(q, J = 7.3, 6H), 3.88 (s, 3H), 7.51 (t, J = 7.6 Hz, 2H); 7.83 (dd, J =
7.1, 1.3 Hz, 1H); 7.88 (dd, J = 7.1, 1.3 Hz, 1H); 7.91 (dd, J = 8.2,
1.3 Hz, 1H); 8.03 (dd, J = 8.2, 1.3 Hz, 1H). ESI-MS negative-ion
on the energetic results obtained in gas phase were included by
means of the polarizable continuum model (PCM)20 on single
point calculations, with the molecular cavity computed, including
explicit hydrogens, with the UFF radius21 allowing calculation
of the Gibbs solvation free energy (DGsolvation). Using a simplified
model (PCM) to describe solvation effects does not account for
specific solvent–solute interactions (e.g. hydrogen bonds) that are
certainly important in this particular reaction in aqueous solution.
Therefore, in all calculations, we included one water molecule to
begin to account for the kinetic solvent isotope effect observed
experimentally. The total free energy in solution (Gsolution) was
calculated by summing the electronic and thermal free energies
to DGsolvation. For conversion from 1 atm standard state to 1 mol L-1
standard state, DGeq from 1c·H2O to MeOH+H2O+NA shown in
Fig. 6 was corrected22 by adding 3.79 kcal mol-1 to the calculated
value according to an A → B + C + D reaction. For structures
of 1c·H2O and TI·H2O the basis set superposition error (BSSE)
was estimated using the Counterpoise method23 implemented in
Gaussian 03. Theoretical calculations for cyclization involving a
number of explicit water molecules, although possible, were not of
interest for this work.
-
mode: m/z (%): calc for C13H9O4 : 229.05; found: 229.05 (100).
4.1.3 n-Isopropyl monoester of 1,8-naphthalic acid (1b). To a
solution containing 0.198 g (1.0 mmol) of 1,8-naphthalic acid in
20 mL of isopropanol at 50 ◦C was added 0.21 mL (1.5 mmol) of
triethylamine, and the reaction was maintained under stirring for
1
12 h. H NMR (400 MHz, CD3CN): d 1.02 (t, J = 7.2 Hz, 9H),
1.18 (d, J = 6.0 Hz, 3H), 1.36 (d, J = 6.3 Hz, 3H), 2.55 (q, J = 7.2
Hz, 6H), 5.14 (quint, J = 6.2, 1H), 7.50 (dd, J = 8.2, 7.1 Hz, 1H),
7.51 (dd, J = 8.2, 7.1 Hz, 1H), 7.78 (dd, J = 7.1, 1.4 Hz, 1H); 7.89
(dd, J = 8.2, 1.4 Hz, 1H); 7.94 (dd, J = 7.1, 1.4 Hz, 1H); 8.01 (dd, J
= 8.2, 1.4 Hz, 1H). ESI-MS negative-ion mode: m/z (%): calc for
-
C15H13O4 : 257.10; found: 257.00 (100).
4.2 Kinetics
Rates of formation of the anhydrides from monoesters of 1,8-
naphthalic acid were followed on a spectrophotometer coupled
with a thermostated water-jacketed cell holder. All solutions were
prepared with CO2 free distilled, demineralized water which was
boiled and cooled under nitrogen. Reactions were initiated by
injection of 10 mL of ca. 10 mM solutions of substrates into 3
mL of buffer solutions. Absorbance versus time data were stored
Acknowledgements
We are grateful to INCT-Catalise, PRONEX, FAPESC, CNPq,
´
directly on a microcomputer and first-order rate constants (kobs
)
and CAPES for support of this work.
were calculated from linear plots, at the wavelength maximum of
340 nm, of ln(A• - At) against time for at least 90% reaction by
using an iterative least-squares program; correlation coefficients
(r) were > 0.999 for all kinetic runs. At conditions where the rate
constant for NA hydrolysis is similar to its formation, absorbance
vs. time data were fitted with eqn (2), according to Scheme 6,5a
with k1 π k2.
Notes and references
1 (a) From enzyme models to model enzymes, A. J. Kirby and F. Hollfelder,
RSC Publishing, Cambridge, 2009; (b) F. M. Menger and M. Ladika, J.
Am. Chem. Soc., 1988, 110, 6794–6796; (c) A. J. Kirby, Acc. Chem. Res.,
1997, 30, 290–296; (d) V. G. Machado and F. Nome, Chem. Commun.,
1997, 1917–1918; (e) V. G. Machado, C. A. Bunton, C. Zucco and F.
Nome, J. Chem. Soc., Perkin Trans. 2, 2000, 169–173.
2 (a) D. L. Rabenstein, T. S. Shi and S. Spain, J. Am. Chem. Soc., 2000,
122, 2401–2402; (b) C. Cox and T. Lectka, J. Am. Chem. Soc., 1998,
120, 10660–10668; (c) K. Bowden and A. Brownhill, J. Chem. Soc.,
Perkin Trans. 2, 1997, 219–221; (d) F. Hollfelder, A. J. Kirby and D.
S. Tawfik, J. Org. Chem., 2001, 66, 5866–5874; (e) N. Asaad and A. J.
Kirby, J. Chem. Soc., Perkin Trans. 2, 2002, 1708–1712.
t
t
2
k1(e−k t −e−k
)
k2e−k t −k1e−k
1
2
1
⎧
⎫
⎪
⎪
−k t
⎪
⎪
⎬
⎪
1
Abs = Ester 1+e
+
+
[
]
⎨
⎪
0
k2 −k1
k1 −k2
⎪
⎩
⎪
⎭
(2)
3 (a) Structure and Mechanism in Protein Science: A Guide to Enzyme
Catalysis and Protein Folding, 1st Edition, A. R. Fersht and W. H.
Freeman, New York, 1998; (b) A. B. Onofrio, A. C. Joussef and F.
Nome, Synth. Commun., 1999, 29, 3039–3049; (c) A. B. Onofrio, J. C.
Gesser, A. C. Joussef and F. Nome, J. Chem. Soc., Perkin Trans. 2, 2001,
1863–1868; (d) Z. J. Wu, F. Q. Ban and R. J. Boyd, J. Am. Chem. Soc.,
2003, 125, 3642–3648.
4 A. J. Kirby, N. Dutta-Roy, D. da Silva, J. M. Goodman, M. F. Lima,
C. D. Roussev and F. Nome, J. Am. Chem. Soc., 2005, 127, 7033–7040.
5 (a) T. C. Barros, S. Yunes, G. Menegon, F. Nome, H. Chaimovich, M.
J. Politi, L. G. Dias and I. M. Cuccovia, J. Chem. Soc., Perkin Trans. 2,
2001, 2342–2350; (b) S. F. Yunes, J. C. Gesser, H. Chaimovich and F.
Nome, J. Phys. Org. Chem., 1997, 10, 461–465.
Scheme 6
4.3 Computational methods
6 (a) E. S. Orth, T. A. S. Brandao, B. S. Souza, J. R. Pliego, B. G. Vaz,
M. N. Eberlin, A. J. Kirby and F. Nome, J. Am. Chem. Soc., 2010, 132,
8513–8523; (b) M. Silva, R. S. Mello, M. A. Farrukh, J. Venturini, C. A.
Bunton, H. M. S. Milagre, M. N. Eberlin, H. D. Fiedler and F. Nome,
J. Org. Chem., 2009, 74, 8254–8260; (c) E. S. Orth, P. L. F. da Silva, R.
S. Mello, C. A. Bunton, H. M. S. Milagre, M. N. Eberlin, H. D. Fiedler
and F. Nome, J. Org. Chem., 2009, 74, 5011–5016; (d) E. S. Orth, T. A. S.
Brandao, H. M. S. Milagre, M. N. Eberlin and F. Nome, J. Am. Chem.
Soc., 2008, 130, 2436–2437; (e) J. B. Domingos, E. Longhinotti, T. A.
S. Brandao, L. S. Santos, M. N. Eberlin, C. A. Bunton and F. Nome, J.
Org. Chem., 2004, 69, 7898–7905; (f) J. B. Domingos, E. Longhinotti,
T. A. S. Brandao, C. A. Bunton, L. S. Santos, M. N. Eberlin and F.
Nome, J. Org. Chem., 2004, 69, 6024–6033.
Gaussian 03 (Revision D.01)16 program was used for all cal-
culations. The B3LYP17 hybrid functional with the 6-31+G(d)
basis set was employed and the stationary points were verified
by calculating the Hessians matrix, where the minimum energy
structures have no imaginary frequency and transition state
structures have one imaginary frequency. To obtain a deeper
insight into the reaction mechanism, we calculated the intrinsic
reaction coordinate (IRC)18 using the Gonzalez–Schlegel second-
order path,19 starting from the optimized transition-state structure,
with a step length of 0.01 a.m.u.1/2 (Bohr). The solvent effects
This journal is
The Royal Society of Chemistry 2011
Org. Biomol. Chem., 2011, 9, 6163–6170 | 6169
©