1-(9-Phenanthryl)-2-naphthylacetonitrile (4f). 1H NMR dH
3.57 (c, 2H); 7.18–7.21 (dd, 1H); 7.27–7.33 (m, 3H); 7.40–7.43
(cd, 1H); 7.48–752 (cd, 1H); 7.66–7.70 (m, 2H); 7.75–7.79
(m, 2H); 7.92 (d, 1H); 7.96 (d, 1H); 8.06 (d, 1H); 8.82
(t, 2H). 13C NMR dC 22.33; 118.12 (q); 122.71; 123.18; 125.68;
126.25; 126.44; 126.64 (q); 126.74; 126.88; 127.17; 127.20; 127.32;
127.34; 128.05; 129.03; 129.13; 130.44 (q); 130.70 (q); 131.11 (q);
131.40 (q); 133.02 (q); 133.28 (q); 133.64 (q); 136.95 (q). m/z =
344 (40); 343 (60); 316 (100); 304 (11); 303 (15); 302 (14); 157 (18);
151 (26). MS m/z: 343 (M+, 100). Exact mass calcd for C26H17N:
343.13610; found: 343.13639.
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a-(4-Cyanophenyl)-2-naphthylacetonitrile (3g). H NMR dH
2812–2815 (Chem. Abstr., 1982, 96, 104049r); Ya. L. Gol’dfarb,
´
5.35 (s, 1H); 7.31 (d, 1H), 7.52–7.56 (m, 4H); 7.68 (d, 2H);
7.85–7.86 (m, 4H). 13C NMR dC 42.74; 112.63 (q); 118.05 (q);
118.52 (q); 124.79; 127.06; 127.15; 127.18; 127.83; 128.01;
128.67; 129.76; 131.63 (q); 133.00 (q); 133.04 (q); 133.25 (q);
140.84 (q). m/z = 269 (19); 268 (100); 267 (54); 241 (15); 240
(50); 166 (21); 140 (11); 139 (13); 127 (11); 120 (13); 107 (15);
106 (11); 77 (10); 63 (9). MS m/z: 268 (M+, 100). Exact mass
calcd for C19H12N2: 268.10004; found: 268.10004.
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Acknowledgements
15 M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria,
M. A. Robb, J. R. Cheeseman, J. A. Montgomery, T. Vreven,
Jr., 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,
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H. P. Hratchian, J. B. Cross, C. Adamo, J. Jaramillo,
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GAUSSIAN 03 (Revision B.04), Gaussian, Inc., Pittsburgh, PA,
2003.
16 The solvent effect was modelled with Tomasi’s polarised conti-
nuum model (PCM) [S. Miertus, E. Scrocco and J. Tomasi, Chem.
Phys., 1981, 55, 117; S. Miertus and J. Tomasi, Chem. Phys., 1982,
65, 239; M. Cossi, B. Barone, R. Camini and J. Tomasi, Chem.
Phys. Lett., 1996, 255, 327.]. The solvent effect was evaluated from
single point PCM calculations on the gas-phase optimized geome-
tries at the B3LYP/6-31G* theory level, electrostatic and non-
electrostatic contributions being considered. In the PCM model the
solvent is represented as a polarizable continuum (with dielectric
constant e) surrounding the molecular complex at an interface
constructed by combining atomic van der Waals radii with the
effective probe radius of the solvent. Charges are allowed to
develop on this interface according to the electrostatic potential
of the solute and e, then the polarized reaction field of the solvent
acts back on the quantum mechanical description of the solute.
The wave function of the complex is relaxed self-consistently with
the reaction field to solve the Poisson–Boltzmann (PB) equations.
The solvent was represented with the following parameters: di-
electric constant and probe radius.
This work was supported by Agencia Co
Consejo Nacional de Investigaciones Cientı
(CONICET) and SECyT, Universidad Nacional de Co
´
rdoba Ciencia (ACC),
ficas y Tecnicas
rdoba,
´
´
´
Argentina.
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This journal is The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2012