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Gas Power Cycles Cengel & Boles, Chapter 8 ME 152.

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Presentation on theme: "Gas Power Cycles Cengel & Boles, Chapter 8 ME 152."— Presentation transcript:

1 Gas Power Cycles Cengel & Boles, Chapter 8 ME 152

2 Analysis of Power Cycles - Basics
Power cycle = Heat engine Recall thermal efficiency: Carnot heat engine: The Carnot cycle has the maximum possible efficiency, but is not a realistic model for a power cycle since it is so impractical ME 152

3 Analysis of Power Cycles - Basics, cont.
More practical models are called ideal cycles - they are internally reversible but typically have external irreversibilities Ideal cycle assumptions include: absence of friction quasi-equilibrium processes pipes and connections between various components are well-insulated, i.e., heat transfer is negligible negligible KE and PE effects (except in diffusers and nozzles) negligible pressure drop in HXers ME 152

4 Gas Power Cycles Working fluid remains in gaseous phase throughout cycle Common gas cycles Otto*: spark-ignition ICE engine, closed system Diesel*: compression-ignition ICE engine, closed system Dual: Otto/Diesel combo, closed system Stirling: ext. combustion, closed system Ericsson: ext. combustion, control volume Brayton*: gas turbine engine or power plant, control volume * covered in this course ME 152

5 Internal Combustion Engine (ICE) terms
Bottom-dead center (BDC) – piston position where volume is maximum Top-dead center (TDC) – piston position where volume is minimum Clearance volume – minimum cylinder volume (VTDC = V2) Compression ratio (r) Displacement volume Mean Effective Pressure (MEP) ME 152

6 ICE terms, cont. Spark-ignition (SI) engine - reciprocating engine where air-fuel combustion is initiated by a spark plug Compression-ignition (CI) engine - reciprocating engine where air-fuel combustion is initiated by compression Four-stroke engine - piston executes intake, compression, expansion, and exhaust in four strokes while crankshaft completes two revolutions Two-stroke engine - piston executes intake, compression, expansion, and exhaust in two strokes while crankshaft completes one revolution ME 152

7 Analysis of Gas Power Cycles
Air-standard assumptions: working fluid is a fixed mass of air which is modeled as a closed system and behaves as an ideal gas all processes are internally reversible unless stated otherwise combustion process is replaced by a heat addition process from an external source exhaust process is replaced by a heat rejection process that restores air to its initial state ME 152

8 Analysis of Gas Power Cycles, cont.
Constant specific heat approach (aka cold-air standard) - for approximate analysis only where cv , cp are evaluated at 25°C, 1 atm Variable specific heat approach - for more accurate analysis where u and h obtained from Table A-17 ME 152

9 Analysis of Gas Power Cycles, cont.
Isentropic compression/expansion if compression ratio (v1/v2) is known, e.g., in Otto or Diesel cycles, use (find u2 or h2 from vr2 in Table A-17) if pressure ratio (P2/P1) is known, e.g., in a Brayton cycle, use (find u2 or h2 from Pr2 in Table A-17) ME 152

10 Otto Cycle Analysis Thermal efficiency
Heat addition (process 2-3, v = const) Heat rejection (process 4-1, v = const) ME 152

11 Diesel Cycle Analysis Thermal efficiency
Heat addition (process 2-3, P = const) Heat rejection (process 4-1, v = const) ME 152

12 Cold-Air Standard Thermal Efficiency
Otto Cycle Diesel Cycle ME 152

13 The Brayton Cycle Ideal cycle for gas turbine engines and power plants
The air-standard Brayton cycle has a closed-loop configuration, even though most applications are open-loop Basic components: Compressor (increases pressure of gas) Heat exchanger or combustor (const P heat addition) Turbine (produces power) Heat exchanger (const P heat rejection) ME 152

14 Air-Standard Brayton Cycle Analysis
Compressor Combustor (heat addition) Turbine Heat Exchanger (heat rejection) ME 152

15 Air-Standard Brayton Cycle Analysis, cont.
Thermal Efficiency Back Work Ratio as discussed in Ch. 6, a gas compressor requires much greater work input per unit mass than a pump for a given pressure rise; thus the rbw for a gas power cycle (40-60%) is much greater than that for a vapor power cycle (1-2%) ME 152

16 Air-Standard Brayton Cycle Analysis, cont.
Cold-air standard thermal efficiency High pressure ratios (rp =P2/P1) yield the highest thermal efficiency, however, moderate pressure ratios often yield a higher power-to-weight ratio Maximum turbine inlet temperature is around 1700 K, imposed by metallurgical properties ME 152

17 Improving Gas Turbine Cycle Performance
Regeneration - utilizes turbine exhaust gas to preheat air entering the combustor; this reduces heat addition requirement and increases thermal efficiency Multistage turbine with reheat - similar to vapor power cycles; increases thermal efficiency Compressor intercooling - gas is cooled between compressor stages; decreases compressor work and bwr, increases thermal efficiency ME 152

18 Gas Turbine Aircraft Propulsion
Gas turbines are ideal for aircraft propulsion due to high power-to-weight ratio Basic turbojet engine - inlet diffuser, compressor, combustor, turbine, exit nozzle Turbofan engine - inlet fan brings in additional air which bypasses engine core and increases thrust from nozzle Turboprop engine - turbine powers a propeller, which provides primary thrust Ramjet - high-speed air is compressed by ram effect and then heated by combustor; thrust is developed by nozzle w/o need for compressor or turbine ME 152


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