Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis

The Raque Hilsch Vortex Tube (RHVT) is a heat pump system that uses the phenomenon of compressed vortex airflow in a tube for cooling and heating. This study aims to determine the effect of pressure and fraction on RHVT by cooling the surface of the hot tube naturally and forcefully. Tube type testi...

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Main Authors: Alfan Sarifudin, Nugroho Agung Pambudi, Danar Susilo Wijayanto, Indah Widiastuti
Format: Article
Language:English
Published: Elsevier 2020-12-01
Series:Case Studies in Thermal Engineering
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2214157X20304810
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author Alfan Sarifudin
Nugroho Agung Pambudi
Danar Susilo Wijayanto
Indah Widiastuti
author_facet Alfan Sarifudin
Nugroho Agung Pambudi
Danar Susilo Wijayanto
Indah Widiastuti
author_sort Alfan Sarifudin
collection DOAJ
description The Raque Hilsch Vortex Tube (RHVT) is a heat pump system that uses the phenomenon of compressed vortex airflow in a tube for cooling and heating. This study aims to determine the effect of pressure and fraction on RHVT by cooling the surface of the hot tube naturally and forcefully. Tube type testing was conducted with a pressure variation of 0.5–1.5 bar and a fraction of 30%–70%. The results of the analysis show that forced cooling on the surface of the hot tube decreases the heating performance (Th, ΔTh, Q˙h, ηish, and COPh) and improves the cooling performance (Tc, ΔTc, Q˙c, ηisc and COPref). The higher pressure increases the performance of Th ΔTh, Q˙h, Tc ΔTc, and Q˙c, and decrease the performance of ηish, COPh, ηisc, and COPref. The fraction 40% is the most optimal parameter for the performance of Tc ΔTc, Q˙c. The 60% fraction works best for Th, ΔTh, Q˙h, ηish, and COPh, while the fraction 70% works best for Q˙c and COPref. The most optimal performance values include Th (41 °C), ΔTh (14 °C), Q˙h (2.369kJ/s), ηish(24.21%), COPh (0.092), Tc (13.450 °C), ΔTc (13.550 °C), Q˙c (3.280kJ/s), ηisc (20.84%), and COPref (0.123).
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spelling doaj.art-0e343e15acb94738a12e3b1866edddfb2022-12-21T23:17:20ZengElsevierCase Studies in Thermal Engineering2214-157X2020-12-0122100739Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysisAlfan Sarifudin0Nugroho Agung Pambudi1Danar Susilo Wijayanto2Indah Widiastuti3Corresponding author.; Department of Mechanical Engineering Education, Universitas Sebelas Maret, Sutami No.36 A Road, Pucangsawit, Jebres, Surakarta City, Central Java Province, 57126, IndonesiaCorresponding author.; Department of Mechanical Engineering Education, Universitas Sebelas Maret, Sutami No.36 A Road, Pucangsawit, Jebres, Surakarta City, Central Java Province, 57126, IndonesiaDepartment of Mechanical Engineering Education, Universitas Sebelas Maret, Sutami No.36 A Road, Pucangsawit, Jebres, Surakarta City, Central Java Province, 57126, IndonesiaDepartment of Mechanical Engineering Education, Universitas Sebelas Maret, Sutami No.36 A Road, Pucangsawit, Jebres, Surakarta City, Central Java Province, 57126, IndonesiaThe Raque Hilsch Vortex Tube (RHVT) is a heat pump system that uses the phenomenon of compressed vortex airflow in a tube for cooling and heating. This study aims to determine the effect of pressure and fraction on RHVT by cooling the surface of the hot tube naturally and forcefully. Tube type testing was conducted with a pressure variation of 0.5–1.5 bar and a fraction of 30%–70%. The results of the analysis show that forced cooling on the surface of the hot tube decreases the heating performance (Th, ΔTh, Q˙h, ηish, and COPh) and improves the cooling performance (Tc, ΔTc, Q˙c, ηisc and COPref). The higher pressure increases the performance of Th ΔTh, Q˙h, Tc ΔTc, and Q˙c, and decrease the performance of ηish, COPh, ηisc, and COPref. The fraction 40% is the most optimal parameter for the performance of Tc ΔTc, Q˙c. The 60% fraction works best for Th, ΔTh, Q˙h, ηish, and COPh, while the fraction 70% works best for Q˙c and COPref. The most optimal performance values include Th (41 °C), ΔTh (14 °C), Q˙h (2.369kJ/s), ηish(24.21%), COPh (0.092), Tc (13.450 °C), ΔTc (13.550 °C), Q˙c (3.280kJ/s), ηisc (20.84%), and COPref (0.123).http://www.sciencedirect.com/science/article/pii/S2214157X20304810Coefficient of the performance (COP)ExperimentHeat flowIsentropic efficiencyMathematical analysis
spellingShingle Alfan Sarifudin
Nugroho Agung Pambudi
Danar Susilo Wijayanto
Indah Widiastuti
Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis
Case Studies in Thermal Engineering
Coefficient of the performance (COP)
Experiment
Heat flow
Isentropic efficiency
Mathematical analysis
title Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis
title_full Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis
title_fullStr Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis
title_full_unstemmed Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis
title_short Investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis
title_sort investigation on cooling the hot tube surfaces of vortex tube at different pressure and fraction with comprehensive thermal performance analysis
topic Coefficient of the performance (COP)
Experiment
Heat flow
Isentropic efficiency
Mathematical analysis
url http://www.sciencedirect.com/science/article/pii/S2214157X20304810
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AT nugrohoagungpambudi investigationoncoolingthehottubesurfacesofvortextubeatdifferentpressureandfractionwithcomprehensivethermalperformanceanalysis
AT danarsusilowijayanto investigationoncoolingthehottubesurfacesofvortextubeatdifferentpressureandfractionwithcomprehensivethermalperformanceanalysis
AT indahwidiastuti investigationoncoolingthehottubesurfacesofvortextubeatdifferentpressureandfractionwithcomprehensivethermalperformanceanalysis