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34
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34250822454
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13C NMR spectra of (R)-1 are identical to those of (S)-1.
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13C NMR spectra of (R)-1 are identical to those of (S)-1.
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35
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34250876457
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The signals for the four pyrrole NH protons of calix[4]pyrrole (S)-1 were found to disappear upon the addition of 1.0-1.2 equivalents of (S)-2-phenylbutyrate.
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The signals for the four pyrrole NH protons of calix[4]pyrrole (S)-1 were found to disappear upon the addition of 1.0-1.2 equivalents of (S)-2-phenylbutyrate.
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37
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34250877057
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ITC measurements were performed as follows: Solutions of the chosen receptor in acetonitrile were made up so as to provide a receptor concentration range of 0.1-1 mM. These solutions were then individually titrated with the appropriate alkylammonium salts at (30 ± 0.01)°C. The original heat pulses were normalized using reference titrations carried out using the same salt solution but in pure acetonitrile.
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b) ITC measurements were performed as follows: Solutions of the chosen receptor in acetonitrile were made up so as to provide a receptor concentration range of 0.1-1 mM. These solutions were then individually titrated with the appropriate alkylammonium salts at (30 ± 0.01)°C. The original heat pulses were normalized using reference titrations carried out using the same salt solution but in pure acetonitrile.
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38
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34250840760
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Non-linear curve-fittings were performed with Origin 7.0 (OriginLab Co.) using a 1:1 fitting program provided by the ITC manufacturer (MicroCal, Inc.).
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Non-linear curve-fittings were performed with Origin 7.0 (OriginLab Co.) using a 1:1 fitting program provided by the ITC manufacturer (MicroCal, Inc.).
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39
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34250853668
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An initial conformational analysis of each molecular system was performed by molecular dynamics (MD) simulation using the SANDER module of AMBER employing the parm99 force field.[14] From the MD simulation trajectory for each molecular system, a total of 200 structures were collected which were then subjected to an optimization procedure using the AM1 semi-empirical method[15] to find the energy minima that would be used as initial structures for the DFT calculations at the B3LYP/ 3-21G level[16] using the Gaussian 98 package.[17] Frequency calculations were performed to verify the identity of each stationary point as a minimum. To provide a more complete description of the interactions with anionic guests, single-point energy calculations were then carried out at the B3LYP/6-31G+ G* level using the optimized geometries obtained from the B3LYP/3-21G* analyses
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[17] Frequency calculations were performed to verify the identity of each stationary point as a minimum. To provide a more complete description of the interactions with anionic guests, single-point energy calculations were then carried out at the B3LYP/6-31G+ G* level using the optimized geometries obtained from the B3LYP/3-21G* analyses.
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40
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34250804962
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University of California, San Francisco
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D. A. Case, D. A. Pearlman, J. W. Caldwell, et al. see Supporting Information, AMBER 7, University of California, San Francisco, 2002.
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(2002)
Supporting Information, AMBER 7
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42
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0842341771
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b) M. J. S. Dewar, E. G. Zoebisch, E. F. Healy, J. Am. Chem. Soc. 1985, 107, 3902-3909.
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Dewar, M.J.S.1
Zoebisch, E.G.2
Healy, E.F.3
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44
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34250888301
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M. J. Frisch et al. see Supporting Information, Gaussian 98, Revision A.7 Gaussian, Inc., Pittsburgh PA, 1998.
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M. J. Frisch et al. see Supporting Information, Gaussian 98, Revision A.7 Gaussian, Inc., Pittsburgh PA, 1998.
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45
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34250885314
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Subsequent to submission of this manuscript a single-crystal X-ray structure of a 3,3′-dibromonaphthyl derivative of (S)-1 was obtained. This structure proved analogous to that calculated for receptor (S)-1 in the absence of an added substrate.
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Subsequent to submission of this manuscript a single-crystal X-ray structure of a 3,3′-dibromonaphthyl derivative of (S)-1 was obtained. This structure proved analogous to that calculated for receptor (S)-1 in the absence of an added substrate.
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