Affiliation:
1. Sivas Cumhuriyet Üniversitesi
2. Dikçal Makina İmalat San.Tic.Ltd.Şti
3. KOCAELİ ÜNİVERSİTESİ, KARAMÜRSEL MESLEK YÜKSEKOKULU, TEKNİK PROGRAMLAR BÖLÜMÜ, MEKATRONİK PR.
Abstract
In this study, a simple thermoacoustic refrigerator system experiment set was established by using the design parameters in accordance with the relevant literature. In the experimental setup, a loudspeaker was used as acoustic power source and a suitable frequency value was determined for the system. Three kinds of stack materials with different thermal conductivity coefficients, respectively, mylar, cotton and glass wool were placed in the resonance tube. The temperature values at both ends of the stack material were measured by placed temperature gauges. In the measurements made within the same time period, the temperature differences were measured as 5.2°C for mylar, 4.7°C for cotton and 4.3°C for glass wool, respectively. It was determined that the highest temperature difference was in the mylar material.
Publisher
Bitlis Eren Universitesi Fen Bilimleri Dergisi
Reference26 articles.
1. [1] J. Chi, J. Xu, L. Zhang, Z. Wu, J. Hu, and E. Luo, “Study of a gas-liquid-coupled heat-driven room-temperature thermoacoustic refrigerator with different working gases”, Energy Conversion and Management, vol. 246, p. 114657, Oct. 2021, doi: 10.1016/j.enconman.2021.114657.
2. [2] P. A. Habibbhai, M. Yadav, and K. Nagori, “Experimental analysis of thermoacoustic refrigeration with combination of different gases and stack material”, International Research Journal of Engineering and Technology vol. 05, no. 04, Apr-2018
3. [3] N. Rott, “Thermoacoustics”, Advanced in Applied Mechanics, 20, pp.135-174,1980.
4. [4] G. Swift, “Thermoacoustic engines”, Journal Acoustical Society of America, 84, pp.1145-1180,1988
5. [5] J. Wheatley, G.W. Swift, T. Hofler, ‘Heat-Driven Acoustic Cooling Engine Having No Moving Parts’, The Journal of the Acoustical Society of America., vol.88, no. 4, pp. 2046-2048, 1990.