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178 ENGINEERING THERMODYNAMICS

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Water
out
h = 192 kJ/kg 2

h = 240 kJ/kg
Water in

1

2

1

20 m
(Z – Z )

21

Boundary

Q

Fig. 4.53

Q = (h 2 – h 1 ) +
CC 22 12
2

F −
HG

I
KJ
+ (Z 2 – Z 1 ) g + W

Here W = 0 (no pumps)
CC 22 12
2


= 0 (given)

∴ Q = (192 – 240) + 20 9 81 1000 ×. = – 47.8 kJ/kg
∴ Heat transfer from water/kg = 47.8 kJ/kg. (Ans.)
Example 4.47. The gas leaving the turbine of a gas turbine jet engine flows steadily into
the engine jet pipe at a temperature of 900°C, a pressure of 2 bar and a velocity of 300 m/s relative
to the pipe. Gas leaves the pipe at a temperature of 820°C and a pressure of 1.1 bar. Heat transfer
from the gas is negligible. Using the following data evaluate the relative velocity of gas leaving
the jet pipe. For the gas at t = 820°C, h = 800 kJ/kg and at 910°C, 915 kJ/kg.
Solution. Pressure at entry to the engine jet pipe, p 1 = 2 bar
Velocity relative to the pipe, C 1 = 300 m/s
Heat transfer from gas, Q = 0
At temperature, t 1 = 910°C, h 1 = 915 kJ/kg
At temperature, t 2 = 820°C, h 2 = 800 kJ/kg
Relative velocity of gas leaving the jet pipe, C 2 :
Steady flow energy equation is given by :


h 1 +
C 12
2 + Z^1 g + Q = h^2 +

C 22
2 + Z^2 g + W
Q = 0
W = 0
Z 1 = Z 2 (assumed)

h 1 + C^1

2
2 = h^2 +

C 22
2
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