Experimental studies of a thermoacoustic Stirling prime mover and its application to a cooler

An acoustic field spontaneously induced in a thermoacoustic prime mover consisting of a looped tube and resonator is determined through simultaneously measurements of pressure P and velocity U. A thermal efficiency of the thermoacoustic prime mover of this type has been reported to reach 30%. The measurements of the acoustic field in the present system revealed that a phase lead of U relative to P takes a negative value of about −20° in the regenerator where the output power of the prime mover is generated. It was concluded that the possession of a negative phase lead at this position is taken as a clue in a significant increase in the output power. Moreover, the analysis in the thermoacoustic mechanism shows that a precise position for the location of a second regenerator acting as a heat pump exists in the looped tube. Indeed, by locating the second regenerator at the position, a thermoacoustic cooler was constructed. The thermoacoustic cooler could generate a low temperature of −25 °C without involving any moving parts.

[1]  G. W. Swift,et al.  An intrinsically irreversible thermoacoustic heat engine , 1983 .

[2]  R. Radebaugh Development of a thermoacoustically driven orifice pulse tube refrigerator , 1990 .

[3]  Taichi Yazaki,et al.  Measurement of sound generation in thermoacoustic oscillations , 1998, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[4]  G. W. Swift,et al.  Understanding some simple phenomena in thermoacoustics with applications to acoustical heat engines , 1985 .

[5]  R Raspet,et al.  Working gases in thermoacoustic engines. , 1999, The Journal of the Acoustical Society of America.

[6]  A. Atchley Analysis of the initial buildup of oscillations in a thermoacoustic prime mover , 1994 .

[7]  Tetsushi Biwa,et al.  Work flow measurements in a thermoacoustic engine , 2001 .

[8]  Tetsushi Biwa,et al.  Thermodynamical mode selection rule observed in thermoacoustic oscillations , 2002 .

[9]  Tetsushi Biwa,et al.  A pistonless Stirling cooler , 2002 .

[10]  Anthony A. Atchley,et al.  Stability curves for a thermoacoustic prime mover , 1993 .

[11]  Steven L. Garrett Reinventing the engine , 1999, Nature.

[12]  Akira Tominaga,et al.  Thermodynamic aspects of thermoacoustic theory , 1995 .

[13]  Peter H. Ceperley,et al.  A pistonless Stirling engine—The traveling wave heat engine , 1979 .

[14]  T. Biwa,et al.  Acoustic field in a thermoacoustic Stirling engine having a looped tube and resonator , 2002 .

[15]  G. Swift,et al.  A thermoacoustic-Stirling heat engine: detailed study , 2000, The Journal of the Acoustical Society of America.

[16]  G. Swift,et al.  Experiments with an Intrinsically Irreversible Acoustic Heat Engine , 1983 .

[17]  T. Yazaki,et al.  TRAVELING WAVE THERMOACOUSTIC ENGINE IN A LOOPED TUBE , 1998 .

[18]  G. Swift,et al.  A thermoacoustic Stirling heat engine , 1999, Nature.

[19]  W. P. Arnott,et al.  Thermoacoustic engines , 1991, IEEE 1991 Ultrasonics Symposium,.

[20]  Gregory W. Swift Thermoacoustic Engines and Refrigerators , 1995 .