674 ENGINEERING THERMODYNAMICSdharm
\M-therm\Th13-5.pm513.10.7. Closed Cycle Gas Turbine (Constant pressure or joule cycle).
Fig. 13.47 shows a gas turbine operating on a constant pressure cycle in which the closed
system consists of air behaving as an ideal gas. The various operations are as follows : Refer Figs.
13.48 and 13.49.
Operation 1-2 : The air is compressed isentropically from the lower pressure p 1 to the
upper pressure p 2 , the temperature rising from T 1 to T 2. No heat flow
occurs.
Operation 2-3 : Heat flow into the system increasing the volume from V 2 to V 3 and
temperature from T 2 to T 3 whilst the pressure remains constant at p 2.
Heat received = mcp (T 3 – T 2 ).
Operation 3-4 : The air is expanded isentropically from p 2 to p 1 , the temperature falling
from T 3 to T 4. No heat flow occurs.
Operation 4-1 : Heat is rejected from the system as the volume decreases from V 4 to V 1
and the temperature from T 4 to T 1 whilst the pressure remains con-
stant at p 1. Heat rejected = mcp (T 4 – T 1 )
ηair-standard =
Work done
Heat received
=
Heat received/cycle Heat rejected/cycle
Heat received/cycle−=mc T T mc T T
mc T TTT
TTp p
p()()
()32 41
3241
321
−− −
−=− −
−
Now, from isentropic expansionT
Tp
p2
12
11
=
F
HGI
KJ−γ
γWork2C T1Heater34Cooling
medium
Fig. 13.47. Closed cycle gas turbine.