The Clapeyron equation can be simplified for liquid–vapor and solid–vapor
phase changes by utilizing some approximations. At low pressures vg vf,
and thus vfgvg. By treating the vapor as an ideal gas, we have vgRT/P.
Substituting these approximations into Eq. 12–22, we find
or
For small temperature intervals hfgcan be treated as a constant at some aver-
age value. Then integrating this equation between two saturation states yields
(12–24)
This equation is called the Clapeyron–Clausius equation,and it can be
used to determine the variation of saturation pressure with temperature. It
can also be used in the solid–vapor region by replacing hfg by hig (the
enthalpy of sublimation) of the substance.
lna
P 2
P 1
b
sat
hfg
R
a
1
T 1
1
T 2
b
sat
a
dP
P
b
sat
hfg
R
a
dT
T^2
b
sat
a
dP
dT
b
sat
Phfg
RT^2
660 | Thermodynamics
where, from Table A–11,
since T(°C) T(K). Substituting, we get
The tabulated value of hfgat 20°C is 182.27 kJ/kg. The small difference
between the two values is due to the approximation used in determining the
slope of the saturation curve at 20°C.
182.40 kJ/kg
hfg 1 293.15 K 21 0.035153 m^3 >kg 21 17.70 kPa>K2a
1 kJ
1 kPa#m^3
b
646.18504.58 kPa
8°C
17.70 kPa>K
a
dP
d T
b
sat,20°C
a
¢P
¢T
b
sat,20°C
Psat @ 24°CPsat @ 16°C
24°C16°C
vfg 1 vgvf (^2) @ 20°C0.0359690.00081610.035153 m^3 >kg
EXAMPLE 12–6 Extrapolating Tabular Data
with the Clapeyron Equation
Estimate the saturation pressure of refrigerant-134a at 50°F, using the
data available in the refrigerant tables.
Solution The saturation pressure of refrigerant-134a is to be determined
using other tabulated data.
Analysis Table A–11E lists saturation data at temperatures 40°F and
above. Therefore, we should either resort to other sources or use extrapolation