2190 J . Org. Chem., Vol. 65, No. 7, 2000
Oh et al.
Ta ble 3. Activa tion P a r a m eter sa for th e Rea ction s of
Y-Ben zylid en em a lon on itr iles w ith X-Ben zyla m in es in
Aceton itr ile
benzylammonium ion in the putative T(. As to the TS
imbalance, the instantaneously localized negative charge
on Câ may facilitate the proton shift to Câ in the TS.
X
Y
∆Hq/kcal mol-1
-∆Sq/cal mol-1 K-1
p-OMe
p-OMe
p-Cl
p-Cl
a
p-Me
p-NO2
p-Me
5.6
5.8
6.1
5.8
32
35
33
38
p-NO2
Calculated by the Eyring equation. The maximum errors
calculated (by the method of Wiberg, K. B. Physical Organic
Chemistry; Wiley: New York, 1964; p 378) are (0.5 kcal mol-1
and (2 eu for ∆Hq and ∆Sq, respectively.
There remains an important result of the negative FY
for the addition of benzylamines to BMN in contrast to
the positive FY for the addition to NS to be explained
consistently with our proposed mechanism: For this
purpose, we should consider relative extent of resonance
delocalization within the reactants, BMN and NS (II and
III), as well as that within the activating groups of the
carbanion intermediates. The resonance delocalization in
+
polarization of the R-carbon to CR should be much
stronger in BMN than in NS.
The relatively lower electron density on CR-Câ due to
strong electron acceptor ability of the (CN)2 group should
lead to smaller primary kinetic isotope effects7 for the
reaction of NS (kH/kD = 2.30-3.08).4
There is almost a linear increase of kH/kD with σY (e.g.,
for X ) p-MeO, kH/kD ) 0.36σY + 2.45, r ) 0.981)
suggesting that a greater degree of bond formation (âx
increases with σY) results in a greater degree of proton
transfer in the TS, I.
The cross-interaction constant, FXY, calculated by sub-
jecting 20 rate data to multiple linear regression using
eq 2a is -0.31. This is also reasonable considering the
values for SN2 reaction (FXY ) - 0.6 to -0.8)5a if we
account for the falloff (=0.47)8 due to an intervening
group, CH2, in benzylamine (leading to FXY = -0.7). The
negative sign of FXY also ensures us an involvement of
the normal N-CR bond formation process in the TS,
excluding any possibilities of T( intermediate formation
for which the sign of FXY has been found to be positive in
the carbonyl addition reactions.9 The smaller magnitude
of FXY found for the addition to BMN than to NS is again
a manifestation of the dissociative nature of the TS for
the addition to BMN, since the magnitude of FXY is a
measure of the degree of bond formation.
II should be stronger than that in III since the two CN
groups provide a stronger π-electron-accepting ability.
The resonance parameters such as R (Swain-Lupton)
and σR (NMR chemical shift) show that two CN groups
are much stronger resonance electron acceptors than an
NO2 group; R (0.30 for (CN)2 and 0.13 for NO2) and σR
(0.36 for (CN)2 and 0.16 for NO2).6 On the other hand,
resonance stabilization of the carbanion in T( by H(NO2)
groups in NS is known to be much stronger than that by
the (CN)2 groups in BMN.2 However, this should apply
to the reactions in aqueous solution, where the terminal
anionic NO2 group in NS is strongly stabilized by hydra-
tion, IV, while stabilization by hydration of the anionic
(CN)2 groups in BMN is small, V. This difference in the
extent of solvation between the two, IV and V, should
be the main reason for the large difference in the strength
of resonance stabilization of the carbanions on the two
activating groups, (CN)2 , H(NO2), in aqueous solution.
In acetonitrile, however, weaker solvation of carbanions
on the two activating groups, H(NO2) in NS and (CN)2
in BMN, may cause to reduce the large difference of
solvating power, and the stronger electron withdrawing
power of the (CN)2 group in BMN may prevail.
The activation parameters, ∆Hq and ∆Sq in Table 3,
are consistent with the concurrent addition of nucleophile
and proton transfer, I.
The bond formation process normally requires small
activation energy, since exclusion repulsion energy is
partially offset by the bond energy of the forming bond.
In the present reactions, a π bond is broken concurrently,
but this is facilitated by the imbalance of the TS in which
reactant resonance stabilization is lost ahead of the bond
formation. The large negative entropy of activation (-32
to -38 eu) is consistent with the four-membered type of
constrained TS structure, I.
In summary, the addition of benzylamine (BA) to
benzylidenemalononitrile (BMN) occurs in a single step
in which the addition of BA to CR of BMN and proton
transfer from BA to Câ of BMN take place concurrently
with a four-membered cyclic TS structure, I. The reaction
center carbon, CR, becomes more positive (FY < 0) on going
from the reactant to transition state due to strong
polarization of the R-carbon, CR+, in the TS by the strong
electron-withdrawing polar effects of the two CN groups.
A measure of the electron-withdrawing power of the
(CN)2 group in the TS can be provided by the R- value,
which has been defined for π-electron acceptor substit-
uents in the reaction with strong conjugation with
electron-rich reaction centers. The R- values for (CN)2
and NO2 are 0.98 and 0.62, respectively;6 these are much
greater than the R values (0.30 and 0.13, respectively),
and the difference between the two (∆R- ) 0.36) is also
very large. Since both the inductive and resonance
electron-withdrawing power of the (CN)2 group are much
stronger than those of the NO2 group (vide supra),
(8) (a) Page, M.; Williams, A. Organic and Bio-organic Mechanisms;
Longman: London, 1997; p 250. (b) Hansch, C.; Hoekman, D.; Gao,
H. Chem. Rev. 1996, 96, 1045.
(9) (a) Lee, I. Bull. Korean Chem. Soc. 1994, 15, 985. (b) Oh, H. K.;
Shin, C. H.; Lee, I. J . Chem. Soc., Perkin Trans. 2 1995, 1169. (c) Lee,
I.; Koh, H. J . New J . Chem. 1996, 20, 131. (d) Koh, H. J .; Kim, O. S.;
Lee, H. W.; Lee, I.. J . Phys. Org. Chem. 1997, 10, 725. (e) Kim, T. H.;
Huh, C.; Lee, B. S.; Lee, I. J . Chem. Soc., Perkin Trans. 2 1995, 2257.