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OCTOBER 19-20, 2012 - YMCA University of Science & Technology

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2.2. Gas Turbines<br />

Proceedings <strong>of</strong> the National Conference on<br />

Trends and Advances in Mechanical Engineering,<br />

<strong>YMCA</strong> <strong>University</strong> <strong>of</strong> <strong>Science</strong> & <strong>Technology</strong>, Faridabad, Haryana, Oct <strong>19</strong>-<strong>20</strong>, <strong>20</strong>12<br />

For the expansion ratio, r e temperature at the exit <strong>of</strong> the turbine isentropic process can be calculated by<br />

( γ g −1)<br />

γ g<br />

gos gi e<br />

T = T ( r )<br />

The actual temperature T go at the exit <strong>of</strong> the turbine can be calculated by<br />

T<br />

ηT<br />

=<br />

T<br />

And the inlet and outlet humidity ratios will be the same<br />

w<br />

gi<br />

gi<br />

gi<br />

−T<br />

−T<br />

= w<br />

The energy balance yields the turbine work W T given by the following relation<br />

go<br />

gos<br />

go<br />

WT = hgi − hgo<br />

The exergy balance for the turbine gives the exergy destruction e DT as following<br />

2.3. Combustor<br />

e = ( e − e ) − W<br />

DT gi go T<br />

Mass <strong>of</strong> fuel supplied can be calculated by energy balance between the energy supplied by the fuel and change in<br />

enthalpy <strong>of</strong> combustion products due to this heat addition. Change in enthalpy <strong>of</strong> air after adding fuel in<br />

combustion chamber is<br />

η m CV = h − h = h − h<br />

cc f go gi<br />

3 2<br />

The exergy balance <strong>of</strong> the combustion chamber yields exergy destruction<br />

Where<br />

and ∆ g = ∆H −T ( s − s )<br />

r r av P R<br />

eDCC = m<br />

fCCe fCC<br />

+ eai − ego<br />

e = ∆ g + R T<br />

fCC r f a<br />

(s P −s R ) is the entropy change during the combustion process and is given as<br />

where<br />

⎡ Tgo pgo ⎤ ⎡ Tgo pgo<br />

⎤<br />

sP − sR = xa ⎢C pa<br />

ln − Ra ln ⎥+ xv ⎢C pv<br />

ln −Rv<br />

ln ⎥<br />

⎣ Tai pai ⎦ ⎣ Tai pai<br />

⎦<br />

x a<br />

1<br />

= and<br />

1 + w<br />

ln<br />

p<br />

x<br />

p<br />

v<br />

f<br />

a<br />

w<br />

=<br />

1 + w <br />

The effect <strong>of</strong> water vapor present in fuel is neglected and humidity ratio at combustion chamber outlet will be<br />

higher than inlet.<br />

2.4. Air Preheater (regenerator)<br />

Temperature <strong>of</strong> air (T ao ) at the exit <strong>of</strong> a heat exchanger can be calculated by<br />

Tao<br />

−T<br />

Heat Exchanger Effectiveness =<br />

T −T<br />

Applying the energy balance equation on the heat exchanger yields<br />

gi<br />

ai<br />

ai<br />

182

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