Initial stage "P_1=4.8 bars; T_1=160^oC=160+273=433K; V_1=0.25 m^3"
First process; Adiabatic expansion. "P_2=1.5 bar"
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=C_p-C_v=1.005-0.714=0.291kJ\/kgK"
Putting all the values; "m=\\frac{P_1V_1}{RT_1}\\frac{4.8*0.25}{0.291*433}=0.00952kg"
Now , during process 1-2
"P_1V_1^r=P_2V_2^r"
"V_2=V_1(\\frac{P_1}{P_2})^{\\frac{1}{r}}" r = 1.4 for air.
"V_2=0.25(\\frac{4.8}{1.5})^{\\frac{1}{1.4}}=0.5738 m^3"
"W_{1-2}=" Work done in adiabatic process.
"W_{1-2}=\\frac{P_1V_1-P_2V_2}{r-1}=\\frac{4.8*0.25-1.5*0.5738}{1.4-1}=0.84825kJ"
Considering process 2-3
First, let us calculate "T_2"
"P_1V_1^r=P_2V_2^r\\implies \\frac{T_1^r}{P_1^{r-1}}= \\frac{T_2^r}{P_2^{r-1}}"
"T_2=T_1(\\frac{P_2}{P_1})^{\\frac{1-r}{r}}=433(\\frac{1.5}{4.8})^{\\frac{1-1.4}{1.4}}=310.5699K"
Now as a change in enthalpy ="mC_pdT"
"80=0.00952(1.005)(T_3-310.5699) \\implies T_3=8672.123K"
By the first law of thermodynamics
"Q=\\triangle U+W"
"80=mC_vdT+W_{2-3}"
"80=0.00952*0.714(8672.123-310.5699)+W_{2-3}"
"W_{2-3}=23.16418 kJ"
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