Cykl Carnota

According to the Second Law of Thermodynamics, no heat engine can convert all absorbed heat into work. Work is lost as heat in all irreversible processes. Since heat flow through a finite temperature drop is inherently irreversible, some energy must always be rejected to the cold reservoir, making perfect efficiency impossible.

Sadi Carnot developed a hypothetical heat engine cycle to determine the maximum theoretical efficiency of any heat engine. The Carnot cycle operates between two temperature reservoirs and uses only reversible processes: isothermal expansion and compression, plus adiabatic expansion and compression. This idealized cycle establishes the theoretical efficiency limit for all real heat engines.

The Carnot cycle consists of four stages: isothermal expansion where the gas absorbs heat from a hot reservoir, adiabatic expansion where temperature drops to match the cold reservoir, isothermal compression where heat is rejected to the cold reservoir, and adiabatic compression returning the gas to its initial state. Each stage is reversible and involves an ideal gas.

Isothermal heat exchange occurs at constant temperature, eliminating temperature drops that cause irreversibility. Adiabatic processes change temperature without heat transfer, avoiding irreversible heat flow. By combining these reversible processes, the Carnot cycle minimizes energy loss and achieves the maximum possible efficiency for any heat engine operating between two temperature reservoirs.

Heat flow through a finite temperature difference is an irreversible process that wastes energy. To maximize efficiency, the Carnot cycle requires heat exchange to occur isothermally, meaning at constant temperature. This eliminates the temperature gradient that causes irreversibility, allowing the engine to extract maximum work from the heat absorbed.

The Carnot cycle assumes the working fluid is an ideal gas. This simplification allows the cycle to be analyzed theoretically and provides a benchmark for comparing real heat engine performance. The ideal gas assumption enables precise calculation of the maximum theoretical efficiency achievable between any two temperature reservoirs.

The Carnot cycle operates between only two temperature reservoirs and follows the Second Law of Thermodynamics. This unique property allows the cycle to define an absolute temperature scale that is independent of any specific substance used for measurement, providing a universal standard for temperature that applies to all materials.