708 | Thermodynamics
A mixture of two or more gases of fixed chemical composi-
tion is called a nonreacting gas mixtureThe composition of a
gas mixture is described by specifying either the mole frac-
tionor the mass fractionof each component, defined as
where
The apparent(or average) molar massand gas constantof a
mixture are expressed as
Also,
Dalton’s law of additive pressuresstates that the pressure
of a gas mixture is equal to the sum of the pressures each gas
would exert if it existed alone at the mixture temperature and
volume. Amagat’s law of additive volumesstates that the vol-
ume of a gas mixture is equal to the sum of the volumes each
gas would occupy if it existed alone at the mixture tempera-
ture and pressure. Dalton’s and Amagat’s laws hold exactly
for ideal-gas mixtures, but only approximately for real-gas
mixtures. They can be expressed as
Dalton’s law:
Amagat’s law:
Here Piis called the component pressureand Viis called
the component volume. Also, the ratio Pi/Pmis called the
pressure fractionand the ratio Vi/Vmis called the volume
fractionof component i. For ideal gases,Piand Vican be
related to yiby
The quantity yiPmis called the partial pressureand the quan-
tity yiVmis called the partial volume. The P-v-Tbehavior
of real-gas mixtures can be predicted by using generalized
Pi
Pm
Vi
Vm
Ni
Nm
yi
Vma
k
i 1
Vi 1 Tm, Pm 2
Pma
k
i 1
Pi 1 Tm, Vm 2
mfiyi
Mi
Mm
¬and¬Mm
1
a
k
i 1
mfi
Mi
Mm
mm
Nm
a
k
i 1
yiMi¬and¬Rm
Ru
Mm
mma
k
i 1
mi¬and¬Nma
k
i 1
Ni
mfi
mi
mm
¬and¬yi
Ni
Nm
SUMMARY
compressibility charts. The compressibility factor of the mix-
ture can be expressed in terms of the compressibility factors
of the individual gases as
where Ziis determined either at Tmand Vm(Dalton’s law) or at
Tmand Pm(Amagat’s law) for each individual gas. The P-v-T
behavior of a gas mixture can also be predicted approximately
by Kay’s rule,which involves treating a gas mixture as a pure
substance with pseudocritical properties determined from
The extensive propertiesof a gas mixture, in general, can
be determined by summing the contributions of each compo-
nent of the mixture. The evaluation of intensive propertiesof
a gas mixture, however, involves averaging in terms of mass
or mole fractions:
and
These relations are exact for ideal-gas mixtures and approxi-
mate for real-gas mixtures. The properties or property changes
of individual components can be determined by using ideal-
gas or real-gas relations developed in earlier chapters.
cp,ma
k
i 1
mficp,i¬and¬cp,ma
k
i 1
yicp,i
cv,ma
k
i 1
mficv,i¬and¬cv,ma
k
i 1
yicv,i
sma
k
i 1
mfisi¬and¬sma
k
i 1
yisi
hma
k
i 1
mfihi¬and¬hma
k
i 1
yihi
uma
k
i 1
mfiui¬and¬uma
k
i 1
yiui
Sma
k
i 1
Sia
k
i 1
mi sia
k
i 1
Nisi
Hma
k
i 1
Hia
k
i 1
mihia
k
i 1
Nihi
Uma
k
i 1
Uia
k
i 1
miuia
k
i 1
Niui
P¿cr,ma
k
i 1
yi Pcr,i¬and¬T¿cr,m (^) a
k
i 1
yi Tcr,i
Zma
k
i 1
yi Zi
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