Initial stage P1=4.8bars;T1=160oC=160+273=433K;V1=0.25m3 
First process; Adiabatic expansion. P2=1.5bar 
Second process: Heat given at constant pressure 
dh= Change in enthalpy = 80 kJ
So P-V diagram 
Let mass of air flowing = m
Now, ideal air has the equation; PV= mRT, where R=Cp−Cv=1.005−0.714=0.291kJ/kgK 
Putting all the values; m=RT1P1V10.291∗4334.8∗0.25=0.00952kg 
Now , during process 1-2
P1V1r=P2V2r 
V2=V1(P2P1)r1 r = 1.4 for air. 
V2=0.25(1.54.8)1.41=0.5738m3 
W1−2= Work done in adiabatic process. 
 W1−2=r−1P1V1−P2V2=1.4−14.8∗0.25−1.5∗0.5738=0.84825kJ
Considering process 2-3
First, let us calculate T2  
P1V1r=P2V2r⟹P1r−1T1r=P2r−1T2r 
 T2=T1(P1P2)r1−r=433(4.81.5)1.41−1.4=310.5699K
Now as a change in enthalpy =mCpdT 
80=0.00952(1.005)(T3−310.5699)⟹T3=8672.123K 
By the first law of thermodynamics 
Q=△U+W 
80=mCvdT+W2−3 
80=0.00952∗0.714(8672.123−310.5699)+W2−3 
W2−3=23.16418kJ 
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