4.7. In an ideal liquefaction system the gas to be liquefied is first compressed isothermally and reversibly from its initial state to a high pressure, whereupon the gas is expanded through a reversible adiabatic expander to the saturated-liquid condition. To what absolute pressure must nitrogen gas be compressed at the end of the isothermal compression assuming that the nitrogen gas obeys the relation pV= ZNRT, where Z is the compressibility factor? The nitrogen gas is initially available at 0.101 MPa and 300 K.

Elements Of Electromagnetics
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4.7. In an ideal liquefaction system the gas to be liquefied is first compressed isothermally and
reversibly from its initial state to a high pressure, whereupon the gas is expanded through
a reversible adiabatic expander to the saturated-liquid condition. To what absolute pressure
must nitrogen gas be compressed at the end of the isothermal compression assuming that
the nitrogen gas obeys the relation pV= ZNRT, where Z is the compressibility factor? The
nitrogen gas is initially available at 0.101 MPa and 300 K.
Transcribed Image Text:4.7. In an ideal liquefaction system the gas to be liquefied is first compressed isothermally and reversibly from its initial state to a high pressure, whereupon the gas is expanded through a reversible adiabatic expander to the saturated-liquid condition. To what absolute pressure must nitrogen gas be compressed at the end of the isothermal compression assuming that the nitrogen gas obeys the relation pV= ZNRT, where Z is the compressibility factor? The nitrogen gas is initially available at 0.101 MPa and 300 K.
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