CHAP. 6: THERMODYNAMICS OF HOMOGENEOUS MIXTURES [CONTENTS] 162
S Symbols: The values of thermodynamic quantities in the standard state of an ideal gas at the
standard pressure are denoted using the superscript◦, e.g.Hm◦,i, Sm◦,i,···.
The values of thermodynamic quantities in the standard state of a pure component at the
temperature and pressure of the system are denoted using the superscript•, e.g.Hm•,i, Sm•,i,···.
The values of thermodynamic quantities in the standard state of a hypothetical pure sub-
stance at infinite dilution will be denoted using the superscript[x], e.g.Hm[x,i], Sm[x,i],···.
The values of thermodynamic quantities in the standard state of a unit molar concentration
will be denoted using the superscript[c], e.g.Hm[c],i, S[mc],i,···.
The values of thermodynamic quantities in the standard state of unit molality will be
denoted using the superscript[m], e.g.Hm[m,i], Sm[m,i],···.
Note:For the activity and the activity coefficients, however, symbolsa[ix],a[ic],a[im],γ[ 1 x],
γ[ic],γ[im]are used in a different meaning [see6.5.4,6.5.5].
Figure6.3illustrates the standard values of enthalpy of component 1 in a binary mixture.
6.5.4 Activity
The activity of theithcomponent in a mixture is defined by the relation
ai=
fi
fist
, (6.89)
wherefistis the fugacity in the chosen standard state [see6.1.2].
U Main unit:dimensionless quantity.
An alternative definition of activity follows from the relation for fugacity (6.74)
ai= exp
(
μi−μsti
RT
)
= exp
(
Gi−Gstm,i
RT
)
. (6.90)
- The dependence of activity on temperature is expressed by the relation
lnai(T 2 ) = lnai(T 1 ) +
∫T 2
T 1
(
∂lnai
∂T
)
p,n
dT , (6.91)