TABLE 1. Results from the NMR Analysis of Acetoacetanilide (5)
in Solutions of Varying Acidity
TABLE 2. Calculated Relative Stabilities and NMR Data for Ions
6-12 at the MP2/6-311++G(d,p) Level (DFT Calculations,
B3PW91/6-311++G(d,p) Level)a
acidity, temp,
solvent
CDCl3
Ho
°C
25 30.7, 50.6, 120.3,
124.6, 128.9, 137.6,
164.4, 204.3
-2.7 -10 28.1, 46.3, 122.1,
127.3, 128.4, 132.7,
13C signals,a δ
15N signal,a δ
132.0 (doublet)
CF3CO2H
FSO3H
144.1 (doublet)
150.9 (doublet)
162.3 (doublet)
168.8, 209.3
-15
-40 28.4, 42.9, 122.6,
129.3, 129.8, 130.1,
168.8, 220.6
FSO3H, SbF5 -24
-40 29.7, 44.9, 123.5,
(1:1)
126.9, 130.2, 131.7,
165.8, 237.5
a Superacidic samples were prepared with SO2CIF as cosolvent; the 13
C
external standard was d6-acetone; the 15N external standard was 15N-labeled
urea in d4-methanol.
the superacidic solutions. If the N,O-diprotonated species
(dication 6) is generated as the superelectrophilic intermediate,
then a triplet 15N resonance should be visible in the 15N NMR
spectrum (assuming rapid proton exchange does not obscure
1H-15N coupling). In the strongest superacid used, SbF5-
FSO3H-SO2ClF, the 15N resonance appears downfield at δ
162.3 as a doublet. The amide 15N is significantly deshielded
in SbF5-FSO3H-SO2ClF, which is a consequence of the
formation of the neighboring carboxonium ion (and increasing
positive charge). On the basis of these data, it is proposed that
acetoacetanilide (5) forms a significant equilibrium concentration
1
of the O,O-diprotonated species (7). The H NMR spectra of
acetoacetanilide (5) were also obtained from superacidic media
(FSO3H, CF3SO3H, and SbF5-FSO3H solutions at -50 °C),
and the spectra are consistent with the formation of dication 7.
In each of the superacid solutions, the spectra clearly show the
methyl (CH3), methylene (CH2), amide (NH), and phenyl (C6H5)
protons. The spectrum from FSO3H is typical: δ 2.15 (3H),
3.85 (2H), 6.75-6.84 (5H), 9.35 (NH). The carboxonium
proton(s) could not be observed, possibly due to fast exchange
with the acid. With greater acidity, both the NH and the
methylene peaks maintain the same intensity. This observation
argues against the formation of N,O-diprotonated species
(dication 6) and any possible enol-type structures (vide infra).
Model calculations were performed on the protonated prod-
ucts from acetoacetanilide (5) to estimate the relative energies
of the diprotonated species (6-9) and to compare experimental
NMR chemical shift values with those from theory (Table 2).9
Likewise, monocationic products (10-12) were also studied.
At both the ab initio MP2/6-311++G(d,p) and density func-
tional theory B3PW91/6-311++G(d,p) levels of theory,10 the
a The 15N signals are calculated in reference to NH3 (gas phase); the 13
signals are calculated in reference to Si(CH3)4. b Not a stable minimum,
-OH2 bonds set at a fixed length. c Not a stable minimum, -OH bond set
at a fixed length. d Not a stable minimum, -NH bond set at a fixed length.
C
N,O-diprotonated species (6) and the O,O-diprotonated species
(7) are found at energy minima (as determined by frequency
calculations), with structure 6 being at least 8 kcal‚mol-1 less
stable than structure 7. Although the enol-type structure (8) is
at an energy minimum, it is about 14 kcal‚mol-1 less stable
than structure 7. The isomeric enol-type structure (9) is not at
an energy minimum, but rearranges upon optimization. 15N and
13C NMR GIAO data, calculated at the B3PW91/6-311++G-
(d,p)//B3PW91/6-311++G(d,p) and HF/6-311++G(d,p)//MP2/
6-311++G(d,p) levels, indicate that the 15N NMR resonances
are diagnostic for N versus O protonation, as they vary sizably
between 6 and 7 (65-75 ppm). The experimental spectrum from
protonation of compound 5 in SbF5-FSO3H-SO2ClF exhibits
the 15N resonance at δ 162.3, reasonably close to that predicted
for the O,O-diprotonated species (7). The calculated values for
13C resonances differ little for structures 6 and 7, and therefore
they are not as useful in distinguishing between N versus O
protonation, but the calculated 13C resonance for C2 does appear
to rule out the enol-type structure (8) as a major component of
the equilibrium mixture in superacid. In comparing the calcu-
lated and experimental 13C spectra for dication 7, it is seen that
both theoretical models predict the experimental spectrum fairly
well. The density functional B3PW91 performs particularly well
(8) (a) Olah, G. A.; Rasul, G.; York, C. T.; Prakash, G. K. S. J. Am.
Chem. Soc. 1995, 117, 11211. (b) Klumpp, D. A.; Rendy, R.; Zhang, Y.;
Gomez, A.; McElrea, A. Org. Lett. 2004, 6, 1789.
(9) 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,
A D.; Rabuck, K. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.;
Ortiz, J. V.; Baboul, A. G.; 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.; 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.11.4; Gaussian, Inc.: Pittsburgh, PA, 1998.
(10) (a) Becke, A. D. J. Chem. Phys. 1993, 98, 5648. (b) Wolinski, K.;
Hinton, J. F.; Pulay, P. J. Am. Chem. Soc. 1990, 112, 8251.
9762 J. Org. Chem., Vol. 72, No. 25, 2007