The Carnot Cycle: Processes, Efficiency, and Detailed Derivation The Carnot cycle is a theoretical thermodynamic cycle that provides an idealized model for heat engines. Named after the French physicist Sadi Carnot, who first described it in 1824, the Carnot cycle defines the maximum possible efficiency that any heat engine can achieve. In this detailed blog, we will explore the processes involved in the Carnot cycle, derive its efficiency, and discuss its significance in thermodynamics. Understanding the Carnot Cycle The Carnot cycle consists of four reversible processes: two isothermal (constant temperature) processes and two adiabatic (no heat exchange) processes. These processes can be visualized on a Pressure-Volume (P-V) diagram and a Temperature-Entropy (T-S) diagram. Processes of the Carnot Cycle Isothermal Expansion (A to B) : The gas undergoes isothermal expansion at the high temperature T H T_H T H . Heat Q H Q_H Q H is absorbed from the high-temperature reservoir...