l27 - the brayton cycle

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Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 27 Gas Power Generation The Brayton Cycle

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Page 1: L27 - The Brayton Cycle

Department of Mechanical EngineeringME 322 – Mechanical Engineering

Thermodynamics

Lecture 27

Gas Power GenerationThe Brayton Cycle

Page 2: L27 - The Brayton Cycle

Gas Power Cycles• Much higher power output to weight ratio compared to

vapor power cycles– Well suited for mobile power plants– Smaller stationary power plants

• Commonly known as the gas turbine

Open cycle Closed cycle

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Page 3: L27 - The Brayton Cycle

The Gas TurbineComparison of the schematic to the ‘real thing’

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Page 4: L27 - The Brayton Cycle

Gas Turbine Examples

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Page 5: L27 - The Brayton Cycle

The Air Standard Cycle (ASC) Analysis

• A fixed amount of air modeled as an ideal gas is the working fluid

• The combustion process is replaced by a heat transfer from an external source

• All processes are internally reversible

The Cold Air Standard Cycle Analysis

• All of the above plus … the heat capacity of the air is assumed to be constant

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Page 6: L27 - The Brayton Cycle

The Brayton Cycle• 1-2: Reversible and adiabatic compression• 2-3: Constant pressure heat addition• 3-4: Reversible and adiabatic expansion• 4-1 Constant pressure heat rejection

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Brayton Cycle Analysis

2 1cW m h h

3 2inQ m h h

3 4tW m h h

4 1outQ m h h

cycle net t cW W W W

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Page 8: L27 - The Brayton Cycle

Brayton Cycle PerformanceThermal Efficiency

,ASCnet t c

thin in

W W WQ Q

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4 1,ASC

3 2

1th

h hh h

3 2 4 1 4 1

3 2 3 2

1h h h h h h

h h h h

3 4 2 1 3 4 2 1

3 2 3 2

m h h m h h h h h h

m h h h h

Page 9: L27 - The Brayton Cycle

Cold Brayton Cycle Performance

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Cold Air Standard Thermal Efficiency

4 1 4 1,cold ASC

3 2 3 2

1 1 pth

p

h h c T Th h c T T

3 34 4

2 1 1 2

1 1T TT TT T T T

Processes 3-4 and 1-2 are isentropic

1 4 14 1

3 2 2 3 2

/ 11 1

/ 1T T TT T

T T T T T

1 / 1 /

3 3 2 2

4 4 1 1

k k k kT P P TT P P T

Page 10: L27 - The Brayton Cycle

Cold Brayton Cycle Performance

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1 4 1,cold ASC

/ 11th

T T T

2 3 2/ 1T T T 1

2

1 TT

Substituting ...

Since process 1-2 is isentropic,

1 / 1

1 1 1,cold ASC

2 2 2

1 1 1k k k

thT P vT P v

Page 11: L27 - The Brayton Cycle

Cold Brayton Cycle Performance

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Define ...

Finally ... we have several ways to write the cold ASC thermal efficiency,

1,cold ASC

2

1 /1 /1

2

111

2

1

1 1

1 1

th

k kk k

k

k

TT

P PRP

v CRv

2

1

pressure ratioP PRP

1

2

compression ratiov CRv

Page 12: L27 - The Brayton Cycle

Gas Turbine Irreversibilities

Isentropic efficiencies in the turbine and compressor

Isentropic efficiencies in the turbine and compressor and pressure drops

in the heat exchangers

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