5932 J . Org. Chem., Vol. 62, No. 17, 1997
El Seoud et al.
Ha. The relevant point is that three hydrogens are
contributing to the kinetic solvent isotope effect, i.e., the
TS contains DNPC and two water molecules, over the
entire range of øw.
10-6 M),2 is solubilized in the ranges 0.4 g øw g 0.8 by
acetonitrile-water complexes that are either rich in
acetonitrile (for øw e 0.4) or rich in water (for øw g 0.8).
Alternatively, it is solubilized by the acetonitrile clusters
in the region of microheterogeneity (0.4 e øw e 0.8). On
the other hand, 1-methyl-3-oxypyridinium betaine (solu-
bility in pure water >2.0 M)8a forms its own solvation
sphere, the composition of which is always rich in water.8c
The remarkable similarity of Figure 1A,B indicates that
both processes, i.e., solvation of RB and hydrolysis of
DNPC are sensitive to the same interaction mechanisms,
mainly H-bonding and dipolar interactions. (iii) Both RB
and DNPC are hydrophobic substrates, and there are
certainly solvent effects both on GS and TS. One way to
explain our data is that solvation of the TS does not
change much as a function of øw, but the observed solvent
effects could be due to the smaller number of GS
molecules with adequate solvation to reach the TS. This
limiting case does not fit our results because it implies
an almost constant ∆Hq;6a this is not observed, Table 2.
Because the Gibbs free energies of transfer of several
nonelectrolytes from water to mixtures of water and
aprotic solvents are relatively insensitive to the binary
solvent composition,27,28 it is plausible that kinetic solvent
effects on the GS are not dominant in the present
reaction, so that we concentrate on solvation of the TS.6b-e
(iv) In the acetonitrile molecule the partial negative
dipole charge is localized on the nitrogen while the
positive charge of the dipole is diffused onto the methyl
group. Hence, it can solvate positive centers much
stronger than negative centers. On the other hand, the
water molecule is capable of solvating both types of
centers effectively. In the TS shown in Figure 4, the
partial negative charge is still localized on the carbonyl
oxygen while the positive charge is diffused; i.e., the TS
is more efficiently solvated by water, and solvent kinetic
effects should be sensitive to the state of water in the
binary solvent mixture.
Before addressing solvent effects on the hydrolysis of
DNPC, we discuss some relevant aspects of the structure
of acetonitrile-water mixtures:2,7-10,21-24 when the or-
ganic solvent is added to water it replaces the uncoordi-
nated water molecules. The limit of øW beyond which
acetonitrile cannot be accommodated within the cavities
of ordinary water is øw ≈ 0.85.10,21 Below this øw limit
solvent microheterogeneity sets in, and there exists two
“microdomains”, one highly structured consisting pre-
dominantly of coordinated water molecules and a rela-
tively disordered one containing mostly acetonitrile
H-bonded to water molecules.21,22 Calculations of the
Kirkwood-Buff integral functions showed that the prob-
ability of finding a water molecule close to an acetonitrile
molecule is minimum at øw ≈ 0.65.10,23a,b Addition of more
acetonitrile leads to a change in the relative concentra-
tions of the two microdomains, but their compositions do
not vary appreciably. At øw e 0.3 the water clusters have
become so few and far apart that new interactions set
in. Water-acetonitrile interactions become important;
this results in the formation of complexes, e.g., (CH3CN)m
- H2O where m ) 1-4.10,23c,24a,b At still lower øw values,
the structure of acetonitrile dominates, and species such
as (CH3CN)m and CH3CN are abundant.23c It should be
born in mind, however, that the onset of formation of the
different regions is not sharp and is dependent on the
method used to study the system.10
In addressing the results shown in Figures 1 and 2,
the following points are relevant: (i) A detailed analysis
of solvent kinetic effects on hydrolysis of DNPC over the
whole øw range is beyond the scope of the present work
and may not even be possible because of the above-
mentioned solvent microheterogeneity. This explains the
fact that studies in which overall solvent kinetic effects
have been separated into contributing interactions of
solvent components with GS and TS have been confined
to the water-rich region.6c,25,26 Additionally, experimental
determination of thermodynamic functions of transfer of
DNPC from a reference solvent to aqueous acetonitrile
mixtures that could shed light on solvent interactions
with GS and TS27 is not feasible because of the facile
hydrolysis of this ester. (ii) Our results indicate that
solvatochromism of RB in acetonitrile-water mixtures
is very different from that of the small, hydrophilic probe
1-methyl-3-oxypyridinium betaine.8c This indicates that
RB, being very hydrophobic (solubility in water ) 7.2 ×
The initial addition of acetonitrile to water (øw from
0.971 to 0.871) results in a decrease of kobs and increase
in ∆Hq and ∆Sq since uncoordinated water molecules
would be considerably more polar (i.e., of higher kinetic
reactivity) and form stronger H-bonds than their coor-
dinated counterparts.1,29 In the intermediate øw region
(øw from 0.783 to 0.552), the structure of each micro-
domain should remain relatively constant so long as they
exist.21 Consequently, the solvent-dependent process, i.e.,
hydrolysis of DNPC or solvation of RB, may vary little
as shown in Figure 1A,B. Addition of more acetonitrile
(øw e 0.453, Table 2) results in formation of mobile
acetonitrile-water clusters. In this acetonitrile-rich
region the rate constant decrease simply reflects the
decrease in [water]. The observed decrease of ∆Hq may
be due to the fact that water-acetonitrile interactions
are weaker that water-water interactions.21-24 The
accompanied entropy decrease occurs because the reac-
tant water has more degrees of freedom. It is interesting
(21) (a) Easteal, A. J . Aust. J . Chem. 1979, 32, 1379. (b) Balakrish-
nan, S.; Easteal, A. J . Aust. J . Chem. 1981, 34, 943. (c) Easteal, A. J .;
Woolf, L. A. J . Chem. Thermodyn. 1982, 14, 755.
(22) (a) Gorbunov, B. Z.; Naberukhin, Yu. I. J . Mol. Struct. 1972,
14, 113. Gorbunov, B. Z.; Naberukhin, Yu. I. J . Struct. Chem. 1975,
16, 755.
(23) (a) Matteoli, E.; Lepori, L. J . Phys. Chem. 1984, 80, 2856. (b)
Blandamer, M. J .; Blundell, N. J .; Burgess, J .; Cowles, H. J .; Horn, I.
M. J . Chem. Soc., Faraday Trans. 1990, 86, 277. (c) Rowlen, K. L.;
Harris, J . M. Anal. Chem. 1991, 63, 964.
(24) (a) Wakisaka, A.; Shimizu, Y.; Nishi, N.; Tokumaru, K.;
Sakuragi, H. J . Chem. Soc., Faraday Trans. 1992, 88, 1129. (b)
Wakisaka, A.; Takahashi, S.; Nishi, N. J . Chem. Soc., Faraday Trans.
1995, 91, 4063.
that the gradual increase in ∆Gq (∆∆Gq ) ∆Gqøw0.1
-
∆Gqøw0.453) is due to a loss of entropy (T∆∆Sq ) -6.5 kcal/
mol, Table 2) not compensated by a gain in enthalpy
(∆∆Hq ) -4.6 kcal/mol, Table 2).
(25) Blandamer; M. J .; Burgess, J . Chem. Soc. Rev. 1975, 4, 55 and
references cited therein.
Con clu sion s
(26) (a) Blokzijl, W.; Engberts, J . B. N.; J ager, J .; Blandamer, M. J .
J . Phys. Chem. 1987, 91, 6022. (b) Blokzijl, W.; Blandamer, M. J .;
Engberts, J . B. N. J . Org. Chem. 1991, 56, 1832.
(i) Calculation of the kinetic order with respect to one
component of a binary solvent mixture should be based
(27) (a) Abraham, M. H. Prog. Phys. Org. Chem. 1974, 11, 2. (b)
Yates, K.; McClelland, R. A. Ibid. 1974, 11, 324. (c) Buncel, E.; Wilson,
H. Acc. Chem. Res. 1979, 12, 42.
(28) Cox, B. G. J . Chem. Soc., Perkin Trans. 2 1973, 607.
(29) Symons, M. C. R. Acc. Chem. Res. 1981, 14, 179.