulation solution such as water and IPA is discussed in the present work. The pure water permeability, pore size distribution, surface hydrophilicity and membrane morphology were investigated. Due to the addition of DMSO to casting solution, the mean pore size increased almost $0.2{\mu}m$ and the water flux increased about 1000-1800 LMH.

Comparison Of CATHARE2 And RELAP5/MOD3 Predictions On The BETHSY 6.2% TC Small-Break Loss-Of-Coolant Experiment (CATHARE2와 RELAP5/MOD3를 이용한 BETHSY 6.2 TC 소형 냉각재상실사고 실험결과의 해석)

  • Chung, Young-Jong;Jeong, Jae-Jun;Chang, Won-Pyo;Kim, Dong-Su
    • Nuclear Engineering and Technology
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    • v.26 no.1
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    • pp.126-139
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    • 1994
  • Best-estimate thermal-hydraulic codes, CATHARE2 V1.2 and RELAP5/MOD3, hate been assessed against the BETHSY 6.2 tc six-inch cold leg break loss-of-coolant accident (LOCA) test. Main objective is to analyze the overall capabilities of the two codes on physical phenomena of concern during the small break LOCA i.e. two-phase critical flow, depressurization, core water level de-pression, loop seal clearing, liquid holdup, etc. The calculation results show that the too codes predict well both in the occurrences and trends of major two-phase flow phenomena observed. Especially, the CATHARE2 calculations show better agreements with the experimental data. However, the two codes, in common, show some deviations in the predictions of loop seal clearing, collapsed core water level after the loop seal clearing, and accumulator injection behaviors. The discrepancies found from the comprision with the experimental data are larger in the RELAP5 results than in the CATHARE2. To analyze the deviations of the two code predictions in detail, several sensitivity calculations have been performed. In addition to the change of two-phase discharge coefficients for the break junction, fine nodalization and some corrections of the interphase drag term are made. For CATHARE2, the change of interphase drag force improves the mass distribution in the primary side. And the prediction of SG pressure is improved by the modification of boundary conditions. For RELAP5, any single input change doesn't improve the whole result and it is found that the interphase drag model has still large uncertainties.

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