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Volumn 102, Issue 16, 1980, Pages 5169-5176

The Quinones of Azulene. A Theoretical Prognosis

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EID: 0000756257     PISSN: 00027863     EISSN: 15205126     Source Type: Journal    
DOI: 10.1021/ja00536a007     Document Type: Article
Times cited : (54)

References (71)
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    • 1971, 49 (June 7), 34-51. See, however. Packer, L.; Smith, J. R. Proc. Natl. Acad. Sci. U.S.A.
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    • Topics in Nonbenzenoid Aromatic Chemistry
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    • 1978, 100, 5268-5271, and references cited therein. Nakagawa, M. Agnew. Chem., Int. Ed. Engl., 18, 204-214, and references cited therein.
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    • For a discussion of aromaticity in annulenones see
    • For a discussion of aromaticity in annulenones see: Hess, B. A., Jr.; Schaad, L. J.; Holyoke, C. W., Jr. Tetrahedron 1972, 28, 3299-3305.
    • (1972) Tetrahedron , vol.28 , pp. 3299-3305
    • Hess, B.A.1    Schaad, L.J.2    Holyoke, C.W.3
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    • 1969, 91, 789-795. Dewar, M. J. S.; Morita, T. Tetrahedron., 91
    • Dewar, M. J. S.; deLlano, C. J. Am. Chem. Soc. 1969, 91, 789-795. Dewar, M. J. S.; Morita, T. Tetrahedron. 1969, 91, 796-802, 802-806.
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    • Part 2 1974, 4(2), 1-362. “Proceedings of the Symposium on Quinones as Anticancer Agents”, Driscoll, J. S., Ed. J. Am. Chem. Soc. 4(A)
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    • (1974) Cancer Chemother. Rep. , pp. 1-33
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    • 1975, 97, 1285-1293, 1294-1301, 1302-1306, Dewar, M. J. S.; Lo, D. H.; Ramsden, C. A. Hückel Molecular Orbital Theory”; Academic Press: New York.
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    • X-ray structure of azulene: 1962, 15, 1. X-ray structure of naphthalene: Cruickshank, D. W. J.; Sparks, R. A. Proc. R. Soc. London, Ser. A
    • X-ray structure of azulene: Robertson, J. M.; Shearer, H. M. M.; Sim, G. A.; Watson, D. G. Acta Crystallogr. 1962, 15, 1. X-ray structure of naphthalene: Cruickshank, D. W. J.; Sparks, R. A. Proc. R. Soc. London, Ser. A 1960, 258, 270.
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    • These values were estimated from Allinger's potentials for bending strain [Allinger, N. L.; Tribble, M. T.; Miller, M. A.; Werz, D. H. J. Am Chem. Soc. 1971, 93, 1637-1648] applied to MINDO/3-optimized geometries of 26-AQ and 26-NQ, respectively, and seem in line with the previously quoted value of 16 kcal/mol for the strain energy of azulene [Streitwieser, A., Jr. “Molecular Orbital Theory for Organic Chemists”; Wiley: New York, p 244].
    • A strain energy of 18,7 kcal/mol was assumed for the azuloquinones and 2.6 kcal/mol for the naphthoquinones. These values were estimated from Allinger's potentials for bending strain [Allinger, N. L.; Tribble, M. T.; Miller, M. A.; Werz, D. H. J. Am Chem. Soc. 1971, 93, 1637-1648] applied to MINDO/3-optimized geometries of 26-AQ and 26-NQ, respectively, and seem in line with the previously quoted value of 16 kcal/mol for the strain energy of azulene [Streitwieser, A., Jr. “Molecular Orbital Theory for Organic Chemists”; Wiley: New York, 1961; p 244].
    • (1961) A strain energy of 18,7 kcal/mol was assumed for the azuloquinones and 2.6 kcal/mol for the naphthoquinones.
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    • 1975, Fleming, I. “Frontier Orbitals and Organic Chemical Reactions”; Wiley: New York
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    • Organic Syntheses
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    • Prentice-Hall: Englewood Cliffs, N.J., 1975; Chapter 7. The program used for these calculations was written by Simmons (Simmons, H. E. Prog. Org. Chem. 1970, 7, 1) and extensively modified by M. D. Gordon. Two-center integrals were calculated by the method of Nishimoto and Mataga (Nishimoto, K.; Mataga, N. Z. Phys. Chem. (Frankfurt am Main) 1957, 12, 335), and core resonance integrals were calculated by the method of Nishimoto and Forster (Nishimoto, K.; Forster, L. S. Theor. Chim. Acta, 3, 407). Ionization potentials and one-center electron repulsion integrals were taken as-11.16 and 11.13 eV for carbon and-17.70 and 15.23 eV for oxygen.
    • See, for example, Borden, W. T. “Modern Molecular Orbital Theory for Organic Chemists”; Prentice-Hall: Englewood Cliffs, N.J., 1975; Chapter 7. The program used for these calculations was written by Simmons (Simmons, H. E. Prog. Org. Chem. 1970, 7, 1) and extensively modified by M. D. Gordon. Two-center integrals were calculated by the method of Nishimoto and Mataga (Nishimoto, K.; Mataga, N. Z. Phys. Chem. (Frankfurt am Main) 1957, 12, 335), and core resonance integrals were calculated by the method of Nishimoto and Forster (Nishimoto, K.; Forster, L. S. Theor. Chim. Acta 1965, 3, 407). Ionization potentials and one-center electron repulsion integrals were taken as-11.16 and 11.13 eV for carbon and-17.70 and 15.23 eV for oxygen.
    • (1965) Modern Molecular Orbital Theory for Organic Chemists
    • Borden, W.T.1
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    • In ref 30
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    • 1977, 2511. See also: Bischof, P.; Gleiter, R.; Hafner, K.; Knauer, K. H.; Spanget-Larsen, J.; Suss, H. U. Chem. Ber.
    • Pentalene X-ray: Kitschke, B.; Lindner, H. J. Tetrahedron Lett. 1977, 2511. See also: Bischof, P.; Gleiter, R.; Hafner, K.; Knauer, K. H.; Spanget-Larsen, J.; Suss, H. U. Chem. Ber. 1978, 111, 932.
    • (1978) Tetrahedron Lett. , vol.111 , pp. 932
    • Kitschke, B.1    Lindner, H.J.2


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