again essentially followed pseudo-first-order kinetics (Figure
1b; Table 1, entries 4-6). Since the rates of tin hydride
mediated reactions depend primarily upon the stability of
the radical intermediates10 unlike in the case of cations, the
ꢀ-silicon substituent is able to stabilize to some extent the
radical at C-4 which is manifested in the observation of rate
enhancement by 3-fold. The magnitude of ꢀ-stabilization
was, however, much less than expected (calculated ꢀ-stabi-
lization energy was ∼3.2 kJ/mol vs 12.3 kJ/mol reported
for 2-trimethylsilyl-2-methyl propyl radical6).
From the above results, it is clear that while the ꢀ-effect
of silicon is absent in the case of a cationic intermediate the
effect is considerably suppressed in the case of a radical
intermediate. Three possible factors, (a) the antiaromaticity,
(b) involvement of N-lone pair, and (c) the dihedral angle,
might be considered, all of which could potentially suppress
the ꢀ-effect. It is indeed true that the dihedral angle11 plays
a dominant role in controlling the magnitude of the ꢀ-effect.
The optimized structure (Figure 2a) of the ꢀ-lactam contain-
Therefore, with the N-lone pair effect also failing to
satisfactorily explain our observation, one has to invoke the
role of antiaromaticity in these systems, which is in our view
mainly responsible for suppression of ꢀ-effect. Although the
suppression of the ꢀ-effect of silicon is beyond any doubt,
the subtle difference in its extent in the radical and the
cationic regime is not clear; the geometry of the radical and
cation at C-4 might be playing an important role which
accounts for the difference in percent antiaromatic destabi-
lization and thus can explain the suppressed ꢀ-effect to a
different extent.
To ascertain the relative reactivities of the ꢀ-lactams with
and without ꢀ-silyl groups at C-3, we carried out theoretical
calculations at the ROMP2)FC/6-31G**//B3LYP/3-21G*
level12 using Gaussian 98. Thus, the result showed no significant
change in charge distribution, especially at C-4 which is ꢀ to
silicon for both silylated and nonsilylated systems with a cation
or a radical generated at C-4. Although charge distribution in
the ground state is not an accurate method for predicting the
reactivity, development of any extra charge at C-4 indicated
the absence of any ꢀ-effect of silicon in these systems. The
results are in good agreement with our experimental findings.
The computational results also showed no significant change
in energetics whether silicon is present in the ꢀ-position or not.
Computation on cyclobutylamine systems as our ꢀ-lactam
model also showed no change in energetics. Although the
numbers refer to the thermodynamic changes, it is unlikely that
there would be a substantial change in kinetic barrier (Table
S4, Supporting Information).
The isodesmic calculation on the radical reaction using
B3LYP/3-21G* (using Gaussian 03)13 optimized geometries
pointed out strongly repressed ꢀ-silyl effect (stabilization
energies were only 3.36 kJ/mol for N-unprotected and 4.52
kJ/mol for N-protected ꢀ-lactam) supporting our experimental
results (Scheme S4, Supporting Information). Therefore, the
ꢀ-silyl effect has essentially been faded away because of the
Figure 2. (a) Calculated dihedral angle of the ꢀ-silyl cation. (b)
Kinetics of radical displacement of N-substituted ꢀ-lactams.
ing an empty p-orbital indicated that the concerned dihedral
angle was ∼32°, which suggests that the ꢀ-effect should still
be substantial at this dihedral angle, of the order of ∼104.11
Thus, the dihedral angle could not alone explain the
suppression of the ꢀ-effect.
(12) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb,
M. A.; Cheeseman, J. R.; Zakrzewski, V. G.; Montgomery, J. A., Jr.;
Stratmann, R. E.; Burant, J. C.; Dapprich, S.; Millam, J. M.; Daniels, A. D.;
Kudin, K. N.; Strain, M. C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi, M.;
Cammi, R.; Mennucci, B.; Pomelli, C.; Adamo, C.; Clifford, S.; Ochterski,
J.; Petersson, G. A.; Ayala, P. Y.; Cui, Q.; Morokuma, K.; Malick, D. K.;
Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.; Ortiz,
J. V.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.; Komaromi, I.;
Gomperts, R.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.; Peng,
C. Y.; Nanayakkara, A.; Gonzalez, C.; Challacombe, M.; Gill, P. M. W.;
Johnson, B.; Chen, W.; Wong, M. W.; Andres, J. L.; Gonzalez, C.; Head-
Gordon, M.; Replogle, E. S.; Pople, J. A. Gaussian 98, revision A.5;
Gaussian, Inc.: Pittsburgh, PA, 1998.
The involvement of the N-lone pair in stabilization of the
cation or radical should be of the same order, if at all, in all
the cases since we were dealing with similar systems.
Moreover, even where such stabilization is weak, we still
observed considerable suppression of the ꢀ-effect as revealed
in the radical-mediated reaction shown in Figure 2b (stabi-
lization is only about 3.3 kJ/mol). It is interesting to note
that our results on the ꢀ-effect of silicon followed the same
trend as the reported suppressed ꢀ-secondary deuterium
isotope effects2a in ꢀ-lactam systems for a cationic or a
radical intermediate. The absence of any downfield shift of
NH in 1-3 in the presence of excess thiophenol points out
again no additional participation of N-lone pair with the
carbonyl.
(13) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb,
M. A.; Cheeseman, J. R.; Montgomery, J. A., Jr.; Vreven, T.; Kudin, K. N.;
Burant, J. C.; Millam, J. M.; Iyengar, S. S.; Tomasi, J.; Barone, V.;
Mennucci, B.; Cossi, M.; Scalmani, G.; Rega, N.; Petersson, G. A.;
Nakatsuji, H.; Hada, M.; Ehara, M.; Toyota, K.; Fukuda, R.; Hasegawa, J.;
Ishida, M.; Nakajima, T.; Honda, Y.; Kitao, O.; Nakai, H.; Klene, M.; Li,
X.; Knox, J. E.; Hratchian, H. P.; Cross, J. B.; Bakken, V.; Adamo, C.;
Jaramillo, J.; Gomperts, R.; Stratmann, R. E.; Yazyev, O.; Austin, A. J.;
Cammi, R.; Pomelli, C.; Ochterski, J. W.; Ayala, P. Y.; Morokuma, K.;
Voth, G. A.; Salvador, P.; Dannenberg, J. J.; Zakrzewski, V. G.; Dapprich,
S.; Daniels, A. D.; Strain, M. C.; Farkas, O.; Malick, D. K.; Rabuck, A. D.;
Raghavachari, K.; Foresman, J. B.; Ortiz, J. V.; Cui, Q.; Baboul, A. G.;
Clifford, S.; Cioslowski, J.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz,
P.; Komaromi, I.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.;
Peng, C. Y.; Nanayakkara, A.; Challacombe, M.; Gill, P. M. W.; Johnson,
B.; Chen, W.; Wong, M. W.; Gonzalez, C.; Pople, J. A. Gaussian 03,
revision C.02; Gaussian, Inc.: Wallingford, CT, 2004.
(10) (a) Kuivila, H. G.; Menapace, L. W.; Warner, C. R. J. Am. Chem.
Soc. 1962, 84, 3584. (b) Chatgilialoglu, C.; Ingold, K. U.; Scaiano, J. C.
J. Am. Chem. Soc. 1981, 103, 7739.
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Org. Lett., Vol. 11, No. 24, 2009