THE THERMODYNAMIC CHARACTERISTICS OF ION EXCHANGE
1015
∆
S, J/(equiv K)
are shown in Fig. 4. We see that the entropy of the sys-
tem increases as the fraction of metal cations in the
polymer grows for both Na –H and Cu –H exchange
processes. This is in agreement with the model concept
of a decrease in polymer phase ordering as hydroxo-
nium ions are replaced by metal cations.
+
+
2+
+
2
0
0
0
2
1
To summarize, model considerations and the exper-
imental data obtained show that the type of the cation
sorbed and the structure and counterion polymer com-
position substantially influence the character and val-
ues of the thermodynamic functions of ion exchange
for the sulfonated polymer based on cis-tetraphenyl-
calix[4]resorcinarene.
1
–
–
10
20
REFERENCES
1
. H. Altshuler, E. Ostapova, O. Fedyaeva, et al., Macro-
mol. Symp. 181, 1 (2002).
2
. S. V. Bleshinskii and V. F. Abramova, Chemistry of
Indium (Akad. Nauk Kirg. SSR, Frunze, 1958) [in Rus-
sian].
0
0.2
0.4
0.6
0.8
1.0
Cat
x
3
. G. Schwarzenbach and H. Flaschka, Die komplexome-
trische Titration (F. Enke, Stuttgart, 1965; Khimiya,
Moscow, 1970).
+
+
Fig. 4. Differential entropy of exchange for the (1) Na –H
2
+
+
and (2) Cu –ç reactions in the sulfonated polymer based
on cis-tetraphenylcalix[4]resorcinarene at 293 K calculated
according to (4).
4. A. I. Busev, V. G. Tiptsova, and V. M. Ivanov, Practical
Manual on Analytical Chemistry of Rare Elements
(Khimiya, Moscow, 1996) [in Russian].
5
. M. Marhol, Ion Exchangers in Analytical Chemistry:
Their Properties and Use in Inorganic Chemistry, vol. 14
of Comprehensive Analytical Chemistry (Elsevier,
Amsterdam, 1982; Mir, Moscow, 1985).
exchange because the heats of mixing and the differ-
ence in heat content between 0.1 M solutions of NaCl
and HCl or 0.005 M solutions of CuCl and HCl are
2
smaller than measurement errors.
6
. Thermodynamic Properties of Pure Substances: A
Handbook, Ed. by L. V. Gurvich (Nauka, Moscow,
The standard thermodynamic functions of ion
exchange are strongly influenced by the difference in
the resolvation energies of the ions involved in
exchange [9]. The dependences of the differential ther-
modynamic functions of ion exchange on the counter-
ion polymer composition are determined by changes in
the interaction between the ions involved and ionogen
groups. Taking [11] into account, the differential Gibbs
1
982), Vol. 4, p. 486 [in Russian].
7
. R. A. Robinson and R. M. Stokes, Electrolyte Solutions:
The Measurement and Interpretation of Conductance,
Chemical Potential, and Diffusion in Solutions of Simple
Electrolytes, 2nd ed. (Academic, New York, 1959; Inos-
trannaya Literatura, Moscow, 1963).
8
9
. International Union of Pure and Applied Chemistry:
Commission on the Nomenclature of Organic Chemis-
try: Nomenclature of Organic Chemistry, 4th ed., Ed. by
J. Rigaudy and S. P. Klesney (Pergamon, Oxford, 1979;
VINITI, Moscow, 1979).
energy was calculated as ∆G = RT[(z – z ) –
H
Cat
a
lnk
]. The behavior of the ∆G (xCat/H) functions was
Cat/H
a
characterized by considering the logk
(x ) func-
Cat/H Cat
. Ion Exchange: Series of Advances, Ed. by J. Marinsky
tions plotted in Fig. 2. An increase in the differential
enthalpy of ion exchange as the content of metal cations
(New York, 1966; Mir, Moscow, 1968), Vol. 1.
in the polymer grows (Fig. 3) is determined by the 10. V. S. Soldatov and V. A. Bychkova, Ion-Exchange Equi-
energy nonequivalence of exchange sites in the poly-
libria in Multicomponent Systems (Nauka i Tekhnika,
Minsk, 1988) [in Russian].
mer. The differential entropies of ion exchange ∆S cal-
culated by the equation
1
1. G. L. Gaines, Jr. and H. C. Thomas, J. Chem. Phys. 11
(4), 714 (1953).
(
∆S)T, xCat = ((∆H – ∆G)/T)T, xCat
(4)
12. N. Bjerrum, Z. Phys. Chem. 106, 219 (1923).
RUSSIAN JOURNAL OF PHYSICAL CHEMISTRY A Vol. 81 No. 7 2007