288 research outputs found

    Reflection on Recent Research Progresses of CFD Computational Methodologies

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    ๋ณธ ์—ฐ๊ตฌ๋Š” ํ•ญ๊ณต์‹ ๊ธฐ์ˆ ์—ฐ๊ตฌ์†Œ์™€ ๊ต์œก๊ณผํ•™๊ธฐ์ˆ ๋ถ€์˜ NSL(National Space Lab.) ํ”„๋กœ๊ทธ๋žจ(NRF-2014M1A3 A3A02034856)์˜ ์ง€์›์„ ๋ฐ›์•„ ์ด๋ฃจ์–ด์กŒ์œผ๋ฉฐ, ๋˜ํ•œ KISTI ์Šˆํผ์ปดํ“จํ„ฐ ์„ผํ„ฐ(KSC-2015-C3-052)์˜ ์ง€์›์„ ๋ฐ›์•„ ์ด๋ฃจ์–ด์กŒ์Šต๋‹ˆ๋‹คOAIID:RECH_ACHV_DSTSH_NO:A201702756RECH_ACHV_FG:RR00200003ADJUST_YN:EMP_ID:A001138CITE_RATE:FILENAME:TD1-2.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:FILEURL:https://srnd.snu.ac.kr/eXrepEIR/fws/file/7af6ca5e-cd97-4a4e-b99d-55259ce0039a/linkCONFIRM:

    Effects of Numerical Flux, Limiter and Grid Density on the Aerodynamic Analysis of 3-Dimensional Transonic Flight Vehicle

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    ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๋‚ ๊ฐœ์™€ ๋™์ฒด๊ฐ€ ๊ฒฐํ•ฉ๋œ ์ฒœ์Œ์† ๋น„ํ–‰์ฒด ์ฃผ๋ณ€์˜ ์œ ๋™์„ ์ „์‚ฐ์œ ์ฒด์—ญํ•™(CFD)์„ ์ด์šฉํ•˜์—ฌ ์ˆ˜์น˜์ ์œผ๋กœ ํ•ด์„ํ•œ ๋‚ด์šฉ์„ ๋‹ค๋ฃจ๊ณ  ์žˆ๋‹ค. ์ฒœ์Œ์†์œผ๋กœ ๋น„ํ–‰ํ•˜๋Š” ๋น„ํ–‰์ฒด์˜ ์ฃผ๋ณ€์—๋Š” ์ถฉ๊ฒฉํŒŒ๊ฐ€ ๋ฐœ์ƒํ•  ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์—, ์ถฉ๊ฒฉํŒŒ๊ฐ€ ์กด์žฌํ•˜๋Š” ์œ ๋™์„ ์ •ํ™•ํ•˜๊ฒŒ ํ•ด์„ํ•  ์ˆ˜ ์žˆ๋Š” ์ˆ˜์น˜๊ธฐ๋ฒ•์„ ์ ์šฉํ•˜๊ณ , ์‚ฌ์šฉ๋œ ์ˆ˜์น˜๊ธฐ๋ฒ•์˜ ์ •ํ™•๋„๋ฅผ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•œ ๋‹ค์ฐจ์› ๊ณต๊ฐ„ ์ œํ•œ ๊ธฐ๋ฒ•(MLP) ๋“ฑ์„ ์ ์šฉํ•˜์—ฌ ์ •๋ฐ€ํ•œ ๊ณ„์‚ฐ์„ ์ˆ˜ํ–‰ํ•˜๊ณ ์žํ•œ๋‹ค. ํ•ด์„๋œ ๊ฒฐ๊ณผ์™€ ์‹คํ—˜์น˜๋ฅผ ๋น„๊ตํ•จ์œผ๋กœ์จ ํ•ด์„์— ์‚ฌ์šฉ๋œ ์ฝ”๋“œ๋ฅผ ๊ฒ€์ฆํ•˜๊ณ , ๋‹ค์–‘ํ•œ ๊ธฐ๋ฒ•๋“ค์„ ์ ์šฉํ•˜์—ฌ ํ•ด์„ํ•œ ๊ฒฐ๊ณผ ๋ฐ ๊ฒฉ์ž ๋ฐ€๋„์— ๋”ฐ๋ฅธ ํ•ด์„ ๊ฒฐ๊ณผ๋“ค์„ ๋น„๊ตํ•ด ๋ด„์œผ๋กœ์จ ๊ฐ ๊ธฐ๋ฒ•๋“ค๊ณผ ๊ฒฉ์ž ๋ฐ€๋„๊ฐ€ ํ•ด์„ ๊ฒฐ๊ณผ์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ์•Œ์•„๋ณด๋„๋ก ํ•œ๋‹ค. ํ•ด์„๋œ ๊ฒฐ๊ณผ๋ฅผ ํ†ตํ•ด ๋น„ํ–‰์ฒด ์ฃผ๋ณ€ ์œ ๋™์˜ ๋ฌผ๋ฆฌ์  ํ˜„์ƒ์„ ๋ถ„์„ํ•˜๊ณ , ํŠนํžˆ ๋™์ฒด์™€ ๋‚ ๊ฐœ์˜ ๊ฒฐํ•ฉ๋ถ€๋‚˜ ๋น„ํ–‰์ฒด ํ›„๋ฉด์—์„œ ๋ฐœ์ƒํ•˜๋Š” ๋ณต์žกํ•œ ์œ ๋™์„ ์ค‘์ ์ ์œผ๋กœ ๋‹ค๋ฃจ๊ณ ์ž ํ•œ๋‹ค.This research deals with a numerical study on the flow around the transonic wing-body model by using Computational Fluid Dynamics(CFD). Because the shock may occur under the transonic flow, numerical schemes that can solve the flow with shock robustly are applied, and the Multi-dimensional Limiting Process(MLP) is also applied to enhance the accuracy of the numerical schemes used. The computational results are compared with the experimental data in order to validate the CFD code used in this research. The effect of each numerical scheme on the computational results is dealt with by comparing the numerical schemes used in this research. Grid refinement test is also conducted to show the effect of grid density on the results. The flow physics around the model is analysed through the results, especially at the wing-body junction and the base of the body.OAIID:RECH_ACHV_DSTSH_NO:420150000004648014RECH_ACHV_FG:RR00200003ADJUST_YN:EMP_ID:A001138CITE_RATE:FILENAME:์ˆ˜์น˜ํ”Œ๋Ÿญ์Šค__์ œํ•œ์ž_๋ฐ_๊ฒฉ์ž๋ฐ€๋„๊ฐ€_3์ฐจ์›_๋น„ํ–‰์ฒด_๊ณต๋ ฅํ•ด์„์—_๋ฏธ์น˜๋Š”_์˜ํ–ฅ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:FILEURL:https://srnd.snu.ac.kr/eXrepEIR/fws/file/b8226825-20c0-4482-a714-ca409bb00b52/linkCONFIRM:

    Development of Unsteady Preconditioned Multi-Phase Roem and Ausmpw+ Schemes

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    ๋ณธ ๋…ผ๋ฌธ์€ 2015๋…„๋„ ๋ฏธ๋ž˜์ฐฝ์กฐ๊ณผํ•™๋ถ€์˜ ์žฌ์›์œผ๋กœ NSL์‚ฌ์—…(NRF-2014M1A3A3A02034856)๊ณผ ๋ฏผใ†๊ตฐํ˜‘๋ ฅ ๊ธฐ์ˆ ์‚ฌ์—…(Civil-Military Technology Cooperation Program)์˜ ์ง€์›์„ ๋ฐ›์•„ ์ž‘์„ฑ๋˜์—ˆ์Šต๋‹ˆ๋‹ค.OAIID:RECH_ACHV_DSTSH_NO:420160000004648010RECH_ACHV_FG:RR00200003ADJUST_YN:EMP_ID:A001138CITE_RATE:FILENAME:๋น„์ •์ƒ_์˜ˆ์กฐ๊ฑดํ™”_๊ธฐ๋ฒ•์„_์ ์šฉํ•œ_๋‹ค์ƒ์œ ๋™_RoeMAUSMPW+_์ˆ˜์น˜๊ธฐ๋ฒ•ยทยท.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:FILEURL:https://srnd.snu.ac.kr/eXrepEIR/fws/file/696b8222-7074-43e7-8294-9499eb9c0b74/linkCONFIRM:

    Subcell Resolution์ด ๊ฐ€๋Šฅํ•œ ๊ณ ์ฐจ ์ •ํ™•๋„ ๋‹ค์ฐจ์› ๊ณต๊ฐ„ ์ œํ•œ ๊ธฐ๋ฒ•(hMLP) ์—ฐ๊ตฌ

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    OAIID:RECH_ACHV_DSTSH_NO:A201616786RECH_ACHV_FG:RR00200003ADJUST_YN:EMP_ID:A001138CITE_RATE:FILENAME:Subcell_Resolution์ด_๊ฐ€๋Šฅํ•œ_๊ณ ์ฐจ_์ •ํ™•๋„_๋‹ค์ฐจ์›_๊ณต๊ฐ„_ยทยท.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:FILEURL:https://srnd.snu.ac.kr/eXrepEIR/fws/file/45634a7f-7640-4833-9229-589efe1fa758/linkCONFIRM:

    Numerical Analysis of Unsteady Cavitating Flows around a 2-D Wedge for Natural and Ventilated Cavitation

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    OAIID:RECH_ACHV_DSTSH_NO:A201702755RECH_ACHV_FG:RR00200003ADJUST_YN:EMP_ID:A001138CITE_RATE:FILENAME:TC1-2.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:FILEURL:https://srnd.snu.ac.kr/eXrepEIR/fws/file/32a138da-77ea-428d-bd08-ee014e25de43/linkCONFIRM:

    Numerical Study of Supersonic Inlet Performance under Various Bleed Conditions

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    This paper deals with a numerical investigation of bleed effect on supersonic inlet performance under various bleed conditions. Because of high computational cost of direct simulation of each bleed holes, slaters 2009 bleed boundary condition model is used. Firstly, the bleed model is implemented and validated by solving validation cases. Then, a supersonic inlet used in Nagashimas experiments and bleeds are simulated to show the effect of bleed on performance of supersonic inlet. The kriging method in conjunction with a GA(Genetic Algorithm) is used to find the optimal condition of bleeds on the supersonic inlet, and EI(Expected Improvement) is introduced to enhance the kriging model. The optimal condition can be achieved when terminal shock is located in the throat of the supersonic inlet and an effect of flow separation is small.OAIID:oai:osos.snu.ac.kr:snu2014-01/104/0000004648/3SEQ:3PERF_CD:SNU2014-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:์šฐ์ฃผ๋ฐœ์‚ฌ์ฒด ์‹ฌํฌ์ง€์›€_๋…ผ๋ฌธ_์„œ์šธ๋Œ€ํ•™๊ต ์ตœ์š”ํ•œ_v 2.0.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€CONFIRM:

    Flow separation and nozzle side load simulations for TOP nozzle

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    OAIID:RECH_ACHV_DSTSH_NO:A201702754RECH_ACHV_FG:RR00200003ADJUST_YN:EMP_ID:A001138CITE_RATE:FILENAME:TC1-1.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:FILEURL:https://srnd.snu.ac.kr/eXrepEIR/fws/file/5fdd5d4c-5c7c-4442-a51e-5c6eab6c8e04/linkCONFIRM:

    Fluid-Structure-Combustion Interaction Simulation for Solid Propellant Rocket Interior Phenomena

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    ๊ณ ์ฒด ๋กœ์ผ“ ๋‚ด๋ถ€ ํ˜„์ƒ ์ „์‚ฐ ํ•ด์„์„ ์œ„ํ•ด ๊ธฐ์กด ์šด๋™ ๊ธฐ์ˆ  ๋ฐฉ๋ฒ•๋“ค์˜ ์žฅ์ ์„ ๊ฒฐํ•ฉํ•œ ALE ๊ธฐ๋ฒ•์„ ๋„์ž…ํ•˜์—ฌ ์œ ์ฒด ๊ตฌ์กฐ ์—ฐ๋™ ํ•ด์„์„ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ์ด๋ฅผ ์œ„ํ•ด ๊ฐœ๋ณ„ ํ•ด์„ ์š”์†Œ(์œ ๋™, ๊ตฌ์กฐ, ์—ฐ์†Œ)์™ธ์˜ ํ†ตํ•ฉ ๊ธฐ๋ฒ•๋“ค๊ณผ ๋ณ€ํ™”ํ•˜๋Š” ํ•ด์„ ์˜์—ญ์— ๋Œ€ํ•œ ์ž๋™ ๊ฒฉ์ž ์ƒ์„ฑ ๊ธฐ๋ฒ•์ด ์—ฐ๊ตฌ๋˜์—ˆ๋‹ค. ๊ฐœ๋ฐœ๋œ ํ•ด์„ ํ”„๋กœ๊ทธ๋žจ์„ ์ด์šฉํ•˜์—ฌ ๊ณ ์ฒด ์ถ”์ง„ ๋กœ์ผ“์˜ ์ ํ™”๊ณผ์ •๋ถ€ํ„ฐ ๋Œ€๋ถ€๋ถ„์˜ ์—ฐ๋ฃŒ๊ฐ€ ์†Œ์ง„๋˜๋Š” ์‹œ์ ๊นŒ์ง€์˜ ์ „์‚ฐ ํ•ด์„์ด ์ˆ˜ํ–‰๋˜์—ˆ์œผ๋ฉฐ ์ด๋ฅผ ํ†ตํ•˜์—ฌ ์—ฐ์†Œ์‹ค ๋‚ด๋ถ€์˜ ์œ ๋™ ๋ฌผ๋ฆฌ ํ˜„์ƒ๊ณผ ์ถ”์ง„์ œ ๊ทธ๋ ˆ์ธ์˜ ๋ณ€ํ˜• ํŠน์„ฑ์„ ๊ด€์ฐฐํ•˜์˜€๋‹ค.A fluid-structure interaction simulation of solid propellant rocket interior is carried out by employing the ALE (Arbitrary Lagrangian Eulerian) description, a hybrid model of continuum motion description combining the advantages of classical Lagrangian and Eulerian description. The integration process for fluid-structure interaction and an automatic re-meshing algorithm are included to analyze an unsteady fluid-structure interaction phenomenon with the deformation of solid grain during the simulation. The developed solver is applied for the full burning simulation of a solid propellant grain, which is a highly-coupled unsteady phenomenon between gas flow and propellant structure. Based on the integrated computed results, flow physics in the combustion chamber and the behavior of a solid propellant deformation are examined.๋ณธ ์—ฐ๊ตฌ๋Š” ๊ต์œก๊ณผํ•™๊ธฐ์ˆ ๋ถ€์˜ ์šฐ์ฃผ๊ธฐ์ดˆ์›์ฒœ๊ธฐ์ˆ  ๊ฐœ๋ฐœ ์‚ฌ์—…(NSL, National Space Lab, No. 2011- 0029871)๊ณผ ๊ตญํ† ํ•ด์–‘๋ถ€ ๊ฑด์„ค๊ธฐ์ˆ ํ˜์‹ ์‚ฌ์—… ์ดˆ์žฅ๋Œ€ ๊ต๋Ÿ‰์‚ฌ์—…๋‹จ(08 ๊ธฐ์ˆ ํ˜์‹  E01)์˜ ์ง€์›์„ ๋ฐ›์•„ ์ด๋ฃจ์–ด์กŒ์Œ.OAIID:oai:osos.snu.ac.kr:snu2012-01/104/0000004648/14SEQ:14PERF_CD:SNU2012-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:๊ณ ์ฒด_๋กœ์ผ“_์—ฐ์†Œ์‹ค_๋‚ด๋ถ€์—_๋Œ€ํ•œ_FScI_ํ•ด์„.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]:

    Multi-dimensional Limiting Process for Arbitrary Higher-order Discontinuous Galerkin Methods for High-fidelity Compressible Flow Analyses

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    ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์••์ถ•์„ฑ ์œ ๋™์žฅ์„ ์ •๋ฐ€ํ•˜๊ฒŒ ํ•ด์„ํ•˜๊ธฐ ์œ„ํ•ด์„œ ๋ถˆ์—ฐ์† ๊ฐค๋Ÿฌํ‚จ ๊ธฐ๋ฒ•์„ ์œ„ํ•œ ๊ฐ•๊ฑดํ•˜๊ณ  ํšจ์œจ์ ์ธ ๋‹ค์ฐจ์› ์ถฉ๊ฒฉํŒŒ ํฌ์ฐฉ ๊ธฐ๋ฒ•์„ ๊ฐœ๋ฐœํ•˜๊ณ ์ž ํ•œ๋‹ค. ๊ทธ๋™์•ˆ ๋ณธ ์—ฐ๊ตฌ ๊ทธ๋ฃน์—์„œ๋Š” ์œ ํ•œ ์ฒด์ ๋ฒ•์„ ๋ฐ”ํƒ•์œผ๋กœ ๋‹ค์ฐจ์› ๋ฌผ๋ฆฌ ์œ ๋™ ํŠน์„ฑ์„ ๋ฐ˜์˜ํ•œ ๋‹ค์ฐจ์› ๊ณต๊ฐ„ ์ œํ•œ ๊ธฐ๋ฒ•์„ ์„ฑ๊ณต์ ์œผ๋กœ ๊ฐœ๋ฐœํ•˜์˜€์œผ๋ฉฐ, ์ด๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ ๊ณ ์ฐจ ๋‚ด์‚ฝ์— ์šฉ์ดํ•œ ๋ถˆ์—ฐ์† ๊ฐค๋Ÿฌํ‚จ ๊ธฐ๋ฒ•์œผ๋กœ ํ™•์žฅํ•˜๊ณ ์ž ํ•œ๋‹ค. ์ด๋ฅผ ์œ„ํ•ด์„œ ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ธฐ์กด์— 2 ์ฐจ ์ •ํ™•๋„์˜ ์œ ํ•œ ์ฒด์ ๋ฒ•์—์„œ ์ œ์•ˆํ•œ MLP ๊ธฐ์šธ๊ธฐ ์ œํ•œ์ž์™€ ๋”๋ถˆ์–ด์„œ, ๊ณ ์ฐจ ๋‚ด์‚ฝ๊ธฐ๋ฒ•์— ์ ํ•ฉํ•œ MLP ๊ธฐ๋ฐ˜ Troubled-cell ํ‘œ์‹œ์ž๋ฅผ ์ถ”๊ฐ€์ ์œผ๋กœ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ์ด๋ฅผ ๊ฒฐํ•ฉํ•˜์—ฌ ๊ฐœ๋ฐœํ•œ DG-MLP ๊ธฐ๋ฒ•์˜ ๊ฒฝ์šฐ ์—ฐ์†์ ์ธ ๊ตฌ๊ฐ„์—์„œ ๋†’์€ ์ •ํ™•๋„๋ฅผ ์œ ์ง€ํ•˜๋ฉด์„œ๋„ ๋งค์šฐ ๊ฐ•๊ฑดํ•˜๊ณ  ์ •ํ™•ํ•˜๊ฒŒ ๋ฌผ๋ฆฌ์  ๋น„์„ ํ˜•ํŒŒ๋ฅผ ํฌ์ฐฉํ•จ์„ ํ™•์ธํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค.The present paper deals with the robust and efficient shock capturing strategy for arbitrary higher-order discontinuous Galerkin methods to resolve high speed compressible flow accurately. This approach is a continuous work of extending multi-dimensional limiting process (MLP), which has been successfully developed in finite volume method (FVM), into discontinuous Galerkin Method on unstructured grids. Based on successful analyses and implementations of the MLP slope limiting in FVM, MLP is extendable into DG framework with the MLP-based troubled-cell marker and the hierarchical MLP slope limiting. It is observed that the proposed approach yields outstanding performances in resolving non-compressive as well as compressive flow features.๋ณธ ์—ฐ๊ตฌ๋Š” 2011 ๋…„๋„ ์ •๋ถ€(๊ต์œก๊ณผํ•™๊ธฐ์ˆ ๋ถ€)์˜ ์žฌ์›์œผ๋กœ ๊ตญ๊ฐ€์ˆ˜๋ฆฌ๊ณผํ•™์—ฐ๊ตฌ์†Œ์˜ ์ฃผ์š”์‚ฌ์—… (No. A21001), ํ•œ๊ตญ์—ฐ๊ตฌ์žฌ๋‹จ์„ ํ†ตํ•ด ๊ต์œก๊ณผํ•™๊ธฐ์ˆ ๋ถ€์˜ ์šฐ์ฃผ๊ธฐ์ดˆ์›์ฒœ๊ธฐ์ˆ ๊ฐœ๋ฐœ ์‚ฌ์—…(NSL, National Space Lab, ๊ณผ์ œ๋ฒˆํ˜ธ 20100028975), ๊ตญํ† ํ•ด์–‘๋ถ€ ๊ฑด์„ค๊ธฐ ์ˆ ํ˜์‹ ์‚ฌ์—… ์ดˆ์žฅ๋Œ€๊ต๋Ÿ‰์‚ฌ์—…๋‹จ(08 ๊ธฐ์ˆ ํ˜์‹  E01) ์ง€์›์œผ๋กœ๋ถ€ํ„ฐ ์ง€์›๋ฐ›์•„ ์ˆ˜ํ–‰๋˜์—ˆ์ŒOAIID:oai:osos.snu.ac.kr:snu2011-01/104/0000004648/25SEQ:25PERF_CD:SNU2011-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:๊ณ ์ •๋ฐ€_์••์ถ•์„ฑ_์œ ๋™_ํ•ด์„์„_์œ„ํ•œ_์ž„์˜์˜_๊ณ ์ฐจ์ •ํ™•๋„๋ฅผ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]:

    The Slip-Wall Boundary Conditions Effects and the Entropy Characteristics of the Multi-Species GH Solver

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    Starting from the Eu"s GH(Generalized Hydrodynamic) theory, the multi-species GH numerical solver is developed in this research and its computatyional behaviors are examined for the hypersonic rarefied flow over an axisymmetric body. To improve the accuracy of the developed multi-species GH solver, various slip-wall boundary conditions are tested and the computed results are compared. Additionally, in order to validate the entropy characteristics of the GH equation, the entropy production and entropy generation rates of the GH equation are investigated in the 1-dimensional normal shock structure test at a high Knudsen number.๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๋‹คํ™”ํ•™์ข… ํฌ๋ฐ•์œ ๋™์˜ ํ•ด์„์„ ์œ„ํ•ด, GH(Generalized Hydrodynamic) ๋ฐฉ์ •์‹์„ ๊ธฐ๋ฐ˜์œผ๋กœ ํ•œ ์ถ•๋Œ€์นญ ์œ ๋™ ํ•ด์„์ด ๊ฐ€๋Šฅํ•œ ๋‹คํ™”ํ•™์ข… GH ์ˆ˜์น˜ํ•ด์„ ๊ธฐ๋ฒ•์„ ์ „์‚ฐ์œ ์ฒด์—ญํ•™ ์ˆ˜์น˜ํ•ด์„์ž๋กœ์„œ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ์ตœ์ดˆ๋กœ ๊ตฌํ˜„๋œ ๋‹คํ™”ํ•™์ข… GH ์ˆ˜์น˜๊ธฐ๋ฒ•์€ ์ถ•๋Œ€์นญ ํ˜•์ƒ์˜ ๋ฌผ์ฒด ์ฃผ์œ„์˜ ๊ทน์ดˆ์Œ์† ํฌ๋ฐ•์œ ๋™์„ ๋Œ€์ƒ์œผ๋กœ ํ•˜์—ฌ, DSMC(Direct Simulation Monte Carlo) ๋ฐ N-S(Navier-Stokes) ๋ฐฉ์ •์‹์˜ ๊ฒฐ๊ณผ์™€์˜ ๋น„๊ต๋ฅผ ํ†ตํ•ด ์ •ํ™•๋„๋ฅผ ๊ฒ€์ฆํ•˜๊ณ ์ž ํ•˜์˜€๋‹ค. GH ํ•ด์„์ž์˜ ์ •ํ™•๋„ ํ–ฅ์ƒ์„ ์œ„ํ•ด ๊ณ ์ฒด ๋ฒฝ๋ฉด์—์„œ์˜ ์—ฌ๋Ÿฌ ๊ฐ€์ง€ slip-wall ๊ฒฝ๊ณ„์กฐ๊ฑด์„ ์ ์šฉํ•˜๊ณ  ๊ฐ๊ฐ์˜ ๊ฒฐ๊ณผ๋ฅผ ๋น„๊ตํ•˜์˜€๋‹ค. ๋˜ํ•œ, ๋†’์€ Knudsen ์ˆ˜์˜ 1์ฐจ์› ์ˆ˜์ง ์ถฉ๊ฒฉํŒŒ ๊ตฌ์กฐ ๋ฌธ์ œ๋ฅผ ํ†ตํ•ด GH ๋ฐฉ์ •์‹์˜ ์—”ํŠธ๋กœํ”ผ ํŠน์„ฑ ๋ฐ ์ •ํ™•์„ฑ์„ ๊ณ ์ฐฐํ•˜์˜€๋‹ค.๋ณธ ์—ฐ๊ตฌ๋Š” ๋‘๋‡Œํ•œ๊ตญ 21์‚ฌ์—…๊ณผ ๊ต์œก๊ณผํ•™๊ธฐ์ˆ ๋ถ€ ์˜ ์šฐ์ฃผ๊ธฐ์ดˆ์›์ฒœ๊ธฐ์ˆ ๊ฐœ๋ฐœ ์‚ฌ์—…(NSL, National Space Lab)์˜ ์ง€์›์œผ๋กœ ์ˆ˜ํ–‰๋˜์—ˆ์Šต๋‹ˆ๋‹ค (S10801000121-08A0100-12110).OAIID:oai:osos.snu.ac.kr:snu2009-01/102/0000004648/9SEQ:9PERF_CD:SNU2009-01EVAL_ITEM_CD:102USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:๋‹คํ™”ํ•™์ข…_GH_๋ฐฉ์ •์‹์˜_์ •ํ™•์„ฑ_ํ–ฅ์ƒ์„_์œ„ํ•œ_๋ฒฝ๋ฉด_๊ฒฝ๊ณ„์กฐ๊ฑด_์—ฐ๊ตฌ_๋ฐ_GH_๋ฐฉ์ •์‹์˜_์—”ํŠธ๋กœํ”ผ_ํŠน์„ฑ_๊ณ ์ฐฐ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:NCONFIRM:
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