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  • ๋…ผ๋ฌธ
  • ๊ธฐ์—…์‹ ์šฉ๋ณด๊ณ ์„œ
  • ์ทจ์—…์ž๋ฃŒ
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์ „๋ฌธ์ง€์‹ 65๊ฑด

Static Characteristics of Plain Journal Bearings." Journal of the KSTLE, Vol.6, No.2, pp.76-87, 1990 (6) Vijayaraghavan, D. and Keith JR., T.G., "Effect of Type and Location of Oil Groove on the Performance of Journal Bearings," Tribology Transactions, Vol.35, pp.98-106, 1992 (7) ์‹ ๋™์šฐ, ์ž„์œค์ฒ , โ€œ๊ทธ
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  • ์ตœ๊ทผ 2์ฃผ ํŒ๋งค ์ด๋ ฅ ์—†์Œ
ation ์„ ์–ป๋Š”๋‹ค . ๋ฐ”๋กœ ์œ„์˜ ์‹์—์„œ ๊ฐ ํ•ญ์„ ๊ฐ๊ฐ Pressure head, Velocity head, static head๋ผ๊ณ  ํ•œ๋‹ค. Bernoulliโ€™s Equation์˜ ํ•ด์„์„ ๋ณด๋‹ค ์šฉ์ดํ•˜๊ฒŒ ํ•˜๊ธฐ ์œ„ํ•˜์—ฌ ๊ธฐํ•˜ํ•™์ ์ธ ๊ฐœ๋… ์„ ๋„์ž…ํ•œ ์—๋„ˆ์ง€์„ (Energy line, EL)๊ณผ ์ˆ˜๋ ฅ๊ตฌ๋ฐฐ์„ (Hydraulic grade line, HGL)์„ ์‚ฌ์šฉํ•˜
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  • ์ตœ๊ทผ 2์ฃผ ํŒ๋งค ์ด๋ ฅ ์—†์Œ
pressure_coefficient โ–  ๋ณ„ ์ฒจ 1) ๊ฑด๊ตญ๋Œ€ํ•™๊ต ์•„์Œ์† ํ’๋™ ์ œ์› ๊ตฌ ๋ถ„ ์ œ ์› Type Open Type(๊ฐœ๋ฐฉํ˜•) Rang of Wind Velocity 0.5~30 m/sec Test Section 300ร—300 mm Distribution of Wind Velocity Less than 0.5% at, mean velocity(5~15 m/sec) Turbulence Factor Percent Turbulence 0.5% at 15m/sec Component - B
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  • ์ตœ๊ทผ 2์ฃผ ํŒ๋งค ์ด๋ ฅ ์—†์Œ
์†๋„ ๋ณ€ํ™”๊ตฌ๊ฐ„์„ ๋งˆ์šฐ์Šค๋กœ ๋ฒ”์œ„๋ฅผ ์ •ํ•˜๊ณ  ๊ธฐ์šธ๊ธฐ๋ฅผ ๊ตฌํ–ˆ๋Š”๋ฐ, ๊ทธ ๊ธฐ์šธ๊ธฐ๊ฐ€ ๊ฐ€์†๋„๋ผ๋Š” ๊ฒƒ์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์šด๋™๋งˆ์ฐฐ๊ณ„์ˆ˜๋ฅผ ๊ณ„์‚ฐํ•ด ํ‘œ์— ์ ๊ณ  ์•ž์—์„œ ์‹คํ—˜ํ•œ ๊ฐ’๊ณผ ๋น„๊ตํ•ด ๋ณด์•˜๋‹ค. ์ •์ง€, ์šด๋™๋งˆ์ฐฐ๋ ฅ (statics and kinetic friction) ๊ฒฐ๊ณผ๋ณด๊ณ ์„œ 4์กฐ 
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Coefficient of Thermal Expansion (106/ ) 100 0.120 0.116 13.76 200 0.115 0.125 14.51 300 0.107 0.132 15.36 400 0.098 0.138 15.81 Fig. 4 Step 1, Room Temperature Fig.5 Step 4. Room Temperature Fig. 6 Step 8, Room Temperature Fig. 7 Step 1, High Temperature Fig. 8 Step 4, High Temperature Fig. 9 Ste
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  • ์ตœ๊ทผ 2์ฃผ ํŒ๋งค ์ด๋ ฅ ์—†์Œ
pressureolumeemperature method for estimation of cryogenic liquid volume - ์ตœ๋™์ค€, ์˜ค์ •ํƒ, ๋‹จ์—ด์„๊ณ ๋ คํ•œ์ดˆ์ €์˜จ์•ก์ฒด์งˆ์†Œ์ €์žฅํƒฑํฌ์˜์ง€์ง€๋Œ€์šฉ์ ‘๋ถ€์„ค๊ณ„ - ๊น€์ต์ˆ˜, ๊ทน์ €์˜จ ์ €์žฅ์šฉ๊ธฐ์˜ ๋‹จ์—ดํšจ์œจํ–ฅ์ƒ์— ๊ด€ํ•œ ์—ฐ๊ตฌ - BSI(British Standards), Cryogenic vessels Static vacuum insulated
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coefficient measurements of ZnO single crystal epitaxial films deposited by pulsed laser deposition - J. Appl. Phys. 85, 7884 (1999); doi:10.1063/1.370601 Heterostructures of ZnOZn coaxial nanocables and ZnO nanotubes - Appl. Phys. Lett. 81, 1312 (2002); doi:10.1063/1.1499512 Initial preferred g
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์ƒ๊ธด ์••๋ ฅ์œผ๋กœ์จ 1/2pV2์™€ ๊ฐ™๋‹ค. ๊ทธ๋ฆฌ๊ณ  ๋น„์••์ถ•์„ฑ ํ๋ฆ„์—์„œ๋Š” total pressure์™€ static pressure์˜ ์ฐจ์ด์ด๋ฉฐ,kinetic pressure๋ผ๊ณ ๋„ ํ•œ๋‹ค. ๊ทธ๋ฆฌ๊ณ  static pressure๋Š” mass flow velocity์˜ ๋ฒกํ„ฐ๋ฐฉํ–ฅ์— ์ ‘ํ•˜๋Š” ์ •์ง€๋œ ํ‘œ๋ฉด๊ณผ ๊ด€๋ จ๋œ ์••๋ ฅ์ด๋‹ค. ๋ฒ ๋ฅด๋ˆ„์ด ๋ฐฉ์ •์‹์˜ ๋” ์ž
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pressure rises to 400 kPa, calculate (a) the new temperature; (b) the total heat transfer; and (c) the change in entropy. Solution: For oxygen, take k = 1.40, R = 260 J/kg ? K, and cv = 650 J/kg ? K. Then P9.4 Consider steady adiabatic airflow in a duct. At section B, the pre
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Pressure Distribution) ์ •์••(static pressure)์˜ ๋ณ€ํ™”๋Š” ๋‚ ๊ฐœํ‘œ๋ฉด์— ์ž‘์šฉํ•˜๋Š” ๊ตญ๋ถ€์ •์••(PL: local static pressure)๊ณผ ๋Œ€๊ธฐ์••(: atmospheric pressure)์˜ ์ฐจ์ด๋กœ ํ‘œ์‹œ๋  ์ˆ˜ ์žˆ๋‹ค. โ–ณP : ์ •์••๋ณ€ํ™”, : ๋‚ ๊ฐœํ‘œ๋ฉด์— ์ž‘์šฉํ•˜๋Š” ๊ตญ๋ถ€์ •์••, : ๋Œ€๊ธฐ์•• ๊ทธ๋ฆผ์€ ์—์–ดํฌ์ผ ์ฃผ์œ„์˜ ์••๋ ฅ
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