AB-INITIO MOLECULAR-ORBITAL STUDY OF THE AMIDE-I VIBRATIONAL INTERACTIONS BETWEEN THE PEPTIDE GROUPS IN DIPEPTIDE AND TRIPEPTIDE AND CONSIDERATIONS ON THE CONFORMATION OF THE EXTENDED HELIX
H. Torii et M. Tasumi, AB-INITIO MOLECULAR-ORBITAL STUDY OF THE AMIDE-I VIBRATIONAL INTERACTIONS BETWEEN THE PEPTIDE GROUPS IN DIPEPTIDE AND TRIPEPTIDE AND CONSIDERATIONS ON THE CONFORMATION OF THE EXTENDED HELIX, Journal of Raman spectroscopy, 29(1), 1998, pp. 81-86
Interrelationships among the coupling between the amide I vibrations o
f peptide groups, the A-E-1 wavenumber difference of the amide I mode
and the conformation of helical polypeptide chains were examined theor
etically. Ab initio molecular orbital (MO) calculations were performed
for a glycine dipeptide and a glycine tripeptide with various phi and
psi angles to obtain the coupling constants between the amide I vibra
tions of the nearest peptide groups and between those of the second ne
arest peptide groups. It was found that the coupling constants between
the second nearest peptide groups were reasonably well. explained by
the transition dipole coupling mechanism, whereas the coupling constan
ts between the nearest peptide groups contained other factors that mai
nly depended on psi. The wavenumbers of the A and E-1 components of th
e amide I mode were calculated for various helices on the basis of the
se coupling constants. The A component is strong in the infrared (IR)
spectrum when the transition dipole of the amide I vibration is nearly
parallel to the helix axis, whereas the E-1 component has a strong IR
intensity when they are nearly perpendicular to each other. The A com
ponent has a strong Raman intensity in both cases. Therefore, the Rama
n-infrared wavenumber difference of 10-20 cm(-1) observed for the amid
e I bands of poly(L-glutamate) and poly(L-lysine) with charged side ch
ains indicates that these polypeptides, in that so-called 'extended he
lix' state, have conformations giving rise to strong IR bands of the E
-1 component which are lower in wavenumber than the Raman bands of the
A component by 10-20 cm(-1). The ranges of the phi and psi angles tha
t are consistent with such spectral features are discussed on the basi
s of the calculated structures and amide I wavenumbers. (C) 1998 John
Wiley & Sons, Ltd.