15 research outputs found

    Numerical Study on Flow Characteristics of Synthetic Jet with Rectangular and Circular Slot Exit

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    ์‚ฌ๊ฐํ˜• ๋ฐ ์›ํ˜• ์ถœ๊ตฌ ํ˜•์ƒ synthetic jet์˜ ์ˆ˜์น˜์  ์—ฐ๊ตฌ๋ฅผ ํ†ตํ•˜์—ฌ ์œ ์ž…๋ฅ˜๊ฐ€ ์กด์žฌํ•  ๊ฒฝ์šฐ ํ‰ํŒ์—์„œ์˜ ์œ ๋™ ๊ตฌ์กฐ๋ฅผ ๋ถ„์„ํ•˜์˜€๋‹ค. ์‚ฌ๊ฐํ˜• ์ถœ๊ตฌ ํ˜•์ƒ์˜ ๊ฒฝ์šฐ, jet ์งํ›„์— ๊ฐ•ํ•œ vortex๊ฐ€ ์ƒ์„ฑ๋˜์ง€๋งŒ ์ฃผ๋ณ€์— ์ ์€ momentum์„ ๊ณต๊ธ‰ํ•˜๊ธฐ ๋•Œ๋ฌธ์— ์œ ์ž…๋ฅ˜ ๋ฐฉํ–ฅ์œผ๋กœ ๊ฐˆ์ˆ˜๋ก ์œ ๋™์ œ์–ด ํšจ๊ณผ๊ฐ€ ๊ธ‰๊ฒฉํ•˜๊ฒŒ ๊ฐ์†Œํ•˜๊ฒŒ ๋œ๋‹ค. ์›ํ˜•์ถœ๊ตฌ ํ˜•์ƒ์˜ ๊ฒฝ์šฐ, ๊ทœ์น™์ ์ธ vortex์˜ ํ˜•ํƒœ๊ฐ€ slot ์ค‘์•™๋ถ€ํ„ฐ ๋๊นŒ์ง€ ๋‚˜ํƒ€๋‚˜๊ณ  jet์— ์˜ํ•ด์„œ ๊ณต๊ธ‰๋˜๋Š” vortex์˜ ํ˜•ํƒœ๊ฐ€ ์œ ์ž…๋ฅ˜์˜ ๋ฐฉํ–ฅ์œผ๋กœ ๋ฐœ๋‹ฌ๋˜๊ฒŒ ๋˜์–ด ๋ณด๋‹ค ๋ฉ€๋ฆฌ๊นŒ์ง€ vorticity์˜ ์˜ํ–ฅ์ด ๋ฏธ์น˜๊ฒŒ ๋œ๋‹ค. ์œ ๋™์ œ์–ด ํšจ๊ณผ๋ฅผ ์˜ˆ์ƒํ•˜๊ธฐ ์œ„ํ•˜์—ฌ ์‚ฌ๊ฐํ˜• ๋ฐ ์›ํ˜• ์ถœ๊ตฌ ํ˜•์ƒ์˜ ์œ„์น˜ ๋ณ„ wall shear stress๋ฅผ ๋น„๊ตํ•˜์˜€๋‹ค. ๊ทธ ๊ฒฐ๊ณผ, ์›ํ˜• ์ถœ๊ตฌ ํ˜•์ƒ์ด ์‚ฌ๊ฐํ˜• ์ถœ๊ตฌ ํ˜•์ƒ๋ณด๋‹ค ์œ ๋™์ œ์–ด ํšจ๊ณผ๊ฐ€ ๋” ํด ๊ฒƒ์œผ๋กœ ์˜ˆ์ƒ๋œ๋‹ค.The flow characteristics of synthetic jet depending on rectangular and circular jet exit configuration are investigated using numerical computation with cross flow. In rectangular slot, synthetic jet generates the strong vortex, however, supply fewer momentum and effectiveness of flow control is reduced along flow direction. In circular slot, regular vortex is formed from slot center to end and developed in flow direction. It affects the wider region than rectangular slot. The distribution of wall shear stress is considered in order to indicate the effectiveness of flow control device for flow separation delay. As a result, circular slot is a more suitable candidate for delaying flow separation.๋ณธ ์—ฐ๊ตฌ๋Š” ๋ฐฉ์œ„์‚ฌ์—…์ฒญ๊ณผ ๊ตญ๋ฐฉ๊ณผํ•™์—ฐ๊ตฌ์†Œ์˜ ์ง€์›(UC100031JD), ์Šˆํผ์ปดํ“จํŒ…์„ผํ„ฐ(KSC-2010-C1-0030), ํ•ญ๊ณต ์šฐ์ฃผ ์‹ ๊ธฐ์ˆ  ์—ฐ๊ตฌ์†Œ์˜ ์ง€์›์œผ๋กœ ์ˆ˜ํ–‰๋˜์—ˆ์Œ.OAIID:oai:osos.snu.ac.kr:snu2011-01/104/0000004648/13SEQ:13PERF_CD:SNU2011-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:์‚ฌ๊ฐํ˜•_๋ฐ_์›ํ˜•_์ถœ๊ตฌ_Synthetic_Jet์˜_์œ ๋™_ํŠน์„ฑ์—_๋Œ€ํ•œ_์ˆ˜์น˜์ _์—ฐ๊ตฌ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]:

    Experimental Study on Flow Characteristics of Synthetic Jets with Circular Exit

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    ๋ณธ ์—ฐ๊ตฌ๋Š” ๊ต์œก๊ณผํ•™๊ธฐ์ˆ ๋ถ€ ํ•œ๊ตญ์—ฐ๊ตฌ์žฌ๋‹จ(No.20090084669), ๊ตญํ† ํ•ด์–‘๋ถ€๊ฑด์„ค๊ธฐ์ˆ ํ˜์‹ ์‚ฌ์—…('09 ๊ธฐ์ˆ ํ˜์‹  E02), ํ•ญ๊ณต์šฐ์ฃผ์‹ ๊ธฐ์ˆ ์—ฐ๊ตฌ์†Œ ๋ฐ BK21 ์‚ฌ์—…์˜ ์ง€์›์œผ๋กœ ์ˆ˜ํ–‰๋˜์—ˆ์Šต๋‹ˆ๋‹คOAIID:oai:osos.snu.ac.kr:snu2010-01/104/0000004648/36SEQ:36PERF_CD:SNU2010-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:์›ํ˜•_์ถœ๊ตฌ_Synthetic_Jet์˜_์œ ๋™_ํŠน์„ฑ_์—ฐ๊ตฌ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]:

    Flow Control of Smart UAV Airfoil Using Synthetic Jet Part 2 : Flow control in Transition Mode Using Synthetic Jet

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    In order to reduce the download around the Smart UAV(SUAV) at Transition mode, flow control using synthetic jet has been performed. Many of the complex tilt rotor flow features are captured including the leading and trailing edge separation, and the large region of separated flow beneath the wing. Based on the results of part 1 of the present work, synthetic jet is located at 0.01c, 0.95cflap and it is operated with the non-dimensional frequency of 0.5, 5 to control the leading edge and trailing edge separation. Consequently, download is substantially reduced compared to with no control case at transition mode using leading edge jet only. The present results show that the overall flight performance and stability of the SUAV can be remarkably improved by applying the active flow control strategy based on synthetic jet.์Šค๋งˆํŠธ ๋ฌด์ธ๊ธฐ ์ตํ˜• ์ฃผ์œ„์˜ ์œ ๋™ ๊ตฌ์กฐ๋ฅผ ํŒŒ์•…ํ•˜๊ณ  ์ด๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ synthetic jet์„ ์ด์šฉํ•˜์—ฌ ์ฒœ์ด ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ์˜ ์ˆ˜์ตํ•˜์ค‘ ๊ฐ์†Œ ์—ฌ๋ถ€๋ฅผ ํŒŒ์•…ํ•˜์˜€๋‹ค. ์Šค๋งˆํŠธ ๋ฌด์ธ๊ธฐ์˜ ์‹ค์ œ ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ์˜ ์œ ๋™ ๊ตฌ์กฐ๋ฅผ ๋ถ„์„ํ•˜์—ฌ ์•ž์ „ ๋ฐ ๋’ท์ „์—์„œ ๋ฐœ์ƒํ•˜๋Š” ์™€๋ฅ˜์— ์˜ํ•ด์„œ ์ˆ˜์ตํ•˜์ค‘์ด ํฌ๊ฒŒ ์ฆ๊ฐ€ํ•จ์„ ๋ฐํ˜”๋‹ค. ์ด์— ์•ž์ „๊ณผ ๋’ท์ „์—์„œ ๋ฐœ์ƒํ•˜๋Š” ์œ ๋™์˜ ๋ฐ•๋ฆฌ๋ฅผ ํšจ๊ณผ์ ์œผ๋กœ ์ œ์–ดํ•˜๊ธฐ ์œ„ํ•˜์—ฌ Part 1์˜ ๊ฒฐ๊ณผ๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ 0.01c, 0.95cflap ์ง€์ ์— jet์„ ์œ„์น˜์‹œํ‚ค๊ณ  ๊ฐ๊ฐ ๋ฌด์ฐจ์› ์ฃผํŒŒ์ˆ˜(F+)๋ฅผ 0.5, 5๋กœ ์ž‘๋™์‹œ์ผœ ๊ทธ์— ๋”ฐ๋ฅธ ์œ ๋™๊ตฌ์กฐ ๋ณ€ํ™”์™€ ํ•ญ๋ ฅ ๊ฐ์†Œ์œจ์„ ์•Œ์•„๋ณด์•˜๋‹ค. ๊ทธ ๊ฒฐ๊ณผ ์ฒœ์ด ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ์˜ ์œ ๋™ ์ œ์–ด๋ฅผ ์œ„ํ•ด์„œ๋Š” ์•ž์ „์— ์œ„์น˜ํ•œ jet๋งŒ์„ ์ž‘๋™์‹œํ‚ฌ ๊ฒฝ์šฐ ๊ฐ€์žฅ ํšจ๊ณผ์ ์œผ๋กœ ์ˆ˜์ตํ•˜์ค‘์„ ๊ฐ์†Œ์‹œํ‚ฌ ์ˆ˜ ์žˆ์Œ์„ ๋ฐํ˜”๋‹ค. ์ด์— ์ •์ง€ ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ์ฒœ์ด ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ synthetic jet์„ ์ด์šฉํ•˜์—ฌ ์œ ๋™์„ ์ œ์–ดํ•œ๋‹ค๋ฉด ์Šค๋งˆํŠธ์ „ ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ์˜ ๋น„ํ–‰์„ฑ๋Šฅ๊ณผ ์•ˆ์ •์„ฑ์„ ๋™์‹œ์— ํ–ฅ์ƒ์‹œํ‚ฌ ์ˆ˜ ์žˆ์„ ๊ฒƒ์ด๋‹ค.๋ณธ ์—ฐ๊ตฌ๋Š” ์ง€์‹๊ฒฝ์ œ๋ถ€ ์ง€์›์œผ๋กœ ์ˆ˜ํ–‰ํ•˜๋Š” 21์„ธ๊ธฐ ํ”„๋ก ํ‹ฐ์–ด ๊ธฐ์ˆ ๊ฐœ๋ฐœ์‚ฌ์—…(์Šค๋งˆํŠธ๋ฌด์ธ๊ธฐ๊ธฐ์ˆ ๊ฐœ๋ฐœ) ๋ฐ ๋ฐฉ์œ„์‚ฌ์—…์ฒญ๊ณผ ๊ตญ๋ฐฉ๊ณผํ•™์—ฐ๊ตฌ์†Œ์˜ ์ง€์› (๊ณ„์•ฝ๋ฒˆํ˜ธ UD0700 41AD)๊ณผ ํ•œ๊ตญ๊ณผํ•™๊ธฐ์ˆ ์ •๋ณด์—ฐ๊ตฌ์› ์Šˆํผ์ปดํ“จํŒ…์„ผํ„ฐ (KSC-2007- S00-1016), BK 21์‚ฌ์—…์˜ ์ง€์›์„ ํ†ตํ•ด ์ˆ˜ํ–‰๋˜์—ˆ์Šต๋‹ˆ๋‹ค.OAIID:oai:osos.snu.ac.kr:snu2009-01/102/0000004648/11SEQ:11PERF_CD:SNU2009-01EVAL_ITEM_CD:102USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:Synthetic jet์„ ์ด์šฉํ•œ ์Šค๋งˆํŠธ ๋ฌด์ธ๊ธฐ(SUAV) ์œ ๋™์ œ์–ด Part 2.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:NCONFIRM:

    Flow Control of Smart UAV Airfoil Using Synthetic Jet Part 1 : Flow control in Hovering Mode Using Synthetic Jet

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    In order to reduce the download around the Smart UAV(SUAV) at hovering, flow control using synthetic jet has been performed. Many of the complex tilt rotor flow features are captured including the leading and trailing edge separation, and the large region of separated flow beneath the wing. In order to control the leading edge andtrailing edge separation, synthetic jet is located at 0.01c, 0.3cflap, 0.95cflap. As non-dimensional frequency, the flow pattern is altered and the rate of drag reduction is changed. The results show that synthetic jets shorten the vortex period and decrease the vortex size by changing local flow structure. By using leading edge jet and trailing edge jet, download is efficiently reduced compared to no control case at hovering mode.์Šค๋งˆํŠธ ๋ฌด์ธ๊ธฐ ์ตํ˜• ์ฃผ์œ„์˜ ์œ ๋™ ๊ตฌ์กฐ๋ฅผ ํŒŒ์•…ํ•˜๊ณ  ์ด๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ synthetic jet์„ ์ด์šฉํ•˜์—ฌ ์ •์ง€ ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ์˜ ์ˆ˜์ตํ•˜์ค‘ ๊ฐ์†Œ ์—ฌ๋ถ€๋ฅผ ํŒŒ์•…ํ•˜์˜€๋‹ค. ์Šค๋งˆํŠธ ๋ฌด์ธ๊ธฐ์˜ ์‹ค์ œ ๋น„ํ–‰ ๋ชจ๋“œ์— ๋Œ€ํ•˜์—ฌ ์œ ๋™ ๊ตฌ์กฐ๋ฅผ ๋ถ„์„ํ•˜์—ฌ ์•ž์ „ ๋ฐ ๋’ท์ „์—์„œ ๋ฐœ์ƒํ•˜๋Š” ์™€๋ฅ˜์— ์˜ํ•ด์„œ ์ˆ˜์ตํ•˜์ค‘์ด ํฌ๊ฒŒ ์ฆ๊ฐ€ํ•จ์„ ๋ฐํ˜”๋‹ค. ์ด์— ์•ž์ „๊ณผ ๋’ท์ „์—์„œ ๋ฐœ์ƒํ•˜๋Š” ์œ ๋™์˜ ๋ฐ•๋ฆฌ๋ฅผ ์ œ์–ดํ•˜๊ธฐ ์œ„ํ•˜์—ฌ 0.01c, 0.3cflap, 0.95cflap ์œ„์น˜์— jet์„ ์œ„์น˜์‹œ์ผฐ๋‹ค. ๋˜ํ•œ ๋ฌด์ฐจ์› ์ฃผํŒŒ์ˆ˜(F+)์˜ ๋ณ€ํ™”์— ๋”ฐ๋ฅธ ์œ ๋™ ๊ตฌ์กฐ ๋ณ€ํ™”์™€ ํ•ญ๋ ฅ ๊ฐ์†Œ์œจ์„ ์•Œ์•„๋ณด์•˜๋‹ค. ๊ทธ ๊ฒฐ๊ณผ, ์™€๋ฅ˜์˜ ์œ ๋™ ๊ตฌ์กฐ๋ฅผ ๋ณ€ํ™”์‹œ์ผœ ์•ž์ „๊ณผ ๋’ท์ „์—์„œ ๋ฐœ์ƒํ•˜๋Š” ๊ฑฐ๋Œ€ํ•œ ์™€๋ฅ˜์˜ ๋ฐ•๋ฆฌ ์ฃผ๊ธฐ๋ฅผ ์งง๊ฒŒ ํ•˜๊ณ  ์™€๋ฅ˜์˜ ํฌ๊ธฐ๋ฅผ ๊ฐ์†Œ์‹œ์ผœ ์ •์ง€ ๋น„ํ–‰ ๋ชจ๋“œ์—์„œ ์ˆ˜์ต ํ•˜์ค‘์„ ํšจ๊ณผ์ ์œผ๋กœ ๊ฐ์†Œ์‹œํ‚ฌ ์ˆ˜ ์žˆ์—ˆ๋‹ค.๋ณธ ์—ฐ๊ตฌ๋Š” ์ง€์‹๊ฒฝ์ œ๋ถ€ ์ง€์›์œผ๋กœ ์ˆ˜ํ–‰ํ•˜๋Š” 21์„ธ๊ธฐ ํ”„๋ก ํ‹ฐ์–ด ๊ธฐ์ˆ ๊ฐœ๋ฐœ์‚ฌ์—…(์Šค๋งˆํŠธ๋ฌด์ธ๊ธฐ๊ธฐ์ˆ ๊ฐœ๋ฐœ) ๋ฐ ๋ฐฉ์œ„์‚ฌ์—…์ฒญ๊ณผ ๊ตญ๋ฐฉ๊ณผํ•™์—ฐ๊ตฌ์†Œ์˜ ์ง€์› (๊ณ„์•ฝ๋ฒˆํ˜ธ UD0700 41AD)๊ณผ ํ•œ๊ตญ๊ณผํ•™๊ธฐ์ˆ ์ •๋ณด์—ฐ๊ตฌ์› ์Šˆํผ์ปดํ“จํŒ…์„ผํ„ฐ (KSC-2007- S00-1016), BK 21์‚ฌ์—…์˜ ์ง€์›์„ ํ†ตํ•ด ์ˆ˜ํ–‰๋˜์—ˆ์Šต๋‹ˆ๋‹ค.OAIID:oai:osos.snu.ac.kr:snu2009-01/102/0000004648/10SEQ:10PERF_CD:SNU2009-01EVAL_ITEM_CD:102USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:Synthetic jet์„ ์ด์šฉํ•œ ์Šค๋งˆํŠธ ๋ฌด์ธ๊ธฐ(SUAV) ์œ ๋™์ œ์–ด Part 1.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]_YN:NCONFIRM:

    Experimental Study on Flow Characteristics of Synthetic Jet with Circular Exit Array in Separated Flow

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    Piezo-electric diaphragm์œผ๋กœ ์ž‘๋™๋˜๋Š” synthetic jet์„ ๋ฐ•๋ฆฌ ์œ ๋™ ์ œ์–ด์— ์ ์šฉํ•˜๊ธฐ ์œ„ํ•œ ์‹คํ—˜์„ ์ˆ˜ํ–‰ํ•˜์—ฌ ์ „์‚ฐ ์ˆ˜์น˜ ํ•ด์„ ๊ฒฐ๊ณผ์™€ ์œ ๋™ ํ˜„์ƒ์„ ๋น„๊ต ๋ถ„์„ํ•˜์˜€๋‹ค. ์™ธ๋ถ€ ์œ ๋™์ด ์—†๋Š” ์กฐ๊ฑด์—์„œ ์—ด์„  ์œ ์†๊ณ„๋ฅผ ํ™œ์šฉํ•œ ์ถœ๊ตฌ ์†๋„ ์ธก์ • ์‹คํ—˜์„ ํ†ตํ•ด ์ž‘๋™ ์ฃผํŒŒ์ˆ˜์™€ ์ถœ๊ตฌ ์ง€๋ฆ„์ด ์ถœ๊ตฌ ์œ ์† ๋ณ€ํ™”์— ์ค‘์š”ํ•œ ์—ญํ• ์„ ํ•˜๊ณ  ์žˆ์Œ์„ ๊ฒ€์ฆํ–ˆ๋‹ค. ์ถœ๊ตฌ ๋‹จ๋ฉด์ ์ด ๋™์ผํ•œ ์กฐ๊ฑด์˜ ์‹คํ—˜์—์„œ๋Š” ๋™์ผํ•œ ์œ ๋Ÿ‰์ด ์ถœ๊ตฌ๋ฅผ ํ†ตํ•ด ๋ถ„์ถœ๋˜๋”๋ผ๋„ ์ถœ๊ตฌ ๋‘˜๋ ˆ์˜ ๊ธธ์ด๊ฐ€ ์ปค์งˆ์ˆ˜๋ก ์ ์„ฑ์˜ ์˜ํ–ฅ์ด ์ฆ๊ฐ€ํ•˜์—ฌ ์ถœ๊ตฌ ์œ ์†์ด ๊ฐ์†Œํ•จ์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์™ธ๋ถ€ ์œ ์ž…๋ฅ˜๊ฐ€ ์žˆ๋Š” inclined flat plate์—์„œ synthetic jet ์ž‘๋™ ์ „/ํ›„์˜ ์••๋ ฅ ๊ณ„์ˆ˜ ๋ถ„ํฌ๋ฅผ ๋น„๊ตํ•˜์—ฌ ์œ ๋™ ์ œ์–ด ์„ฑ๋Šฅ์„ ๊ฒฐ์ •ํ•˜๋Š” ํ•ต์‹ฌ ํŒŒ๋ผ๋ฏธํ„ฐ์˜ ์—ญํ• ์„ ๊ฒ€์ฆํ–ˆ๋‹ค. ๊ทธ ๊ฒฐ๊ณผ ์ฃผ์–ด์ง„ ๋ฐ•๋ฆฌ ๋ฐœ์ƒ ์กฐ๊ฑด์—์„œ ์ตœ์ ์˜ ์œ ๋™ ์ œ์–ด ์„ฑ๋Šฅ์„ ๋ฐœํœ˜ํ•˜๋Š” ์ž‘๋™ ์ฃผํŒŒ์ˆ˜, ์ถœ๊ตฌ ์ง€๋ฆ„, ์ถœ๊ตฌ ๊ฐ„๊ฒฉ์„ ๋ฐœ๊ฒฌํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค.The control of separated flow on an inclined flat plate using synthetic jet which actuated by piezo-electric diaphragm was investigated experimentally. Experimental results were compared with computational results in order to analyze flow physics. According to the result of jet velocity using hot wire anemometry with no cross flow, we found that actuation frequency and orifice diameter played important role in jet velocity. On the condition of same exit area, jet velocity was decreased because of exit perimeter which related with viscous effect. According to the result of measuring static pressure on the inclined flat plate with cross flow, we found that actuation frequency and orifice diameter and gap between orifices played important role in separation control performance.๋ณธ ์—ฐ๊ตฌ๋Š” ๋ฐฉ์œ„์‚ฌ์—…์ฒญ ๋ฐ ๊ตญ๋ฐฉ๊ณผํ•™์—ฐ๊ตฌ์†Œ (UC100031JD), ์Šˆํผ์ปดํ“จํŒ…์„ผํ„ฐ(KSC-2010-C1- 0030), ํ•ญ๊ณต ์šฐ์ฃผ ์‹ ๊ธฐ์ˆ  ์—ฐ๊ตฌ์†Œ, BK 21์˜ ์ง€์› ์œผ๋กœ ์ˆ˜ํ–‰๋˜์—ˆ์Œ.OAIID:oai:osos.snu.ac.kr:snu2011-01/104/0000004648/24SEQ:24PERF_CD:SNU2011-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:๋ฐฐ์—ด๋œ_์›ํ˜•_์ถœ๊ตฌ_Synthetic_Jet์˜_๋ฐ•๋ฆฌ_์œ ๋™_์ œ์–ด_ํŠน์„ฑ์—_๊ด€ํ•œ_์‹คํ—˜์ _์—ฐ๊ตฌ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]:

    ์ถœ๊ตฌ ํ˜•์ƒ์— ๋”ฐ๋ฅธ Synthetic Jet ๋Šฅ๋™ ์œ ๋™์ œ์–ด์˜ ์‹คํ—˜์  ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€, 2011.8. ๊น€์ข…์•”.Docto

    ํ’๋™์‹คํ—˜์„ ์ด์šฉํ•œ ์ดˆ์†Œํ˜• ๋น„ํ–‰์ฒด ๊ณต๋ ฅ ํŠน์„ฑ ์—ฐ๊ตฌ์™€ ์„ค๊ณ„ ๋ฐ ๊ฐœ๋ฐœ

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€,2003.Maste

    Flow Control Capability of Synthetic Jet for the Separated Flow

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    ๋ณธ ์—ฐ๊ตฌ๋Š” ์„œ์šธ๋Œ€ํ•™๊ต ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€ BK21์‚ฌ์—…, ํ•ญ๊ณต์šฐ์ฃผ์‹ ๊ธฐ์ˆ ์—ฐ๊ตฌ์†Œ์˜ ์ง€์›์œผ๋กœ ์ˆ˜ํ–‰๋˜์—ˆ์Œ. ๋˜ํ•œ ํ•œ๊ตญ๊ณผํ•™์žฌ๋‹จ์„ ํ†ตํ•ด ๊ต์œก๊ณผํ•™๊ธฐ์ˆ ๋ถ€์˜ ์šฐ์ฃผ๊ธฐ์ดˆ์›์ฒœ๊ธฐ์ˆ ๊ฐœ๋ฐœ ์‚ฌ์—…(NSL, National Space Lab)์œผ๋กœ๋ถ€ํ„ฐ ์ง€์›๋ฐ›์•„ ์ˆ˜ํ–‰๋จ(๊ณผ์ œ๋ฒˆํ˜ธ 20090091724).OAIID:oai:osos.snu.ac.kr:snu2010-01/104/0000004648/18SEQ:18PERF_CD:SNU2010-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:Synthetic_jet์„_์ด์šฉํ•œ_๋ฐ•๋ฆฌ_์ œ์–ด_์„ฑ๋Šฅ_์—ฐ๊ตฌ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]:

    Numerical Study on Flow Characteristics of Synthetic Jet with Slot Exit

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    The flow characteristics of synthetic jet depending on rectangular and circular jet exit configuration are investigated using numerical computation with cross flow. In rectangular slot, synthetic jet generates the strong vortex, however, supply fewer momentum and effectiveness of flow control is reduced along flow direction. In circular slot, regular vortex is formed from slot center to end and developed in flow direction. It affects the wider region than rectangular slot. The distribution of wall shear stress is considered in order to indicate the effectiveness of flow control device for flow separation delay. As a result, circular slot is a more suitable candidate for delaying flow separation.๋ณธ ์—ฐ๊ตฌ๋Š” ๋ฐฉ์œ„์‚ฌ์—…์ฒญ๊ณผ ๊ตญ๋ฐฉ๊ณผํ•™์—ฐ๊ตฌ์†Œ์˜ ์ง€์›(UC100031JD), ์Šˆํผ์ปดํ“จํŒ…์„ผํ„ฐ(KSC-2010-CI-0030), ํ•ญ๊ณต ์šฐ์ฃผ ์‹ ๊ธฐ์ˆ  ์—ฐ๊ตฌ์†Œ์˜ ์ง€์›์œผ๋กœ ์ˆ˜ํ–‰๋˜์—ˆ์Œ.OAIID:oai:osos.snu.ac.kr:snu2011-01/104/0000004648/18SEQ:18PERF_CD:SNU2011-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:Synthetic_Jet_์ถœ๊ตฌ_ํ˜•์ƒ์˜_๋ณ€ํ™”์—_๋”ฐ๋ฅธ_์œ ๋™_ํŠน์„ฑ_ํŒŒ์•…์„_์œ„ํ•œ_์ˆ˜์น˜์ _์—ฐ๊ตฌ.pdfDEPT_NM:๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€EMAIL:[email protected]:

    ์‹คํ—˜์  ์—ฐ๊ตฌ๋ฅผ ํ†ตํ•œ SNU ์ดˆ์†Œํ˜• ๋น„ํ–‰์ฒด ์„ค๊ณ„ ๋ฐ ๊ฐœ๋ฐœ = Design and Development of SNU MAV using Experimental Studies

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    ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ผ๋ฐ˜ ํ•ญ๊ณต๊ธฐ์˜ ์„ค๊ณ„๊ฒฝํ—˜์‹์„ ์ด์šฉํ•˜์—ฌ SNU ์ดˆ์†Œํ˜• ๋น„ํ–‰์ฒด๋ฅผ ๊ฐœ๋…์„ค๊ณ„ ํ•˜๊ณ  ์„ค๊ณ„๋œ ๋‚ด์šฉ์„ ํ† ๋Œ€๋กœ ์‹œ์ œ๊ธฐ๋ฅผ ์ œ์ž‘ํ•˜์—ฌ ๋ฐ˜๋ณต์ ์ธ ํ’๋™์‹คํ—˜๊ณผ ๋น„ํ–‰์‹คํ—˜์„ ํ†ตํ•˜์—ฌ ํ˜•์ƒ์„ ์ตœ์ ํ™”ํ•˜์˜€๋‹ค. ๊ทธ๋ฆฌ๊ณ  ๊ณ ํšจ์œจ์˜ ์ถ”์ง„์‹œ์Šคํ…œ์„ ์œ„ํ•ด ํ”„๋กœํŽ ๋Ÿฌ ํ˜•์ƒ์— ๋”ฐ๋ฅธ ์ถ”๋ ฅ์‹คํ—˜๊ณผ ๋ฐ˜์‘๋ฉด๊ธฐ๋ฒ•(RSM)์„ ์ด์šฉํ•˜์—ฌ ์ตœ์ ์˜ ํ”„๋กœํŽ ๋Ÿฌ ํ˜•์ƒ์„ ๋„์ถœํ•˜์˜€๋‹ค. SNU ์ดˆ์†Œํ˜• ๋น„ํ–‰์ฒด๋Š” 210mAh ๋ฐฐํ„ฐ๋ฆฌ๋ฅผ ์žฅ์ฐฉํ•˜์˜€์„ ๊ฒฝ์šฐ 17๋ถ„ ์ด์ƒ์„ ๋น„ํ–‰ํ•  ์ˆ˜ ์žˆ์—ˆ์œผ๋ฉฐ, ์•ˆ์ •์„ฑ๊ณผ ์กฐ์ข…์„ฑ๋ฉด์—์„œ ์ข‹์€ ํŠน์„ฑ์„ ๊ฐ€์ง€๊ณ  ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ; The SNU MAV has been designed through studies on highly efficient aerodynamic shape and propulsion system. The configuration of the vehicle was determined from conventional empirical equations, iterative wind tunnel tests and flight tests. The propeller shape was optimized with the various thrust tests and RSM(Response Surface Method) to obtain the higher efficient propulsion system. It was certified that the MAV could fly for over 17 minutes with a 210mAh battery. In addition, it showed good flight characteristics in both stability and controllability.๋ณธ ์—ฐ๊ตฌ๋Š” ํ•œ๊ตญ๊ณผํ•™์žฌ๋‹จ ํŠน์ •๊ธฐ์ดˆ ์—ฐ๊ตฌ๊ณผ์ œ "ROS-2002-000-000329-0" ์ง€์›์˜ ์ผ๋ถ€๋กœ ์ˆ˜ํ–‰๋จ
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