![]() ![]() ![]() Carnot's theorem įigure 6: A real engine (left) compared to the Carnot cycle (right). The P– V diagram of the reversed Carnot cycle is the same as for the Carnot heat-engine cycle except that the directions of the processes are reversed. ![]() Heat is absorbed from the low-temperature reservoir, heat is rejected to a high-temperature reservoir, and a work input is required to accomplish all this. This time, the cycle remains exactly the same except that the directions of any heat and work interactions are reversed. That is, all the processes that compose it can be reversed, in which case it becomes the Carnot heat pump and refrigeration cycle. This thermal energy is the cycle initiator.Ī Carnot heat-engine cycle described is a totally reversible cycle. This is the Carnot heat engine working efficiency definition as the fraction of the work done by the system to the thermal energy received by the system from the hot reservoir per cycle. In a Carnot cycle, a system or engine transfers energy in the form of heat between two thermal reservoirs at temperatures T H. By Carnot's theorem, it provides an upper limit on the efficiency of any classical thermodynamic engine during the conversion of heat into work, or conversely, the efficiency of a refrigeration system in creating a temperature difference through the application of work to the system. A Carnot cycle is an ideal thermodynamic cycle proposed by French physicist Sadi Carnot in 1824 and expanded upon by others in the 1830s and 1840s. ![]()
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