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(ꢂ/2 in both dimensions) window functions, and processed
with the Bruker software package.
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Anticancer Res. 1999; 19(1A): 269.
Calculations
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All calculations were carried out with the Gaussian 98
program.12 Geometry optimization of the conformations
of 3 and 4 was performed without constraints at the
B3LYP/6–31G(d) level. The population percentages were
calculated from the gas-phase electronic energies of the
conformers through the Boltzmann equation at 298K; the
entropic terms were neglected. Attempts to evaluate the
influence of the solvent on the relative energies of the
conformers were made using a continuum solvent model
(C-PCM)19 at different dielectric constant values, but the
runs stopped without completion owing to the molecular
size of 3 and 4. However, solvent calculations on smaller
models of 3 and 4 lacking the D ring could be performed and
confirmed the preference for conformers such as 3A and 4A.
NMR chemical shifts were calculated at the Hartree–Fock
and density functional levels with the 6–31G(d) or the
10. Palmer KH, Cook CE, Ross FT, Dolar J, Twine ME, Wall ME.
Steroids 1969; 14: 55.
11. (a) Lee C, Yang W, Parr RG. Phys. Rev.
(b) Becke AD. J. Chem. Phys. 1993; 98: 5648.
B 1988; 37: 785;
12. Frisch MJ, Trucks GW, Schlegel HB, Scuseria GE, Robb MA,
Cheeseman JR, Zakrzewski VG, Montgomery JA Jr, Stratmann
RE, Burant JC, Dapprich S, Millam JM, Daniels AD, Kudin KN,
Strain MC, Farkas O, Tomasi J, Barone V, Cossi M, Cammi
R, Mennucci B, Pomelli C, Adamo C, Clifford S, Ochterski J,
Petersson GA, Ayala PY, Cui Q, Morokuma K, Malick DK,
Rabuck AD, Raghavachari K, Foresman JB, Cioslowski J, Ortiz
JV, Baboul AG, Stefanov BB, Liu G, Liashenko A, Piskorz P,
Komaromi I, Gomperts R, Martin RL, Fox DJ, Keith T, Al-Laham
MA, Peng CY, Nanayakkara A, Challacombe M, Gill PMW,
Johnson B, Chen W, Wong MW, Andres JL, Gonzalez C, Head-
Gordon M, Replogle ES, Pople JA. Gaussian 98, Revision A.9.
Gaussian Inc.: Pittsburgh, PA, 1998.
13. Haasnoot CAG, de Leeuw FAAM, Altona C. Tetrahedron 1980;
36: 2783.
14. (a) Wolinski K, Hilton JF, Pulay P. J. Am. Chem. Soc. 1990; 112:
8251; (b) Ditchfield R. Mol. Phys. 1974; 27: 789.
15. Cheeseman JR, Trucks GW, Keith TA, Frisch MJ. J. Chem. Phys.
1996; 104: 5497.
1
6–31G(d,p) basis sets using the GIAO method. All the H
and 13C chemical shifts are referenced to those of TMS.
The absolute 1H and 13C shielding of TMS, based on the
B3LYP/6–31G(d) optimized geometry, were calculated at
the same level/basis set used in the calculation to which they
refer.
Acknowledgments
This work was financially supported by the Universita` degli Studi
di Milano and Universita` degli Studi di Pavia.
16. (a) Eloranta J, Hu J, Suontamo R, Kolehmainen E, Knuutinen J.
Magn. Reson. Chem. 2000; 38: 987; (b) Casanovas J, Namba AM,
Leo´n S, Aquino GLB, da Silva GVJ, Alema´n C. J. Org. Chem. 2001;
66: 3775; (c) Kupka T, Pastema G, Jaworska M, Karali A, Dais P.
Magn. Reson. Chem. 2000; 38: 149; (d) Smith WB. Magn. Reson.
Chem. 1999; 37: 103.
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Copyright 2002 John Wiley & Sons, Ltd.
Magn. Reson. Chem. 2002; 40: 581–588