The thermodynamic efficiency limit of a Spark Ignition (SI) engine is primarily defined by the Carnot cycle, which represents the most efficient theoretical heat engine possible. The Carnot efficiency is determined solely by the temperatures of the hot and cold reservoirs between which the engine operates. In an SI engine, the hot reservoir is the high-temperature combustion gas, and the cold reservoir is the exhaust gas. The efficiency of the Carnot cycle is calculated as 1 minus the ratio of the cold reservoir temperature to the hot reservoir temperature (η_Carnot = 1 - T_cold / T_hot). A higher hot reservoir temperature and a lower cold reservoir temperature lead to a higher theoretical efficiency.
The actual SI engine cycle, known as the Otto cycle, is a simplified model of the SI engine's operation and provides a more practical theoretical efficiency limit than the Carnot cycle. The ideal Otto cycle consists of four processes: isentropic compression, constant volume heat addition (combustion), isentropic expansion, and constant volume heat rejection. The efficiency of an ideal Otto cycle depends direc....
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