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A EROSPACE E NGINEERING L ABORATORY (MAE308)

A EROSPACE E NGINEERING L ABORATORY (MAE308) . P ROF . S EUNG W OOK B AEK D IV . OF A EROSPACE E NGINEERING , KAIST, IN KOREA R OOM : Building N7-2 #3304 T ELEPHONE : 3714 swbaek@kaist.ac.kr http://procom.kaist.ac.kr T A : H YEMIN K IM R OOM : Building N7-2 #3315

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A EROSPACE E NGINEERING L ABORATORY (MAE308)

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  1. AEROSPACE ENGINEERING LABORATORY (MAE308) • PROF. SEUNG WOOK BAEK • DIV.OFAEROSPACE ENGINEERING, KAIST, IN KOREA • ROOM: Building N7-2 #3304 • TELEPHONE : 3714 • swbaek@kaist.ac.kr • http://procom.kaist.ac.kr • TA: HYEMIN KIM • ROOM: Building N7-2 #3315 • TELEPHONE : 3754 • enok2695@kaist.ac.kr

  2. MAE 308 Understanding of polytropic process by using RCM • CONTENTS • 1. Objectives • 2. Background • 3. Experimental setup • 4. Isothermal, Adiabatic process • 5. Thermodynamic relation PROPULSION AND COMBUSTION LABORATORY AEROSPACE ENGINEERING LABORATORY

  3. Objective Polytropic process using the RCM Week 1 Week 2 • RCM operation with air • by varying operation speed • operation with various gases • estimation of • thermodynamic process Determination of specific heat ratio index

  4. Background What is RCM?(Rapid compression machine) → Experimental simulator of HCCI (Homogeneous Charge Compression Ignition) → Single compression stroke Application → Combustion experiment → Analysis of product gas

  5. Experimental setup

  6. Isothermal process n = 1 (monatomic), n = 5/3(diatomic)

  7. Adiabatic process Very short time

  8. Isothermal, Adiabatic process • Carnot cycle • Isothermal process • during heat exchange • Isentropic compression • and expansion Isothermal Heat in Heat in Isentropic compression Isentropic expansion Heat out Isothermal Heat out

  9. Thermodynamic relation Operation time t → 0 Adiabatic 0<t<∞ Polytropic Isothermal t →∞ Ppeak1 > Ppeak2> Ppeak3 State 2. State 1.

  10. Thermodynamic relation Heat loss through the wall… Polytropic process !! Controlling Parameters : Thermal conductivity, internal flow, operation time ….

  11. Thermodynamic relation Thermodynamic relation Operation time Vs. index n Adiabatic Ideal case (Adiabatic) n=1.4(N2), 1.667(Ar) (Isothermal) n=1.0 (Polytropic) n = ? n = LogCRPPeak Index n distribution according to time and CR at aircase

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