Abstract

The Carnot cycle is a prototype of ideal heat engine to draw mechanical energy from the heat flux between two thermal baths with the maximum efficiency, dubbed as the Carnot efficiency ηCη_{\mathrm{C}}. Such efficiency can only be reached by thermodynamical equilibrium processes with infinite time, accompanied unavoidably with vanishing power - energy output per unit time. In real-world applications, the quest to acquire high power leads to an open question whether a fundamental maximum efficiency exists for finite-time heat engines with given power. We experimentally implement a finite-time Carnot cycle with sealed dry air as working substance and verify the existence of a tradeoff relation between power and efficiency. Efficiency up to (0.524±0.034)ηC(0.524\pm0.034)η_{\mathrm{C}} is reached for the engine to generate the maximum power, consistent with the theoretical prediction ηC/2η_{\mathrm{C}}/2. Our results shall provide a new platform for studying finite-time thermodynamics consisting of nonequilibrium processes.

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