Experimental investigation of mass flow rate difference between forward flow and reverse flow of sub-cooled R-22 through stepped short tube orifices
•The low cost stepped short tube orifice (SSTO) was firstly proposed.•The mass flow rates in opposite way of R-22 through SSTO are distinguishing.•11# SSTO has good two-way throttling characteristics. An expansion device of two capillary tubes with a by-pass check valve is popularly used in domestic...
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Veröffentlicht in: | Applied thermal engineering 2017-09, Vol.124, p.1292-1300 |
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Sprache: | eng |
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Zusammenfassung: | •The low cost stepped short tube orifice (SSTO) was firstly proposed.•The mass flow rates in opposite way of R-22 through SSTO are distinguishing.•11# SSTO has good two-way throttling characteristics.
An expansion device of two capillary tubes with a by-pass check valve is popularly used in domestic heat pump systems. In order to reduce the manufacturing cost and improve reliability of the heat pump systems, a stepped short tube orifice consisting of two serial-connected short tube orifices with different diameters is employed as an alternative. The effects of upstream pressure, downstream pressure, upstream degree of sub-cooling and the geometric sizes of stepped short tube orifices on mass flow rate difference between forward flow and reverse flow of R-22 through stepped short tube orifices were investigated in this study. The results showed that there was a distinguishing mass flow rate difference between forward flow and reverse flow of R-22 through stepped short tube orifices under upstream pressure ranged from 1460kPa to 1940kPa, downstream pressure ranged from 420kPa to 680kPa and degree of sub-cooling ranged from 2 to 12°C. The mass flow rate difference is about 10kg/h between forward flow and reverse flow of R-22 through the stepped short tube orifice with sizes of D1=0.8mm, D2=1.0mm, L1=3mm, L2=6.5mm at the upstream pressure of 1940kPa, downstream pressure of 500kPa and the degree of sub-cooling ranging between 2°C and 12°C. |
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ISSN: | 1359-4311 1873-5606 |
DOI: | 10.1016/j.applthermaleng.2017.06.118 |