Performance optimization of tunable standing wave thermoacoustic engine by varying the stack parameters and resonator length: An experimental study

Author(s):  
Harshal Agarwal ◽  
Akhil K T ◽  
Vishnu R Unni ◽  
N T Ravi ◽  
R I Sujith ◽  
...  
2018 ◽  
Author(s):  
Rinasa Agistya Anugrah ◽  
Adhika Widyaparaga ◽  
I. Made Miasa ◽  
Joko Waluyo ◽  
Sugiyanto ◽  
...  

2018 ◽  
Author(s):  
Franido Prihandoto ◽  
Adhika Widyaparaga ◽  
Joko Waluyo ◽  
Samsul Kamal ◽  
Sugiyanto

2010 ◽  
Author(s):  
Dongwei Zhang ◽  
Yaling He ◽  
Yong Wang ◽  
Jing Huang ◽  
Liejin Guo ◽  
...  

2012 ◽  
Author(s):  
Xin Huang ◽  
Gang Zhou ◽  
Qing Li ◽  
Zhongjun Hu

2018 ◽  
Vol 55 (3) ◽  
pp. 877-890 ◽  
Author(s):  
A. C. Alcock ◽  
L. K. Tartibu ◽  
T. C. Jen

2008 ◽  
Vol 123 (5) ◽  
pp. 3543-3543
Author(s):  
Wei Dai ◽  
Bo Yu ◽  
Guoyao Yu ◽  
Ercang Luo

Author(s):  
Ho-Yun Nam ◽  
Byoung-Hae Choi ◽  
Jong-Man Kim ◽  
Byung-Ho Kim

An experimental study has been performed to investigate the frequency of a free surface fluctuation in a vessel with and without an internal structure. Water flows in from the bottom nozzle and flows out at the side wall nozzles. There are two dominant frequency regions which are generated by a standing wave and a jet. In the standing wave region, the frequency is well described by f(4πdV/g)1/2 = 1.07 in a circular vessel. The frequency generated by a jet can be described by a dimensionless period and Froude number according to its fluctuation stability. In the case of a vessel with an internal structure, it needs a geometry factor which is described by a vessel diameter to a hydraulic diameter ratio in a standing wave region.


2013 ◽  
Vol 712-715 ◽  
pp. 1609-1613 ◽  
Author(s):  
Jie Lin ◽  
Feng Wu ◽  
Jin Hua Fei ◽  
Tuo Wang

The relationship between exergy efficiency and output acoustic power of the thermoacoustic engine microcycle model which only was accounted for the heat resistance had been analyzed using finite time thermodynamics.And through the new objective function,we obtain the optimization that not only obtain high exergy efficiency but also high output acoustic power at the same time.Optimized imperfection that we only pursue the high exergy efficiency, we obtain low output acoustic power and vice versa.We approve this conclusion by numerical calculation.The results that we obtained will be useful to optimal the design of a actual thermoacoustic engine.


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