(i) An isothermal expansion till it reches volume 2V, and heat Q flows into the gas (ii) An isobaric compression back to the original volume V (iii) An isochoric increase in pressure till the original pressure P is regained. The efficiency of this cycle can be expressed as 0 (a) == (c) == 4Q-2RT 4Q+3RT 4Q-2RT 40+ RT (b) == (d) E= 40+2RT 4Q-3RT 4Q+2RT 40+ RT
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