The document presents information on the Carnot cycle, a theoretical thermodynamic cycle proposed by Sadi Carnot in 1824. The Carnot cycle consists of four reversible processes involving two isothermal and two adiabatic steps using a perfect gas as a working substance between a heat source and heat sink. The efficiency of the Carnot cycle depends only on the temperature range and provides the maximum possible efficiency for converting heat into work in a thermodynamic cycle. However, the Carnot cycle is impossible to implement in practice due to assumptions of frictionless, infinitely slow isothermal processes and infinitely fast adiabatic processes.