34 HANDBOOK OF ELECTRICAL ENGINEERING
The turbine energy changes fromUteatoUtea+Utea. Substitute (2.40) into (2.29),
Utea+Utea=CptT 3 ( 1 −(rpt+rpt)nt)ηt
=CptT 3 ηt
[
1 −
(
rptn+
ntP 3 nt−^1
P 4 nt
P 223 −
ntrptnt
P 4
P 4
)]
from which,
Utea=+ntηtCptT 3 rptnt−^1
[
rptP 4 −rptP 1 −P 23
P 4
]
( 2. 41 )
The change in efficiencyηpain (2.33) is,
ηpa+ηpa=
Utea+Utea−Ucea−Ucea
Ufea+Ufea
( 2. 42 )
from which, by substituting forUtea,Ucea= 0 .0andUfea= 0 .0 and deducting the initial con-
ditions gives,
ηpa=
Utea
Ufea
( 2. 43 )
The change in work done on the generator
Uoutea=UteakJ/kg ( 2. 44 )
Note that in the above analysis the signs of the practical changes are,
P 1 is negative
P 23 is negative
and P 4 is positive
The pressure dropsP 1 andP 4 are dependent upon the layout of the gas turbine generator,
the dimensions of the ducting systems and the specification of silencers and filters.P 23 is fixed by the
design of the combustion system and cannot be changed by external factors such as ducting systems.
2.2.4.1 Typical values of pressure drop losses
A newly installed gas turbine generator can be taken to have the typical losses given in Table 2.2.
Table 2.2. Typical pressure drop losses in gas turbine
Inlet or Pressure drop % change in
exhaust
Bar Inches
of water
Power
output
Heat
rate
Inlet 0.01245 5.0 −2.00 +0.75
Exhaust 0.006227 2.5 −0.50 +0.40