NMR study of pyrazolo[3,4-c]pyridines
The structural conclusions formulated above from the 15N NMR
data are also supported by the values of the 13C chemical shifts.
Protonation of a nitrogen atom increases the shielding of a
neighboring carbon atom by about 10 ppm.[1] For compounds
1–6, the tautomeric migration of a proton should affect mainly
the C-7a and C-3 resonances. This effect is clearly evident from
the DFT calculations (see Table 7). The experimentally measured
differences in the chemical shifts ꢀδ (C7a-C3) are 3.5 ppm for 1
and 2.0 ppm for 2. In accordance with the experimental results,
the calculated ꢀδ values for the N-1 tautomers are 2.7 ppm (1a)
and 1.3 ppm (2a). In contrast, the values ꢀδ (C7a-C3) of 20.9 ppm
(1b) and 21.7 ppm (2b) were calculated for the N-2 tautomers.
Finally, the calculated energies support our conclusion that the
N-1 form predominates (ꢀE(b − a) is 2.7 kcal mol−1 for 1 and
3.2 kcal mol−1 for 2).[9] According to the Boltzmann distribution
(Table 7), at a temperature of 300 K, the difference in energy
corresponds to an a : b ratio of about 99 : 1, with the population of
the minor tautomer near or even below the limit of detection
for conventional NMR spectroscopy. These results represent
additional support for the conclusions made from the NMR data.
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Conclusions
Using low-temperature NMR spectroscopy, it was found that in
methanol all compounds either exist in one highly dominating
tautomeric form or undergo a rapid chemical exchange process,
evenattemperaturesaslowas171 K. ThepredominanceoftheN1-
H form at laboratory temperature was determined by comparing
the experimental 2JNH, 3JHN, ꢀδN(N2-N1), and ꢀδC(C7a-C3) values
for our compounds with those published for the N-acyl analogs
13 and 14 and the values calculated using DFT. Theoretically
calculated difference in energy favors the N1-H tautomer (a in
Scheme 1), with about 99% of the population at 300 K. All of the
compounds 1–6 were fully characterized by 1H, 13C, and 15N
chemical shifts and by 1H–13C and 1H–15N coupling constants.
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Acknowledgements
This work was supported by the Ministry of Education of the Czech
Republic (grants MSM0021622413 and LC06030 to TB, JT, and RM)
and by the Ministry of Industry, Energy, and Technology of Greece
(Research Grant, Program ENTER). We express our gratitude to the
staff members of the supercomputing centers in Brno and Prague
for CPU time.
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