internal rotational barriers
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Heliyon ◽  
2020 ◽  
Vol 6 (9) ◽  
pp. e04957
Author(s):  
Daniel Rodrigues Lima ◽  
Sílvio Quintino de Aguiar Filho ◽  
Laura Beatriz Camargo do Oh ◽  
Anna Karla dos Santos Pereira ◽  
Douglas Henrique Pereira

2019 ◽  
Vol 1166 ◽  
pp. 112589
Author(s):  
Sílvio Quintino de Aguiar Filho ◽  
Adão Marcos Ferreira Costa ◽  
Igor Hernandes Santos Ribeiro ◽  
Rogério Custodio ◽  
Douglas Henrique Pereira

2019 ◽  
Vol 19 (4) ◽  
pp. 1055
Author(s):  
Ali Hussain Yateem

The barrier to internal rotation around the central C2–C3 single bond of a series of (1E)-monosubstituted 1,3-butadienes and (1E,3E)-1-Y-4-X-disubstituted butadienes, with Y=NH2 or OCH3 and X=NO2, CHO, COOH, CN, CF3, Cl or F, were studied at the density functional w B97X-D/6-31G∗∗ level. The effect of substituents on π-conjugation in disubstituted 1,3-butadienes was studied by correlating the calculated internal rotational barriers with the difference in structural, atomic and molecular properties between the transition state TS and the s-trans conformers. The calculated differences in lengths of C–C, C–NH2 and C–OCH3 single bonds, N-H-N, and C-O-CH3 angles, NH2 out-of-plane angle, natural charges on amino nitrogen and methoxy oxygen, and the maximum electrostatic potential on amino hydrogens, were found to correlate strongly with the rotational barriers. The conjugative interaction was strongly stabilized in the case of strong π-electron acceptors such as NO2 or CHO and is slightly or negligibly affected with Cl and F groups. The resonance stabilization with the remaining acceptors decreases in the order COOH > CN > CF3. Acceptors X maintain their relative order of stabilization for the two donors, and NH2 is more stabilizing. Dominant resonance structures are suggested for highly and negligibly conjugated systems.


2002 ◽  
Vol 2002 (8) ◽  
pp. 403-406
Author(s):  
Majid Monajjemi ◽  
Halleh H. Haeri ◽  
Malihe T. Azad

The internal rotational barriers for formamide are calculated in gas and solution phases (acetonitrile) at the HF/6-31G* (16.64 and 16.18 kcal/mol, respectively) and MP2/6-31G* (16.86 and 16.71 kcal/ mol, respectively) level of theory. Calculated parameters are compared with experimental data and there is a good agreement between them. Orbital populations are obtained by MPA (mulliken population analysis) and NPA (natural population analysis) methods and bond energies are calculated by the NBO method (natural bond orbitals). The distribution of atomic charges are also given. These calculation indicate that the internal rotational barrier is produced because of change in the distribution of orbital populations of 2p y, 2p z, d yz, d y2 and dz2 orbitals of the nitrogen atom.


2002 ◽  
Vol 35 (10) ◽  
pp. 4198-4203 ◽  
Author(s):  
S. Krushev ◽  
W. Paul ◽  
G. D. Smith

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