
R-134a is accelerated in a nozzle from a velocity of 20 m/s. The exit velocity of the refrigerant and the ratio of the inlet to exit area of the nozzle are to be determined.
Assumptions:
- This is a steady-flow process since there is no change with time.
- Potential energy changes are negligible.
- There are no work interactions.
- The device is adiabatic and thus heat transfer is negligible.
Properties: From the refrigerant tables (Table A-13)

Analysis:
(a) There is only one inlet and one exit, and thus \(\overset •m_1 = \overset •m_2 = \overset •m\). We take nozzle as the system, which is a control volume since mass crosses the boundary. The energy balance for this steady-flow system can be expressed in the rate form as

(b) The ratio of the inlet to exit area is determined from the conservation of mass relation,
