Substituent-induced chemical shifts (SCS) by the phenyl group in sterically congested styrene derivatives

1993 ◽  
Vol 31 (4) ◽  
pp. 388-393 ◽  
Author(s):  
Rudolf Knorr ◽  
David S. Stephenson ◽  
Petra Böhrer ◽  
Thi-Phung Hoang
2000 ◽  
Vol 14 (4) ◽  
pp. 259-267 ◽  
Author(s):  
Manuel A. Leiva ◽  
Raul G. E. Morales

By means of13C‒NMR spectroscopy and ab initio molecular orbital theory calculations, we have analyzed the bridge effect of the C=C, C=N and N=N bonds on the long distance charge transfer of4‒dimethylamino‒4'‒nitrostilbenoid compounds in the ground electronic state.After a complete spectral assignment of the13C‒NMR signals in these molecular compounds, we have characterized the effect of the nitrogen centres on the molecular bridge by means of the chemical shifts of the carbon centres, the theoretical charge densities and the dipolar moments.From an electronic molecular point of view, our results describe two main properties of the double bond bridge. The first is related to the local charge accumulation capacity given by the type of the atomic centres and the structural orientation of the double bond bridge, and the second property is related to the modulation of the electronic charge distribution through the molecular system by the electrical polarization of the bridge.Other complementary experimental evidences have permit us to establish new local molecular domains of the bridge effect in these stilbenoid compounds by means of linear correlations between13C‒NMR chemical shifts of the aromatic carbon centres of the acceptor‒phenyl group and the molecular polarity of the species under study.


1984 ◽  
Vol 57 (4) ◽  
pp. 744-754 ◽  
Author(s):  
E. Morita

Abstract The linear correlation of the pKa to the σ* constants of the substituted phenylthio group indicates the validity of the σ* being equal to the sum of the Hammett's constant of these substituent groups and the σ* of the phenyl group (0.6). The inhibitory activity of the compound LSR depends on the reactivity of BtSSR with BtSH and the general stability of the mixed disulfides which form during the curing process. For BtSSR as accelerators, the Hammett's rule applies to scorch delay time versus σ* constant as the variable with negative slope in the LFER. In benzothiazole-2-sulfenamides, the 13C NMR chemical shift of the carbon at the 2-position of the benzothiazolyl group (C8) is consistently greater than the chemical shift at the carbon adjacent to the amino nitrogen (CN) in the same molecule. It indicates that the electronic distribution at the S-N bond is consistently more positive at the S atom and more negative at the amino nitrogen. The 13C NMR chemical shift at C8 is inversely proportional to the σ* constant of the amino substituents. A wider range of amino substituents is applicable for the correlation analysis with 13C chemical shifts than σ* constants as the variable. When benzothiazole-2-sulfenamides are used as accelerators, two linear relationships with slopes of opposite signs are obtained for the N-substituted phenyl and the N-alkyl sulfenamides, respectively, in the relationship of the scorch delay to the 13C8 chemical shift or the σ* constant. Longer scorch delay was obtained with the pertinent electron-withdrawing phenyl or the sterically hindered alkyl substituents. The more basic amino derivatives give a faster acceleration rate and a higher crosslink efficiency. A significant linear correlation was obtained for scorch delay versus Hammett's σ constant of the phenyl substituents of the N,N′-dithiobisformanilides as vulcanizing agents.


1974 ◽  
Vol 52 (19) ◽  
pp. 3415-3423 ◽  
Author(s):  
William F. Reynolds ◽  
Ian R. Peat ◽  
Gordon K. Hamer

Experimental long-range phenyl proton–vinyl proton coupling constants in 4-substituted styrenes are substituent independent. This is also predicted by INDO–finite perturbation theory calculations of these coupling constants. Comparison with calculated and experimental long-range coupling constants for 4-substituted benzaldehydes suggests that the previously reported substituent dependence for the latter coupling constants arises from substituent-induced changes in molecular geometry.Geminal vinyl coupling constants in 4-substituted styrenes, α-methylstyrenes, and α-t-butylstyrenes are substituent dependent with substituent effects increasing as phenyl and vinyl groups are twisted out of planarity. These trends are reproduced by INDO–FPT calculations. It is concluded that the substituent effects are primarily transmitted through space.Both experimental and calculated vinyl 13C–1H coupling constants show strong stereospecific substituent effects. From the pattern of results (particularly the greater field dependence for JC(β)H(9) than JC β)H(8)) it is concluded that these coupling constants.also reflect through-space substituent effects. This is supported by calculations on model compounds with no intervening phenyl group.


1988 ◽  
Vol 53 (11) ◽  
pp. 2957-2961 ◽  
Author(s):  
Karel Waisser ◽  
Miloš Macháček ◽  
Jean Lebvoua ◽  
Jiří Hrbata ◽  
Jaroslav Dršata

1H NMR chemical shifts of thioamide protons have been determined for a group of thiobenzamides, and the values obtained have been correlated with the Hammett constants. From the relations found the σm and σp values of thioamide group and some other σ constants describing the total effect of two substituents in the phenyl group have been calculated. The relation between the hepatotoxicity for rats (expressed as log ALT) and the Hammett constants is described by equation of parabola.


1973 ◽  
Vol 51 (11) ◽  
pp. 1857-1869 ◽  
Author(s):  
W. F. Reynolds ◽  
I. R. Peat ◽  
M. H. Freedman ◽  
J. R. Lyerla Jr

pH dependent 13C chemical shifts for phenylglycine, phenylalanine, and phenylalanyl derivatives demonstrate that the electronic distribution of the phenyl group depends upon the distance of charged groups from the phenyl ring. The pattern of chemical shifts and the results of CNDO/2 MO calculations indicate that this is due to polarization of the phenyl π electron system. 13C chemical shifts and CNDO/2 calculations for α- and β-substituted phenylalkanes (substituent = NH3+, Cl or Br) provide further evidence for a π polarization effect.


1973 ◽  
Vol 51 (11) ◽  
pp. 1782-1789 ◽  
Author(s):  
Alan J. Jones ◽  
A. F. Casy ◽  
K. M. J. McErlane

The carbon-13 magnetic resonance spectra of the diastereoisomers of 1,2-dimethyl- (1) and 1,3-dimethyl-4-phenylpiperidin-4-ol (2), their esters and corresponding hydrochlorides have been determined. The observed chemical shifts can be ascribed to charge polarization or steric effects. The latter is particularly important in establishing the axial configuration of the 4-phenyl group and 3-methyl group in the preferred conformations of α-1 and β-2, respectively, and consequently the stereochemistry of these systems. Substituent additivity effects are similar to those in the piperidones and cyclohexanes. Solvent effects on 13C resonances remove the ambiguities of conformational change suggested in earlier proton studies.


1983 ◽  
Vol 36 (10) ◽  
pp. 2083 ◽  
Author(s):  
D Christoforou ◽  
DAR Happer

The 13C n.m.r. chemical shifts for the non-substituted rings of azobenzene, stilbene, 26 monosubstituted azobenzenes and 28 monosubstituted stilbenes are reported. The effects of substituents in one ring on the chemical shifts of the other have been interpreted in terms of their inductive and resonance effects by means of a dual substituent parameter analysis. The results show that inductive effects are transmitted to the remote ring from the meta and para positions with equal efficiencies and polarize the phenyl group independently of the rest of the molecule. Resonance interaction is greatest when the substituent is para to the azo or vinylene linking group and is relayed with greatest efficiency to the ortho and para carbons of the remote ring. The results of the study are compared with previously unreported data for the corresponding ring carbons of the ethyl arylazo- and arylethenyl-cinnamates, and with literature data on para-substituted biphenyls and terphenyls.


2005 ◽  
Vol 77 (1) ◽  
pp. 291-311 ◽  
Author(s):  
Parag Acharya ◽  
Jyoti Chattopadhyaya

The generation of a single anionic or cationic center at an alkaline or acidic pH in a given molecule presents a unique opportunity to examine the electrostatic make-up of these molecules both at the neutral or ionic state. The generation of a single cationic center in the phenyl-nicotinamide system provided new straightforward evidence showing that the charge density of the electron-deficient pyridinium was actually enhanced by the donation of the charge from the electron-rich phenyl group (i.e., the pyridinyl became more basic by ca. 0.5 pKa unit compared to an analogous system where phenyl was absent) owing to the electrostatic interactions between these two moieties. On the other hand, the generation of the 5'-guanylate ion in the hexameric single-strand (ss) RNA [5'-GAAAAC-3'], in comparison with the constituent trimeric, tetrameric, and pentameric-ssRNAs, has unequivocally shown how far the electrostatic cross-talk (as an interplay of Coulombic attractive or repulsive forces) in this electronically coupled system propagates through the intervening pAp nucleotide steps until the terminal pC-3' residue in comparison with the neutral counterpart. The footprint of the propagation of this electrostatic cross-talk among the neighboring nucleobases is evident by measurement of pKas from the marker protons of ionization point (i.e., of G) as well as from the neighboring marker protons (i.e., of A or C) in the vicinity, as well as from the change of the chemical environment (i.e., chemical shifts) around their aromatic marker protons (δH2, δH8, δH5, and δH6) owing to a change of the stacking-destacking equilibrium as a function of pH.


1994 ◽  
Vol 72 (8) ◽  
pp. 1780-1784 ◽  
Author(s):  
Ted Schaefer ◽  
Robert W. Schurko ◽  
Guy M. Bernard

The proton chemical shifts and the proton spin–spin coupling constants are reported for 1-phenyl-1-butyne and 1-phenyl-1-pentyne dissolved in CS2/C6D12 and acetone-d6. The long-range coupling constants between the methylene and ring protons are used to derive the twofold barriers to internal rotation in these molecules. They are 0.5 ± 0.1 kJ/mol; the perpendicular conformer is the most stable, the one in which the C(3)—C(4) bond of the side chain lies in a plane perpendicular to the phenyl group. This energetic preference is assigned to the difference between C—C and C—H hyperconjugative interactions with the aromatic π electron system, the C—C interaction being larger. Comparison of the twofold components of the internal rotational barriers in biphenyl and diphenylacetylene, that in the latter amounting to 40% of that in the former, implies that the hyperconjugative component of the internal barrier in ethylbenzene is 1.2 ± 0.3 kJ/mol, a minor component of the total magnitude. Molecular orbital computations of the conformational energies of 1 -phenyl-1-butyne all agree that the perpendicular conformer has the lowest energy but only to the extent of 0.1 kJ/mol at most.


1989 ◽  
Vol 67 (6) ◽  
pp. 1015-1021 ◽  
Author(s):  
Ted Schaefer ◽  
Rudy Sebastian ◽  
James Peeling ◽  
Glenn H. Penner ◽  
Kevin Koh

STO-3G MO computations, with substantial geometry optimization, are reported for benzyl alcohol. They are performed at 15° intervals for the angle by which the C—O bond twists out of the plane of the phenyl group, as well as for 30° intervals for the HCOH dihedral angle. The ensuing conformational energies are used to estimate expectation values of these two angles as well as of functions of these angles. The latter are compared with those obtained from long-range proton–proton coupling constants for dilute solutions in CS2 and acetone-d6. At infinite dilution in CS2 these coupling constants give a distribution for motion about the [Formula: see text] bond that happens to agree with the theoretical results for the free molecule. The latter are used to derive the dihedral angle dependence of 3J(HCOH), the coupling constant between the hydroxyl and methylene protons. This dependence is compared with the observed coupling constants in benzyl alcohol in the gas phase at 422 K and with those measured for the 2,6-difluoro and 2,6-dichloro derivatives of benzyl alcohol. Infinite dilution shifts are reported for the latter two compounds and for α,α-dimethylbenzyl alcohol. The first self-association complex of any significance for benzyl alcohol in CS2 at 300 K is most likely a trimer. Between zero and 2.5 mol% in CS2, all five proton chemical shifts of this molecule are linearly proportional to one another, four of them becoming less shielded at decreasing concentrations. Some nuclear magnetic resonance data are also reported for 3,5-dichlorobenzyl alcohol. Keywords: conformations of benzyl alcohol, 1H NMR of benzyl alcohol, STO-3G MO calculations of benzyl alcohol.


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