135.8; 149.6; 167.4. HRMS [MH]+ calc. for C11H17O2Sn
301.0245, found: 301.0249.
and W. Y. Su, Organometallics, 1984, 3, 1718–1727; J. San
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2 R. A. Rossi, A. B. Pierini and A. B. Pene
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stimulated RN1 Process: Reaction of Haloarenes with
´
nory, Chem. Rev.,
Methyl 2-(trimethylstannyl)benzoate (7b). This was isolated
´
nory, The Photo-
as an amber liquid after Kugelrohr distillation (50 1C/1mmHg).
¨
(EI+) m/z (%): 289 (16), 287 (13), 286 (8), 285 (100), 284 (20),
S
Carbanions, in CRC Handbook of Organic Photochemistry
and Photobiology, ed. W. M. Horspool and F. Lenel, CRC
Press, Boca Raton, USA, 2nd edn, 2004, pp. 47; R. A. Rossi,
Photoinduced Aromatic Nucleophilic Substitution Reactions, in
Synthetic Organic Photochemistry, ed. A. G. Griesbeck and
J. Mattay, Marcel Dekker, New York, 2005, pp. 495–527.
3 A. N. Santiago, S. M. Basso, J. P. Montanez and R. A. Rossi,
J. Phys. Org. Chem., 2006, 19, 829–835.
4 S. M. Basso, J. P. Montanez and A. N. Santiago, Lett. Org. Chem.,
2008, 5, 633–639.
5 R. K. Ingham, S. D. Rosenberg and H. Gilman, Chem. Rev., 1960,
60, 459–539.
6 The equation used in the relative reactivity determination of pairs
283 (69), 282 (24), 281 (42), 255 (55), 254 (11), 253 (38), 251
1
(23). H-NMR (400.16 MHz, CDCl3) d: 0.31 (9H, s, JH–Sn
=
27.4 Hz); 3.95 (3H, s); 7.40–7.48 (1H, t); 7.51–7.60 (1H, t);
7.64–7.80 (1H, d); 8.11–8.20 (1H, d); 13C-NMR (CDCl3) d:
ꢀ7.4; 52.3; 128.3; 129.9; 131.9; 135.8; 136.5; 146.9; 168.9. HRMS
[MH]+ calc. for C11H17O2Sn 301.0245, found: 301.0236.
Methyl 3-(trimethylstannanyl)benzoate (7c). This was
isolated as an amber liquid after Kugelrohr distillation
¨
(50 1C/1mmHg). EM (EI+) m/z (%): 289 (18), 287 (14), 286
(10), 285 (100), 284 (30), 283 (74), 282 (26), 281 (43), 255 (24),
254 (6), 253 (171), 251 (10). 1H-NMR (400.16 MHz, CDCl3) d:
0.34 (9H, s, JH–Sn = 27.4 Hz); 3.94 (3H, s); 7.39–7.45 (1H, t);
7.60–7.80 (1H, d); 7.95–8.05 (1H, d); 8.10–8.30 (1H, s);
13C-NMR (CDCl3) d: ꢀ9.4; 52.0; 127.8; 129.4; 129.5; 136.7;
140.3; 142.8; 167.5. HRMS [MH]+ calc. for C11H17O2Sn
301.0245, found: 301.0253.
of substrate vs. nucleophile was: k4/k5
= ln([substrate 4]0/
[substrate 4]t)/ln([substrate 5]0/[substrate 5]t), where [substrate 4]0
and [substrate 5]0 are initial concentrations and [substrate 4]t and
[substrate 5]t are concentrations at time t of both substrates,
see: J. F. Bunnett, in Investigation of Rates and Mechanisms of
Reactions, ed. E. S. Lewis, Wiley-Interscience, New York, 3rd edn,
1974, part 1, pp. 159.
7 D. D. Tanner, J. J. Chen, L. Chen and C. Luelo, J. Am. Chem.
Soc., 1991, 113, 8074–8881.
8 A. B. Pierini, J. S. Duca and M. A. Vera, J. Chem. Soc., Perkin
Trans. 2, 1999, 1003–1009.
Methyl 5-chloro-2-(trimethylstannanyl)benzoate (3). This
9 A. B. Pierini and J. S. Duca, J. Chem. Soc., Perkin Trans. 2, 1995,
1821–1828.
10 A. B. Pierini and D. M. A. Vera, J. Org. Chem., 2003, 68,
9191–9199.
11 D. M. Chipman, J. Chem. Phys., 2000, 112, 5558–5565;
M. T. Cances, B. Mennucci and J. Tomasi, J. Chem. Phys., 1997,
107, 3032–3041.
12 Mass Spectra, in NIST Chemistry WebBook, NIST Standard
Reference Database Number 69, ed. P. J. Linstrom and W. G.
Mallard, March 2003, National Institute of Standards and
nist.gov).
was isolated as a yellow oil after Kugelrohr distillation
¨
1
(50 1C/1mmHg). H-NMR (CDCl3) d: 0.27 (9H, s, JH–Sn
=
27 Hz); 3.92 (3H, s); 7.49–7.61 (2H, m); 8.08–8.09 (1H, d).
13C-NMR (CDCl3) d: ꢀ7.4; 52.5; 129.8; 131.79; 137.7; 167.8.
EM (EI+) m/z (%): 319 (100), 317 (73), 302 (4), 289 (50), 287
(36), 272 (3), 261(6), 259 (14), 231 (5), 165 (2), 151 (24), 133 (7),
118 (5), 89 (5), 75 (7), 63 (4). HRMS (CI) exact mass calc. for
the C11H15ClO2Sn (M+ ꢀ CH3) 318.9548, found (M+ ꢀ CH3)
318.9553.
13 CRC Handbook of Chemistry and Physics 78th edition, CRC Press
Inc., Boca Raton, USA, 1997.
Computational procedures
All calculations were carried out with DFT14 methods, as
implemented in the Gaussian 03 package,15 by employing the
B3LYP16 functional at the 6-31+G* level of theory. This basis
set is known to be appropriate for the theoretical study of the
electronic and geometric properties of RAs.17 Stationary
points were characterized by the normal analysis and obtained
with complete geometry optimization without symmetry
restrictions. Potential energy surfaces (PES) were obtained
by varying the C–Cl bond length, and the B3LYP spin
contamination along the whole fragmentation path was
negligible (hS2i = 0.750–0.751). The solvation effect was
included by using a continuous model in acetonitrile solvent.
14 W. Kohn and I. Sham, Phys. Rev., 1965, 140, A1133–A1138.
15 M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria,
M. A. Robb, J. R. Cheeseman, J. A. Montgomery, Jr.,
T. Vreven, K. N. Kudin, J. C. Burant, J. M. Millam,
S. S. Iyengar, J. Tomasi, V. Barone, B. Mennucci, M. Cossi,
G. Scalmani, N. Rega, G. A. Petersson, H. Nakatsuji, M. Hada,
M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida,
T. Nakajima, Y. Honda, O. Kitao, H. Nakai, M. Klene, X. Li,
J. E. Knox, H. P. Hratchian, J. B. Cross, V. Bakken, C. Adamo,
J. Jaramillo, R. Gomperts, R. E. Stratmann, O. Yazyev,
A. J. Austin, R. Cammi, C. Pomelli, J. Ochterski, P. Y. Ayala,
K. Morokuma, G. A. Voth, P. Salvador, J. J. Dannenberg,
V. G. Zakrzewski, S. Dapprich, A. D. Daniels, M. C. Strain,
O. Farkas, D. K. Malick, A. D. Rabuck, K. Raghavachari,
J. B. Foresman, J. V. Ortiz, Q. Cui, A. G. Baboul, S. Clifford,
J. Cioslowski, B. B. Stefanov, G. Liu, A. Liashenko, P. Piskorz,
I. Komaromi, R. L. Martin, D. J. Fox, T. Keith, M. A. Al-Laham,
C. Y. Peng, A. Nanayakkara, M. Challacombe, P. M. W. Gill,
B. G. Johnson, W. Chen, M. W. Wong, C. Gonzalez and
J. A. Pople, GAUSSIAN 03 (Revision B.02), Gaussian, Inc.,
Wallingford, CT, 2004.
Acknowledgements
This work was supported in part by ACC, CONICET,
SECYT and ANPCyT. J. P. M. and J. G. U. gratefully
acknowledge receipt of fellowships from CONICET.
16 C. Lee, W. Yang and R. G. Parr, Phys. Rev. B: Condens.
Matter, 1988, 37, 785–789; A. D. Becke, Phys. Rev. A: At.,
Mol., Opt. Phys., 1988, 38, 3098–3100; E. Miehlich, A.
Savin, H. Stoll and H. Preuss, Chem. Phys. Lett., 1989, 157,
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