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MAE 4261: AIR-BREATHING ENGINES

MAE 4261: AIR-BREATHING ENGINES. Thermodynamics Review and Cycle Analysis Overview September 1, 2009 Mechanical and Aerospace Engineering Department Florida Institute of Technology D. R. Kirk. INTRODUCTION TO CYCLE ANALYSIS. Cycle Analysis → What determines engine characteristics?

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MAE 4261: AIR-BREATHING ENGINES

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  1. MAE 4261: AIR-BREATHING ENGINES Thermodynamics Review and Cycle Analysis Overview September 1, 2009 Mechanical and Aerospace Engineering Department Florida Institute of Technology D. R. Kirk

  2. INTRODUCTION TO CYCLE ANALYSIS • Cycle Analysis → What determines engine characteristics? • Cycle analysis is study of thermodynamic behavior of air as it flows through engine without regard for mechanical means used to affect its motion • Characterize components by effects they produce • Actual engine behavior is determined by geometry • Cycle analysis is sometimes characterized as representing a “rubber engine” • Main purpose is to determine which characteristics to choose for components of an engine to best satisfy a particular need • Express T, h, Isp, TSFC as function of design parameters • Aircraft engines (and all gas turbine engines) operate on a Brayton Cycle

  3. HEAT ENGINE: PROPULSION CHAIN Mechanical Power Mech. Power to GasFlow Thrust Power Chemical Energy Heat (Thermal Energy) Mechanical Propulsive Combustion Thermal The overall efficiency for the propulsion chain is given by:

  4. CONCEPTS / TOOLS FOR ENGINE IDEAL CYCLE ANALYSIS • Ideal gas equation of state, p = rRT • One-dimensional gas dynamics • Concepts of stagnation and static quantities (temperature, pressure, etc.) • Relations between Mach number and thermodynamic properties • Thermodynamics of propulsion cycle • Make use of 1st and 2nd Laws of Thermodynamics • Behavior of useful quantities: energy, entropy, enthalpy • Relations between thermodynamic properties in a reversible (“lossless”) process • Isentropic = reversible + adiabatic • Properties of cycles (it is cyclic) • Air starts at atmospheric pressure and temperature and ends up at atmospheric pressure and temperature • Definition of ‘Open’ vs. ‘Closed’ Cycles

  5. STAGNATION QUANTITIES DEFINED • Quantities used in describing engine performance are the stagnation pressure, enthalpy and temperature • Stagnation enthalpy, ht , enthalpy state if stream is decelerated adiabatically to zero velocity Ideal gas Stagnation temperature Speed of sound Total to static temperature ratio in terms of Mach number

  6. FOR REVERSIBLE + ADIABATIC = ISENTROPIC PROCESS

  7. RECAP ON THERMODYNAMICS: 1st LAW First law (conservation of energy) for a system: “chunk” of matter of fixed identity E0 = Q - W Change in overall energy (E0 ) = Heat in - Work done E0 = Thermal energy + kinetic energy ... Neglecting changes in kinetic and potential energy E = Q - W ;(Change in thermal energy) On a per unit mass basis, the statement of the first law is thus: e = q - w

  8. RECAP ON THERMODYNAMICS: 2nd LAW The second law defines entropy, s, by: Where dqreversible is the increment of heat received in a reversible process between two states The second law also says that for any process the sum of the entropy changes for the system plus the surroundings is equal to, or greater than, zero Equality only exists in a reversible (ideal) process

  9. REPRESENTING ENGINE PROCESS IN THERMODYNAMIC COORDINATES First Law: E = Q - W, where E is the total energy of the parcel of air. For a cyclic process E is zero (comes back to the same state) Therefore: Q (Net heat in) = W (Net work done) Want a diagram which represents the heat input or output. A way to do this is provided by the Second Law where ds is the change in entropy of a unit mass of the parcel and dq is the heat input per unit mass Thus, one variable should be the entropy , s

  10. STEADY FLOW ENERGY EQUATION (I) For any device in steady flow Heat input Per unit mass flow rate: 2 1 Mass flow Device Shaft work q is heat input/unit mass wshaft is the shaft work / unit mass

  11. STEADY FLOW ENERGY EQUATION (II) • The form of the steady flow energy equation shows that enthalpy, h: h = e + pv = e + p/r • Natural variable to use in fluid flow-energy transfer processes. • For an ideal gas with constant specific heat, dh = cpdT. • Changes in enthalpy are equivalent to changes in temperature. • To summarize, the useful natural variables in representing gas turbine engine processes are h,s (or T, s). • Represent thermodynamic cycle (Brayton) for gas turbine engine on a T,s diagram

  12. THERMODYANMICS: BRAYTON CYCLE MODEL

  13. GAS TURBINE ENGINE COMPONENTS • Inlet: Slows, or diffuses, the flow to the compressor • Fan/Compressor: (generally two, or three, compressors in series) does work on the air and raises its stagnation pressure and temperature • Combustor: Heat is added to the air at roughly constant pressure • Turbine: (generally two or three turbines in series) extracts work from the air to drive the compressor or for power (turboshaft and industrial gas turbines) • Afterburner: (on military engines) adds heat at constant pressure • Nozzle: Raises the velocity of the exiting mass flow • Exhaust gases reject heat to the atmosphere at constant pressure

  14. THERMODYNAMIC CHARACTERISTICSOF COMPONENTS (IDEAL COMPONENTS)

  15. THERMODYNAMIC MODEL OF GAS TURBINE ENGINE CYCLE [Cravalho and Smith]

  16. SCHEMATIC OF CONDITIONS THROUGH A GAS TURBINE [Rolls-Royce]

  17. NOMINAL PRESSURES AND TEMPERATURES FOR A PW4000 TURBOFAN [Pratt&Whitney]

  18. REVIEW OF STATION LOCATIONS

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