Novel Helmholtz resonator used to focus acoustic energy of thermoacoustic engine

A thermoacoustic engine (TE) converts thermal energy into acoustic power without any mechanical moving parts. It shows several advantages over traditional engines, such as simple configuration, stable operation, and environment-friendly working gas. In order to further improve the performance of a thermoacoustically driven system, methods are needed to focus the acoustic energy of a TE to its load. By theoretical analysis based on linear thermoacoustics, a novel Helmholtz resonator is proposed to increase the transmission ability of a TE, which makes full use of the interaction between inertance and compliance effects. With this configuration, the output pressure amplitude of a TE is amplified and the maximal pressure amplitude can occur at the end of the Helmholtz resonator tube with a length much shorter than 1/4 wavelength. Furthermore, the Helmholtz resonator has shown remarkably increased volume flow rates at both ends. In experiments, a Helmholtz resonator amplifies the pressure ratio from 1.22 to 1.49 and produces pressure amplitude of 0.44 MPa with nitrogen of 2.2 MPa as working gas. Relatively good agreements are obtained between computational and experimental results. This research is instructive for comprehensively understanding the transmission characteristics of acoustic components.

[1]  Iljae Lee,et al.  Helmholtz resonator with extended neck. , 2001, The Journal of the Acoustical Society of America.

[2]  Chen Ping,et al.  Effect of pressure disturbance on onset processes in thermoacoustic engine , 2006 .

[3]  Emmanuel C. Nsofor,et al.  Experimental study on the heat transfer at the heat exchanger of the thermoacoustic refrigerating system , 2007 .

[4]  W. Dai,et al.  A Heat-driven thermoacoustic cooler capable of reaching liquid nitrogen temperature , 2005 .

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

[6]  Zhihua Gan,et al.  Investigation on a thermoacoustically driven pulse tube cooler working at 80 K , 2005 .

[7]  Ercang Luo,et al.  An acoustical pump capable of significantly increasing pressure ratio of thermoacoustic heat engines , 2006 .

[8]  Shiu-keung Tang,et al.  On Helmholtz resonators with tapered necks , 2005 .

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

[10]  G. Swift Thermoacoustics: A Unifying Perspective for Some Engines and Refrigerators , 2017 .

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

[12]  Tetsushi Biwa,et al.  Experimental demonstration of thermoacoustic energy conversion in a resonator. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[13]  T. Greenslade Experiments with Helmholtz resonators , 1996 .

[14]  Guobang Chen,et al.  Investigation on Gedeon Streaming in a Traveling Wave Thermoacoustic Engine , 2006 .

[15]  Gregory W. Swift,et al.  Simple harmonic analysis of regenerators , 1996 .

[16]  Gregory W. Swift,et al.  DESIGN ENVIRONMENT FOR LOW-AMPLITUDE THERMOACOUSTIC ENGINES , 1994 .

[17]  Guobang Chen,et al.  Investigation on traveling wave thermoacoustic heat engine with high pressure amplitude , 2005 .

[18]  Guobang Chen,et al.  Thermoacoustically driven pulse tube refrigeration below 80K by introducing an acoustic pressure amplifier , 2006 .

[19]  Gregory W. Swift,et al.  Analysis and performance of a large thermoacoustic engine , 1992 .