876
P. A. Bradley et al.
LETTER
and their corresponding relative energies (in kcal/mol) associated to
the studied N-alkylation for both substituents (R = Me, CO2Et).
a preferential stability of N2–H tautomer in the gas phase
(5.9 kcal/mol). In solution, however, the most polar N1–H
tautomer becomes nearly isoenergetic (only 0.3 kcal/mol
differences).
(8) Tong, Y.; Claiborne, A.; Pyzytulinska, M.; Tao, Z.; Stewart,
K. D.; Kovar, P.; Chen, Z.; Credo, R. B.; Guan, R.; Merta,
P. J.; Zhang, H.; Bouska, J.; Everitt, E. A.; Murry, B. P.;
Hickman, D.; Stratton, T. J.; Wu, J.; Rosenberg, S. H.; Sham,
H. L.; Sowin, T. J.; Lin, N. Bioorg. Med. Chem. Lett. 2007,
17, 3618.
(9) 4-(5-Cyclopropyl-1-methanesulfonylmethyl-1H-pyrazol-
4-yloxy)-2,6-dimethylbenzonitrile (15a)
1H NMR (400 MHz, CDCl3): d = 0.75 (m, 2 H), 0.90 (m, 2
H), 1.80 (m, 1 H), 2.45 (s, 6 H), 3.05 (s, 3 H), 5.35 (s, 2 H),
6.65 (s, 2 H), 7.40 (s, 1 H).
4-(3-Cyclopropyl-1-methanesulfonylmethyl-1H-pyrazol-
4-yloxy)-2,6-dimethylbenzonitrile (15b)
Figure 3 The most stable transition structure found for the potassi-
1H NMR (400 MHz, CDCl3): d = 0.85 (m, 4 H), 1.65 (m, 1
H), 2.45 (s, 6 H), 2.90 (s, 3 H), 5.10 (s, 2 H), 6.70 (s, 2 H),
7.45 (s, 1 H).
(10) All the calculations reported in this paper have been
performed within density functional theory,using the hybrid
three-parameter functional customarily denoted as B3LYP.
In all cases the standard 6-31G** basis set was used as
implemented in Jaguar package (Schrodinger, LLC,
Portland, Oregon). This level (B3LYP/6-31G**) has been
shown to be a convenient method for the computational
study of these types of reactions in terms of computational
cost and accuracy. Reactants and intermediates were
characterized by frequency calculations and have positive
definite Hessian matrixes. Transition structures (TS) show
only one negative eigenvalue in their diagonalized force
constant matrixes, and their associated eigenvectors were
confirmed to correspond to the motion along the reaction
coordinate under consideration. Nonspecific solvent effects
were partially taken into account by means of the standard
Poisson–Boltzmann continuum solvation model, where he
solvent is represented as a polarizable continuum (with
dielectric e) surrounding the molecular complex at an
interface constructed by combining atomic van der Waal
radii with the effective probe radius of the solvent. In several
cases molecular mechanics computations were performed on
several stationary points in order to determine the minimum
energy conformations. These calculations were performed
using the AMBER* force field as implemented in the
MacroModel package (Schrodinger, LLC, Portland,
Oregon). The different possible conformers were optimized
and then Monte Carlo simulations were performed on 1000
structures. All geometries are available on request to the
authors.
(11) 4-(3-Cyclopropyl-5-hydroxymethyl-1-methanesulfonyl-
methyl-1H-pyrazol-4-yloxy)-2,6-dimethylbenzonitrile (6)
Lithium borohydride (0.66 mL, 2 M in THF, 1.32 mmol)
was added dropwise to a solution of compound 24 (250 mg,
0.6 mmol) in THF (6 mL), under nitrogen, and the resulting
mixture was stirred for 30 min. The solvent was removed in
vacuo, and the residue was azeotroped with MeOH (25 mL).
The resulting solid was purified by flash chromatography
(silica gel) eluting with 70% EtOAc in pentane to afford
compound 6 as a white foam (180 mg, 80%). 1H NMR (400
MHz, CDCl3): d = 0.80 (m, 4 H), 1.60 (m, 1 H), 2.40 (t, 1 H),
2.45 (s, 6 H), 3.00 (s, 3 H), 4.60 (d, 2 H), 5.35 (s, 2 H), 6.65
(s, 2 H). Anal. Calcd for C18H21N3O4S·0.66H2O: C, 55.82; H,
5.81; N, 10.85. Found: C, 55.80; H, 5.76; N, 10.87.
CN
N
MeS
N
O
Oxone®
MeOH–H2O
EtO2C
23
O
CN
Me
25 °C, 6 h
N
S
N
O
O
LiBH4, THF
25 °C, 16 h
EtO2C
24
80%
O
CN
Me
N
S
N
O
O
HO
6
Scheme 7
References and Notes
(1) Bradley, P. A.; De Koning, P. D.; Johnson, P. S.;
Lecouturier, Y. C.; McManus, D. J.; Robin, A.; Underwood,
T. J. Org. Process Res. Dev. 2009, 13, 848.
(2) Narsaiah, A. V. Synlett 2002, 1178.
(3) Shinkre, B. A.; Velu, S. S. Synth. Commun. 2007, 37, 2399.
(4) Calverley, M. J. Tetrahedron 1987, 43, 4609.
(5) Del Carmen Cruz, M.; Tamariaz, J. Tetrahedron 2005, 61,
10061.
(6) Lebedev, A. V.; Lebedeva, A. B.; Sheludyakov, V. D.;
Kovaleva, E. A.; Ustinova, O. L.; Kozhevnikov, I. B. Russ.
J. Org. Chem. 2005, 75, 412.
(7) The pyrazoles can exit in two tautomeric forms, that is, the
hydrogen atom may be bound to either the N1 or N2 atom.
This tautomeric equilibrium has not been experimentally
studied in this manuscript, and the corresponding schemes
herein only show an arbitrary tautomer. The stability of both
pyrazole tautomers was computational analyzed for
compounds 12 and 20 in both gas phase and water solution
as the extreme media in terms of dielectric constant. In the
unsubstituted case 12, the tautomers are almost equally
stable in both media (0.7 and 0.0 kcal/mol, respectively, in
favor of N2–H tautomer). On the other hand, in the case of
compound 20, the stabilizing electrostatic interaction
between N2–H and lone pair of the carbonyl group involves
Synlett 2010, No. 6, 873–876 © Thieme Stuttgart · New York