Page 132 - DJJ20063- Thermodynamics 1
P. 132
DJJ20063- Thermodynamics 1
Often C1 is negligible compared with C2. In this case the equation becomes
C 2
+
0 = m (h − h ) 2
2 1 2
C 2
or 2 = (h − h 2 )
1
2
or C = ( 2 h − h 2 ) (3.30)
1
2
Example 3.8
Fluid with a specific enthalpy of 2800 kJ/kg enters a horizontal nozzle with negligible
velocity at the rate of 14 kg/s. At the outlet from the nozzle the specific enthalpy and
3
specific volume of the fluid are 2250 kJ/kg and 1.25 m /kg respectively. Assuming an
adiabatic flow, determine the required outlet area of the nozzle.
Solution to Example 3.8
The steady flow energy equation gives
C 2 −C 2
+
Q −W = m (h 2 − h 1 ) 2 1 ( + gZ 2 − gZ 1 )
2
When applied to the nozzle, this becomes
C 2 −C 2
+
h
0 = m ( − h 1 ) 2 1
2
2
Since the inlet C1 is negligible, this may be written as
2
C = ( 2 h − h )
2 1 2
C2 = √ [2(2800 – 22500]
= √ 1100
= 33.167 m/s
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