342 | Thermodynamics
EXAMPLE 7–4 Entropy Change during a Constant-Pressure
Process
A piston–cylinder device initially contains 3 lbm of liquid water at 20 psia
and 70°F. The water is now heated at constant pressure by the addition of
3450 Btu of heat. Determine the entropy change of the water during this
process.
Solution Liquid water in a piston–cylinder device is heated at constant
pressure. The entropy change of water is to be determined.
Assumptions 1 The tank is stationary and thus the kinetic and potential
energy changes are zero, KE PE 0. 2 The process is quasi-equilibrium.
3 The pressure remains constant during the process and thus P 2 P 1.
Analysis We take the water in the cylinder as the system(Fig. 7–13). This is
a closed systemsince no mass crosses the system boundary during the
process. We note that a piston–cylinder device typically involves a moving
boundary and thus boundary work Wb. Also, heat is transferred to the system.
Water exists as a compressed liquid at the initial state since its pressure is
greater than the saturation pressure of 0.3632 psia at 70°F. By approximat-
ing the compressed liquid as a saturated liquid at the given temperature, the
properties at the initial state are
State 1:
At the final state, the pressure is still 20 psia, but we need one more prop-
erty to fix the state. This property is determined from the energy balance,
Net energy transfer Change in internal, kinetic,
by heat, work, and mass potential, etc., energies
since UWbHfor a constant-pressure quasi-equilibrium process. Then,
State 2:
P 2 20 psia
h 2 1188.1 Btu>lbm
f¬
s 2 1.7761 Btu>lbm#R
1 Table A-6E, interpolation 2
h 2 1188.1 Btu>lbm
3450 Btu 1 3 lbm 21 h 2 38.08 Btu>lbm 2
Qin¢Hm 1 h 2 h 12
QinWb¢U
EinEout¬
¬
¢Esystem
P 1 20 psia
T 1 70°F
f¬
s 1 sf @ 70°F0.07459 Btu>lbm#R
h 1 hf @ 70°F38.08 Btu>lbm
T
s 1 s
1
2
s 2
P = const.
Qin P 1 = 20 psia
H 2 O
T 1 = 70°F
FIGURE 7–13
Schematic and T-sdiagram for
Example 7–4.
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