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1H NMR data showed significantly different (absolute) 2JC2,H3ax and 2J C2,H3eq values in 1αp (7.7 and 4.3 Hz, respectively, whereas nearly identical couplings were observed in 1βp (∼3.6 Hz, As reported previously for 3JC1,H3ax and 3J C1,H3eq (Hori, H, Nakajima, T, Nishida, Y, Ohrui, H, Meguro, H. Tetrahedron Lett. 1988, 29, 6317-6320, 2JC2,H3ax and 2J C2,H3eq can be used to distinguish between 1αp and 1βp see ref 34
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C2,C3 = 44.0 Hz).
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C2,C3 = 44.0 Hz).
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51749122913
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CCC values in unsaturated systems mimics that observed in saturated systems (Klepach, T.; Carmichael, I.; Serianni, A. S., unpublished results).
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CCC values in unsaturated systems mimics that observed in saturated systems (Klepach, T.; Carmichael, I.; Serianni, A. S., unpublished results).
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a, and n were optimized simultaneously during the data fit using the Solver Routine in Microsoft Excel.
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Larger disparities between calculated and experimental J-couplings are not considered to arise from inherent limitations of the DFT methodology but rather from simplifications and assumptions in the structural models used to calculate the couplings. In saccharides, the latter often involve the conformational properties of exocyclic OH groups, which can exert a major effect on both JCH and JCC values. Density functional theory with the B3LYP functional is known to produce accurate structural and energetic parameters in most organic molecules. This particular functional is specifically parametrized to reproduce accurate thermochemistry and matches closely results from high-level composite methods such as the Gaussian03 approach. Work in this laboratory and by other investigators has shown high agreement between B3LYP predictions of indirect nuclear spin-spin coupling constants and calculated couplings obtained by accurate high-level coupl
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CC (Cloran, F.; Carmichael, I.; Serianni, A. S. J. Phys. Chem. A 1999, 103, 3783-3795).
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