Three real heat engines have the same thermal efficiency and are connected in series. The first engine absorbs 2400 kJ of heat from a thermal reservoir at 1250 K and the third engine ejects its waste of 300 kJ to a sink at 150 K. determine the work output from each engine.

Data given:
Q1 = 2400 KJ
Q4 = 300 KJ
For engine E1,
Efficiency η1 = (Q1 – Q2) / Q1
= 1 – (Q2 / Q1)
I.e. Q2 / Q1 = 1 – η1
Similarly for engine E2,
Q3 / Q2 = 1 – η2
For engine E3,
Q4 / Q3 = 1 – η3
Therefore,
(1 – η1) (1 – η2) (1 – η3)
= (Q2 / Q1) X (Q3 / Q2) X (Q4 / Q3)
= Q4 / Q1 = 300 / 2400 = 1 / 8

For same thermal efficiency of each engine:
(1 – η)3 = 1 / 8
1 – η = 1 / 2
η = 1 / 2 = 50%
Now, Q2 / Q1 = 1 – 1 / 2 = 1 / 2
Q1 = 2 Q2
Q2 = Q1 / 2 = 2400 / 2 = 1200 kJ
And
Q3 / Q2 = 1 / 2
Q3 = Q2 / 2 = 1200 / 2 = 600 kJ
Hence work output from first engine (W1) = Q1 – Q2
= 2400 – 1200 = 1200 kJ
From second engine (W2) = Q2 – Q3
= 1200 – 600 = 600 kJ
From third engine (W3) = Q3 – Q4
= 600 – 300 = 300 kJ
Total work done W = W1 + W2 + W3
= 1200 + 600 +300 = 2100 kJ

Hence the total work output of the engines in series is equal to 2100 kJ

Category: Second Law of Thermodynamics

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