Common Data: A thermodynamic cycle with an ideal gas as working fluid is shown below.
If the specific heats of the working fluid are constant and the value of specific heat ratio γ is 1.4, the thermal efficiency (%) of the cycle is
A
42.6
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B
40.9
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C
21
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D
59.7
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Solution
The correct option is C21
Process 2−3 Q2−3=(U3−U2)+W2−3 Q2−3=(U3−U2)+0 =mcv(T3−T2) =mcv(p3V3mR−p2V2mR) =cvR(p3V3−p2V2) =cvcp−cv(400×1−100×1) Q2−3=1γ−1(400−100) =3001.4−1=3000.4=750kJ Q1.2=(U2−U1)+W1−2 =mcv[p2V2mR−p1V1mR]+p(V2−V1) =cvR[p(V2−V1)]+p(V2−V1) =p(V2−V1){cvR+1} =p(1−V1){cvcp−cv+1}[∵V2=1m3] =100(1−V1){1γ−1+1}
Calculating V1 p3Vγ3=p1Vγ1 ∴V1=[p3.Vγ3p1]1γ =[400100×1]11.4 Q1−2=100[1−2.692]×{10.4+1} =−592.2kJ
(minus sign represent heat is rejected). There is no transfer in process 3−1 as it is reversible adiabatic proces.
Effeiency of cycle. η=1−QrejectQadded=1−592.2750 =0.2014=21.04%