Use heat into the gas as positive. The two adiabatic stages have . During constant-pressure heating and constant-volume cooling,The first law over a complete cycle gives , since the internal energy returns to its initial value. ThereforeSubstitute the temperatures:HenceEquivalently, define compression ratio and cutoff ratio :These formulas use the ideal constant-heat-capacity model and reversible adiabatic strokes. The heat-addition and heat-rejection strokes occur over changing gas temperatures, unlike the isothermal heat exchanges of a Carnot engine.
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