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G. I. Borodkin et al. / Tetrahedron Letters 50 (2009) 6779–6782
Table 1
1H chemical shifts (d, ppm) and spin–spin coupling constants (Hz) of cations 2 and 3a
b
X
Cation
X
H-2
H-3
H-5
H-6
NH2
H
2a
—
8.74 (1H, ddd, 4.0, 1.6,
9.14 (1H, dd, 4.0,
9.14 (1H, dd, 4.0, 1.0)
8.74 (1H, ddd, 4.0, 1.6,
9.60
1.0)
—
1.0)
1.0)
(2H)
9.08
(2H)
9.51
(2H)
9.6 (2H)
Me
Et
2b
3b
2c
3c
2d
3d
2e
3e
3f
2.67 (3H, ddd, 0.8, 0.8, 0.4)
2.60 (3H, ddd, 0.7, 0.7, 0.7)
9.13 (1H, qd, 0.8,
0.7)
—
8.97 (1H, dq, 4.0, 0.8)
8.80 (1H, ddq, 4.0, 0.7,
0.4)
8.62 (1H, ddq, 3.9, 1.5,
0.7)
8.84 (1H, ddt, 4.0, 0.8,
0.4)
8.66 (1H, ddt, 3.9, 1.6,
0.6)
8.85 (1H, dd, 4.0, 0.8)
8.71 (1H, dqd, 1.5, 0.7,
0.7)
—
9.01 (1H, dqd, 3.9, 0.7,
0.7)
8.98 (1H, dt, 4.0, 0.7)
1.30 (3H, t, 7.4) 3.05 (2H, qddd,
7.4, 0.8, 0.7, 0.4)
1.24 (3H, t, 7.6) 2.87 (2H, qdd,
7.6, 0.6, 0.5)
0.95 (3H, t, 7.4) 1.71 (2H, tq,
7.8, 7.4) 3.01 (2H, t, 7.8)
0.88 (3H, t, 7.4) 1.66 (2H, tq,
7.6, 7.4) 2.80 (2H, t, 7.6)
1.32 (6H, d, 6.8) 3.64 (1H, sept,
6.8)
9.08 (1H, td, 0.8,
0.8)
—
8.78 (1H, ddt, 1.6, 0.9,
0.5)
—
9.03 (1H, dd, 3.9, 0.9)
8.98 (1H, d, 4.0)
9.6 (2H)
9.6 (2H)
9.1 (2H)
9.5 (2H)
9.5 (2H)
Pr
9.08 (1H, d, 0.8)
8.80 (1H, dd, 1.6, 0.9)
—
—
9.04 (1H, dd, 3.9, 0.9)
8.99 (1H, d, 4.0)c
8.68 (1H, dd, 3.9, 1.6)
8.81 (1H, d, 4.0)c
i-Pr
9.19 (1H)c
—
1.23 (6H, d, 6.9) 3.16 (1H, sept, 8.83 (1H, dd, 1.5, 0.9)
6.9)
9.05 (1H, dd, 3.9, 0.9)
8.67 (1H, dd, 3.9, 1.5)
t-Bu
CH(OH)Me 2g
1.35 (9H, s)
1.55 (3H, d, 6.6) 5.34 (1H, qdd,
6.6, 0.6, 0.6) 5.2 (1H, br s)
8.82 (1H, dd, 1.5, 0.9)
—
—
9.10 (1H, dd, 3.8, 0.9)
9.05 (1H, dd, 4.0, 0.6)
8.63 (1H, dd, 3.8, 1.5)
8.81 (1H, dd, 4.0, 0.8)
9.5 (2H)
9.1 (2H)
9.22 (1H, dd, 0.8,
0.6)
—
3g
1.44 (3H, d, 6.6) 4.91 (1H, qdd, 8.80 (1H, ddd, 1.7, 0.9,
9.04 (1H, dd, 3.9, 0.9)
7.90 (1H, d, 4.4)
8.66 (1H, ddd, 3.9, 1.7,
0.8)
8.07 (1H, dd, 4.4, 1.0)
9.6 (2H)
6.6, 0.8, 0.8) 5.2 (1H, br s)
8.84 (2H, br s)
0.8)
—
NH2
2h
8.61 (1H, d, 1.0)
7.14
(2H)
3h
3i
7.68 (2H, br s)
2.20 (3H, s) 11.6 (1H, br s)
7.84 (1H, dd, 1.5, 0.9)
9.42 (1H, dd, 1.5, 0.9)
—
—
7.80 (1H, dd, 3.8, 1.5)
8.83 (1H, dd, 3.9, 0.9)
8.37 (1H, dd, 3.8, 0.9)
8.43 (1H, dd, 3.9, 1.5)
9.0 (2H)
9.6 (2H)
NHAc
a
b
c
Spectra in DMSO-d6. Chemical shifts are referenced to TMS with DMSO as a secondary internal standard (d 2.50 ppm).
Broad singlet.
Some constants are not determined because of low signal intensity.
4.17 The corresponding 1-amino-2-(N-acetylamino)pyrazinium 2i
undergoes rapid ring closure, such that cation 2i cannot be ob-
served.
It has been proven that in the case of X = alkyl, only steric effects
are essential (Table 2, Fig. 1)
:
lgð2 : 3Þ ¼ ðꢀ0:19 ꢁ 0:07Þ þ ð0:84 ꢁ 0:15ÞEso
r ¼ 0:958; s ¼ 0:13; n ¼ 5
N
N
NH2
N
ð1Þ
ð2Þ
O
-
MesSO3
lgð2 : 3Þ ¼ ðꢀ0:18 ꢁ 0:04Þ ꢀ ð0:41 ꢁ 0:03ÞF
r ¼ 0:990; s ¼ 0:06; n ¼ 5
-H3O+MesSO3
-
N
N
N
N
N
H
NH2
N
NH2
In the case of other substituents, the electronic effect is signifi-
cant: a correlation of lg (2:3) with Eq. (3) using the rI,
2i
4
5
r
oR, and Eos
For the cations that were observed, the structures were estab-
lished by means of 1H NMR spectroscopy (Table 1). In addition,
the structures of cations 2a,h and 3i were determined by X-ray dif-
fraction.18 Assignment of the proton signals was accomplished
using various 2D-NMR techniques. Application of NOESY tech-
niques was based on detection of the Overhauser effect between
the protons of the NH2 group and H-2(6) located in proximity to
each other. The nJ(H,H) values of the cations were determined by
analysis of the spin systems (i.e., simulation and iteration) in the
1H NMR spectra. The resonance due to H-2 in cation 3h occurs at
a relatively high frequency. This is readily explained in terms of a
contribution from the resonance structure 5.
constants gives the following result (Table 2):
lgð2 : 3Þ ¼ ðꢀ0:24 ꢁ 0:08Þ þ ð0:87 ꢁ 0:98ÞrI ꢀ ð1:03 ꢁ 0:60ÞrRo
þ ð0:94 ꢁ 0:11ÞEos r ¼ 0:977; s ¼ 0:12; n ¼ 8
ð3Þ
In order to gain an insight into the reactivity and regioselectiv-
ity of the amination of X-pyrazines 1 (X = H, Me, Et, Pr, i-Pr,
CH(OH)CH3, NH2) in terms of their prediction, the energy barriers
were calculated using the DFT/PBE/3z method23–25 (cf. Ref. 18).
For pyrazines 1b–e,g,h, the asymmetry of the transition state
structures was taken into account based on their dependence on
the nature of the X-substituent on the ring. Table 2 gives the lowest
barriers from these variants for each substituent X. All the
transition states have a single negative normal mode and the
oscillatory vector corresponds to the movement of the NH2 group
from the oxygen atom of the OSO2Mes group to the nitrogen atom
of the pyrazine (Fig. 2). The intrinsic reaction coordinates (IRCs) go
from the transition states directly to the products or to the
reactants.
The isomeric ratio (2:3) was determined by 1H NMR spectros-
copy (Table 2). The ratio is kinetically controlled and highly
responsive to substituent effects. The kinetic control was con-
firmed by the invariance of the 1H NMR spectra of ions 2h and 3i
after aging solutions of the respective salts in DMSO-d6 at 100 °C
for four hours. Consequently, intramolecular and/or intermolecular
þ
transfer of the NH2 cation from one nitrogen atom to another in
the pyrazinium ring does not occur.
Taking into account the proximity of the reaction center to the
X-substituent in 2-X-pyrazines, it can be assumed that the ratio of
isomeric cations is determined not only by electronic effects, but
also by steric effects. The difference in the inductive influence of
the alkyl substituents at positions 2 and 3 is probably insignificant.
As carefully checked, the correlations are statistically reliable. Two-parametric
correlations between lg(2:3) and the EoS ðFÞ-,
rI-constant result in no statistically
significant changes.