This is identical with the observed kinetics, provided that
ϪI ӷ kII[A], and we have kobs = kIkII/kϪI.
However, a reaction between two negative ions, of which at
least one has a high charge, does not seem very probable,
whence a theoretical estimate of the kinetic parameters should
be attempted. The necessary expressions of rate constants,
based on theories of Debye10 and Fuoss,11 are found in a clas-
sical paper by Eigen.12 For the rate constant of a diffusion-
controlled bimolecular reaction between two ions A and B in
solution, represented by kI and kII, we have
When we insert these values in eqns. (10)–(13) together with
k
the relative permittivity of water at 25 ЊC, Kr = 78.54, we find
EaЈ(I) = 13.2 kJ molϪ1, kI = 2.06 × 108 MϪ1 sϪ1 and EaЈ(II) =
51.4 kJ molϪ1, kII = 149.2 MϪ1 sϪ1
There is no significant electrostatic contribution to the
activation energy related to kϪI, because the exponential in
the denominator of eqn. (12) is Ӷ 1. We have from eqn. (12)
k
ϪI = 1.077 × 1011 sϪ1
The sum of the two activation energies is 64.6 kJ molϪ1, to
which we should add a contribution from the dependence of
diffusion coefficients on temperature. This may be estimated
from the temperature dependence of ionic conductivities of
(10)
4Ϫ 13
D
Fe(CN)6
,
which yields Ea = 13.8 kJ molϪ1; it enters only
where
once, because two of the factors DA ϩ DB cancel as seen from
eqns. (10) and (12). We note that the condition kϪI ӷ kII[A] for
third-order kinetics (eqn. (9)) is fulfilled.
(11)
The resulting estimated activation energy and rate constant
are thus Ea = 78.4 kJ molϪ1 and kcalc = 0.285 MϪ2 sϪ1
Each z denotes the charge in units of the electronic charge,
each D the diffusion coefficient and each r the radius of the ion,
and Kr is the relative dielectric constant of the solution (Eigen
uses c.g.s. units, whence his expression of Z is slightly different).
Similarly, the rate constant kϪI is given by
The former value is significantly higher and the latter signifi-
cantly lower than the experimental values. However, the theor-
etical values are highly sensitive to the choice of ionic radii. For
instance, by increasing the radii of the hexacyanoferrate() ion
and the hexacyanoferrate()-bromite ion pair by as little as
15%, perfect agreement between theory and experiment is
obtained.
A negative activation entropy is typical of second- or higher-
order reactions between ions which are not strongly hydrated.
The value found in the present study is in line with values for
other reactions between negative ions in aqueous solution.14
(12)
For two positive or two negative ions the exponential in the
denominator of eqn. (10) is ӷ 1, and so the contribution from
electrostatic interactions to the activation energy is
Conclusion
The reduction of bromite by hexacyanoferrate() is a third-
order reaction in two stages, of which the first, being rate-
determining, is the reduction of bromite to hypobromous acid,
and the second and much faster, is the further reduction to
bromide. The first stage involves two bimolecular reactions,
either one between two negative ions, which means that electro-
static repulsion is the main contribution to energy barriers. This
also explains the much faster reduction of hypobromite: Due to
the low dissociation constant of hypobromous acid, the electro-
static energy barrier is absent in the first elementary process,
and in the second it is reduced by 20%. This alone would cause
an increase in reaction rate by more than a factor of 104 com-
pared to the reduction of bromite, provided that the mechanism
proposed above is correct.
(13)
The diffusion coefficients may be obtained from the ionic
conductivities, using the Nernst–Einstein equation
(14)
For Fe(CN)64Ϫ we have13 λ = 0.0444 S m2 molϪ1, which yields
D = 0.739 × 10Ϫ9 m2 sϪ1. The value of λ for the bromite ion is
unknown, but a reasonable guess on the basis of the values for
the oxoions of Cl and for BrO3Ϫ is λ = 0.0045 S m2 molϪ1, which
gives D = 1.198 × 10Ϫ9 m2 sϪ1
.
For the ionic radii we have several choices, but to avoid the
complication of using different values in different expressions,
we shall use the hydrodynamic radii calculated from the Stokes–
Einstein equation
References
1 T. Andersen and H. E. Lundager Madsen, Anal. Chem., 1965, 37,
49.
2 T. Andersen, H. E. Lundager Madsen and K. Olesen, Trans.
Faraday Soc., 1966, 62, 2409.
3 L. Wang, J. S. Nicoson, K. E. Huff Hartz, J. S. Francisco and
D. W. Margerum, Inorg. Chem., 2002, 41, 108.
(15)
4 J. S. Nicoson, L. Wang, R. H. Becker, K. E. Huff Hartz, C. E.
Muller and D. W. Margerum, Inorg. Chem., 2002, 41, 2975.
5 R. C. Troy and D. W. Margerum, Inorg. Chem., 1991, 30, 3538.
6 C. L. Lee and M. W. Lister, Can. J. Chem., 1979, 57, 1524.
7 J. Clarens, C. R. Acad. Sci, 1913, 156, 1998.
8 M. H. Hashmi and A. A. Ayaz, Anal. Chem., 1963, 35, 908.
9 I. Meybeck, I. Leclerc and R. Kircher, Ger. Pat., 1,069,123 1959
(to SECPIA).
10 P. Debye, Trans. Electrochem. Soc., 1942, 82, 265.
11 R. M. Fuoss, J. Am. Chem. Soc., 1958, 80, 5059.
12 M. Eigen, Z. Elektrochem., 1960, 64, 115.
13 Landolt-Börnstein, Zahlenwerte und Funktionen, 6. Aufl., II. Band,
7. Teil, Springer, Berlin, 1960, pp. 259, 261.
where η, the dynamic viscosity of water at 25 ЊC, equals
0.8903 mPa s. This yields
Fe(CN)64Ϫ: r = 3.32 × 10Ϫ10 m
BrO2Ϫ: r = 2.05 × 10Ϫ10 m
We also need the radius and the diffusion coefficient of the
ion pair of hexacyanoferrate() and bromite. We assume that
the two ions are spherical and then add the volumes calculated
from the above radii. If we further assume that the ion pair is
also spherical, we find its radius r = 3.56 × 10Ϫ10 m. Finally, we
calculate its diffusion coefficient from eqn. (15): D = 0.689 ×
14 A. A. Frost and R. G. Pearson, Kinetics and Mechanism, Wiley,
New York, 2nd edn., 1961, p. 144.
10Ϫ9 m2 sϪ1
.
D a l t o n T r a n s . , 2 0 0 3 , 4 6 5 1 – 4 6 5 3
4653