A pistonless Stirling engine—A new direction in thermoacoustics
Scott Backhaus, Gregory W. Swift
Abstract
Scott Backhaus, Gregory W. Swift
Abstract
Due to its thermodynamic reversibility, the Stirling cycle has an inherent advantage in thermal efficiency over the standard, irreversible standing-wave thermoacoustic cycle. The main disadvantage of the Stirling cycle has been the need for high-pressure, sliding piston seals. Building significantly on the ideas of Ceperley [J. Acoust. Soc. Am. 66, 1508 (1979)], a thermoacoustic version of a 1-kW Stirling engine has been constructed and tested. This engine enjoys both the efficiency advantage of the Stirling cycle and the no-moving-parts advantage of thermoacoustics. In this first attempt, experimental data show that the engine has an efficiency above 35% of the Carnot efficiency, much higher than that of any prior thermoacoustic engine. [Work supported by the Office of Basic Energy Sciences in the U.S. DOE.]
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Due to its thermodynamic reversibility, the Stirling cycle has an inherent advantage in thermal efficiency over the standard, irreversible standing-wave thermoacoustic cycle. The main disadvantage of the Stirling cycle has been the need for high-pressure, sliding piston seals. Building significantly on the ideas of Ceperley [J. Acoust. Soc. Am. 66, 1508 (1979)], a thermoacoustic version of a 1-kW Stirling engine has been constructed and tested. This engine enjoys both the efficiency advantage of the Stirling cycle and the no-moving-parts advantage of thermoacoustics. In this first attempt, experimental data show that the engine has an efficiency above 35% of the Carnot efficiency, much higher than that of any prior thermoacoustic engine. [Work supported by the Office of Basic Energy Sciences in the U.S. DOE.]
Key concepts: Stirling engine, Thermoacoustics, Carnot cycle, Stirling cycle, Thermoacoustic heat engine, Thermal efficiency, Piston (optics), Thermodynamic cycle