Table 5 Physical characteristics of R290, R32 and R410A at the saturation temperature of 50 \(^\circ {\text{C}}\).

From: Reliable smart models for estimating frictional pressure drop in two-phase condensation through smooth channels of varying sizes

Fluids

\(T_{s} \left( {{^\circ }{\text{C}}} \right)\)

\(\rho_{l} \left( {kg m^{ - 3} } \right)\)

\(\rho_{v} \left( {kg m^{ - 3} } \right)\)

\(\nu_{l} \left( {cm^{2} s^{ - 1} } \right)\)

\(\nu_{v} \left( {cm^{2} s^{ - 1} } \right)\)

R290

50

448.87

38.63

0.0016501

0.0024336

R32

50

839.26

98.55

0.00099156

0.0014935

R410A

50

906.80

141.14

0.00090202

0.0014406