The Carnot cycle is not used in real engines primarily because it assumes no increase in entropy, which is unattainable in practical applications due to imperfections in materials and processes. While the cycle theoretically operates between two temperature sinks, the isothermal heat transfer it requires is physically impossible without a temperature gradient. Although the Stirling cycle can achieve maximum theoretical efficiency similar to the Carnot cycle and is implemented in some applications, most engines utilize more practical cycles like the Otto cycle. The discussion highlights that even with a saturated liquid, heat transfer necessitates a gradient at the boundary, reinforcing the impracticality of the Carnot cycle in real-world scenarios. Ultimately, the limitations of the Carnot cycle stem from both theoretical constraints and the inherent behaviors of working fluids.