9976 J. Am. Chem. Soc., Vol. 119, No. 42, 1997
Yamataka et al.
Table 1. Kinetic and Equilibrium Isotope Effects for the Reaction
of Lithium Pinacolone Enolate and Benzaldehyde
substituted benzophenone derivatives and showed a sizable
carbonyl-carbon KIE, and the results were ascribed to a slower
RC step for this sterically hindered ketone and hence a shift of
rate-determining step from ET (for benzophenone) to RC (for
mesityl phenyl ketone).5 In sharp contrast, the reaction of
RMgX gave medium sized KIEs in most cases, and this was
concluded to be due to rate-determining RC mechanism.4
Our conclusion that the reaction of MeLi, PhLi, and
CH2dCHCH2Li with the aromatic carbonyl compounds proceed
via an ET process was different from that by Arnett for the
reaction of lithium pinacolone enolate. The discrepancy should
be due to either the difference of reagents or the difference of
the mechanistic criteria. In the present study, the KIE, sub-
stituent effect, and chemical probe experiments were carried
out for the addition reaction of lithium pinacolone enolate with
benzaldehyde. The results clearly show that the mechanism
for the enolate is different to other RLi and is polar.
labeled position
k/k* a
K/K* b
kH/kD5
1.031 ( 0.004
0.988 ( 0.002
1.019 ( 0.004c
1.094
13
k / k
D5
12k/13k
1.006
a Experimental kinetic isotope effect in THF at 0 °C. b Calculated
equilibrium isotope effect on the addition process at 0 °C. c Calcd from
kH/kD5 and kD5/13k.
carbonyl carbon KIE is expected to be large for the PL and the
rate-determining RC mechanism because the carbonyl carbon
is heavily involved in these C-C bond forming processes. On
the other hand, the carbon KIE is expected to be small for the
rate-determining ET mechanism since there is no contribution
from the reaction-coordinate motion. Distinction between PL
and rate-determining RC is more difficult, and kinetic methods
like KIE are almost ineffective because the two transition states
behave in a similar manner in kinetic criteria. Another way to
differentiate these two mechanisms is needed which examines
the possible intervention of a radical ion-pair intermediate in
the ET-RC sequence, and this will be discussed later.
Isotope effects were determined for C6D5CHO vs C6H5CHO
and C6H513CHO vs C6D5CHO in order to avoid the interference
of 13C natural abundance in intensity measurement. The
observed KIEs at 0 °C were listed in Table 1. In discussing
the observed KIEs, it is useful to know the magnitudes of IEs
on the corresponding equilibria. For this purpose, theoretical
isotope effects on the addition equilibrium were computed by
using ab initio MO methods. Thus, benzaldehyde and benzal-
dehyde-methyl lithium adduct were fully optimized at HF/6-
31+G*, and their vibrational frequencies were calculated. MeLi
was used here instead of lithium pinacolone enolate for
simplicity assuming that the equilibrium IEs are not much
different for the MeLi addition and the lithium enolate addition.
Equilibrium IEs for carbonyl-13C, aldehyde-d1, and phenyl-d5
species were computed from the frequencies of isotopomers by
using eq 2 and listed in Table 1. The HF frequencies were
scaled down by a factor of 0.89 in the IE calculations.
Results and Discussion
Lithium pinacolone enolate was prepared from the reaction
of pinacolone and lithium diisopropylamide in THF at -78 °C
and allowed to react with benzaldehyde at 0 °C. Substituent
effects were determined by competition experiments as previ-
ously reported,4-6 and carbonyl carbon-13 and C6D5 KIEs were
measured as described in the Experimental Section. We used
in the present study FT ion-cyclotron resonance mass spec-
trometry (FT-ICR MS) to determining the carbon KIE of 13C-
labeled compound rather than the conventional liquid scintil-
lation counting method of radioactive 14C compounds. This
new method can be a powerful tool in mechanistic study by
allowing us to measure KIEs of nonradioactive elements, such
as 18O, 15N, D, etc. in addition to 13C. The FT-ICR method
has previously been used to determine equilibrium IEs success-
fully.10 Two chemical probe experiments, enone isomerization
and dehalogenation probes, were carried out as described
previously.6c,7 Ab initio MO calculations were carried out to
estimate the magnitude of equilibrium IEs for the polar process
by using the Gaussian 92 and 94 packages of program.8,9
Carbon KIE. Among the three possible mechanistic alterna-
tives, distinction of the rate-determining ET mechanism from
PL and rate-determining RC can be achieved in a rather
straightforward manner by using the carbonyl-carbon KIE as a
probe. A carbon KIE is larger if the labeled carbon atom is
involved to a greater extent in the reaction-coordinate vibrational
motion at the rate-determining transition state,11,12 and thus the
1 - e-u
1 - e-u
3n-6
3n-6
1i
∏ u2i ∏
3n-6
k1
k2
νqL1
u1i
(
(
)
)
exp[
(u - u )/2]
1i 2i
2i
∏
)
(2)
q
q
3n-7
q
[ ]
1 - e-u
1 - e-u
3n-7
3n-7
1i
∏ u2i ∏
νL2
exp[
(uq - uq )/2]
∏
1i
2i
q
uq1i
2i
(7) Yamataka, H.; Yamaguchi, K.; Takatsuka, T.; Hanafusa, T. Bull.
Chem. Soc. Jpn. 1992, 65, 1157.
The experimental carbonyl-13C KIE was small positive (12k/
13k ) 1.019), which corresponds to 1.039 of 14C KIE. This
value is similar to carbonyl-14C KIEs previously observed for
polar nucleophilic additions to benzophenone; 12k/14k ) 1.035
(BH3/THF), 1.021 (AlH3/Et2O), LiAlH4/THF (1.017), LiAlH4/
Et2O (1.024), LiBH4/Et2O (1.043), and NaBH4/2-PrOH (1.066).13
The theoretical equilibrium IE at carbonyl 13C for the addition
to benzaldehyde was found to be small (12k/13k ) 1.006). The
fact that the experimental carbonyl-13C KIE is larger than the
corresponding equilibrium IE indicates that the carbonyl-carbon
KIE is of primary nature, suggesting that the bonding to the
carbon is changing at the rate-determining transition state. The
IE results are consistent with the PL mechanism for the addition
reaction, although the IE results by themselves do not eliminate
the possibility that the reaction proceeds via fast ET followed
by a slow rate-determining RC step.
(8) Frisch, M. J.; Trucks, G. W.; Head-Gordon, M.; Gill, P. M.; Wong,
M. W.; Foresman, J. B.; Johnson, B. G.; Schlegel, H. B.; Robb, M. A.;
Replogle, E. S.; Gomperts, R.; Andress, J. L.; Rachavachari, K.; Binkley,
J. S.; Gonzalez, C.; Martin, R. L.; Fox, D. J.; Defrees, D. J.; Baker, J.;
Stewart, J. J. P.; Pople, J. A. GAUSSIAN 92; Gaussian Inc.: Pittsburgh,
PA, 1992.
(9) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Gill, P. M. W.; Johnson,
B. G.; Robb, M. A. ; Cheeseman, J. R.; Keith, T.; Petersson, G. A.;
Montgomery, J. A.; Raghavachari, K.; Al-Laham, M. A.; Zakrzewski, V.
G.; Ortiz, J. V.; Foresman, J. B.; Cioslowski, J.; Stefanov, B. B.;
Nanayakkara, A.; Challacombe, M.; Peng, C. Y.; Ayala, P. Y.; Chen, W.;
Wong, M. W.; Andress, J. L.; Replogle, E. S.; Gomperts, R.; Martin, R.
L.; Fox, D. J.; Binkley, J. S.; Defrees, D. J.; Baker, J.; Stewart, J. P.; Head-
Gordon, M.; Gonzalez, C.; Pople, J. A. GAUSSIAN 94, Revision C2;
Gaussian, Inc.: Pittsburgh, PA, 1995.
(10) Yamataka, H.; Mishima, M.; Kuwatani, Y.; Tsuno, Y. J. Am. Chem.
Soc. 1995, 117, 5829.
(11) Melander, L.; Saunders, W. H., Jr. Reaction Rates of Isotopic
Molecules; Wiley-Interscience: New York, 1980.
(12) Sims, L. B.; Lewis, D. E. In Isotopes in Organic Chemistry; Buncel,
E., Lee, C. C., Eds.; Elsevier: Amsterdam, 1984; Vol. VI, Chapter 4.
Yamataka, H.; Ando, T. J. Phys. Chem. 1981, 85, 2281. Yamataka, H.;
Tamura, S.; Hanafusa, T.; Ando, T. J. Am. Chem. Soc. 1985, 107, 5429.
(13) Yamataka, H.: Hanafusa, T. J. Am. Chem. Soc. 1986, 108, 6643.
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