6.2 Isobaric Cooling and Condensation of R134a 2 kg of superheated R134a at p₁ = 1 MPa, T₁ = 70°C undergo an isobaric cooling process to saturated vapor (state 2), saturated liquid (state 3) to compressed liquid state at T4 = 24°C. Determine temperature, pressure, specific volume, internal energy, enthalpy and entropy in the four states; collect the data in a table. Then determine the work and the heat for the process. Use the tables on pages 19-22 of our booklet. There is no compressed liquid table available, hence for state 4 use the approximation based on saturation data.

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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For all problems, draw p-v- and a T-s-diagrams indicating states and processes relative to
saturation lines.

6.2 Isobaric Cooling and Condensation of R134a
2 kg of superheated R134a at p₁ = 1 MPa, T₁ = 70°C undergo an isobaric cooling process to saturated
vapor (state 2), saturated liquid (state 3) to compressed liquid state at T₁ = 24°C.
Determine temperature, pressure, specific volume, internal energy, enthalpy and entropy in the four
states; collect the data in a table. Then determine the work and the heat for the process.
Use the tables on pages 19-22 of our booklet. There is no compressed liquid table available, hence for state 4 use the
approximation based on saturation data.
Transcribed Image Text:6.2 Isobaric Cooling and Condensation of R134a 2 kg of superheated R134a at p₁ = 1 MPa, T₁ = 70°C undergo an isobaric cooling process to saturated vapor (state 2), saturated liquid (state 3) to compressed liquid state at T₁ = 24°C. Determine temperature, pressure, specific volume, internal energy, enthalpy and entropy in the four states; collect the data in a table. Then determine the work and the heat for the process. Use the tables on pages 19-22 of our booklet. There is no compressed liquid table available, hence for state 4 use the approximation based on saturation data.
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