B. Pispisa et al., Structural features of linear, homo-Aib-based peptides in solution: a spectroscopic and molecular mechanics investigation, J PEPT RES, 56(5), 2000, pp. 298-306
In continuation of our studies on the determination of the structural featu
res of functionalized peptides in solution by combining time-resolved fluor
escence data and molecular mechanics results, the conformational properties
of a series of linear, homo-Aib peptides in methanol (a structure-supporti
ng solvent) were investigated. These compounds have the general formula P(A
ib)(n)N, where Aib is alpha -aminoisobutyric acid, N is naphthalene and P i
s the monomethylated protoporphyrin IX, the two latter chromophores being c
ovalently attached to the peptide C- and N-termini, respectively, while n-3
, 6 and 9. According to H-1 NMR and IR spectra, the peptides investigated l
argely populate a 3(10)-helical structure in CDCl3, which is also a structu
re-supporting solvent. Both steady-state and time-resolved fluorescence mea
surements show a strong quenching of the N emission that parallels an incre
ase of the P fluorescence intensity, suggesting the occurrence of long-rang
e energy transfer from N-1* to ground-state P. Comparison of quenching effi
ciencies and lifetime pre-exponents with those obtained theoretically from
the deepest energy minimum conformers is very satisfactory. The computed st
ructures, built up by partially taking into account the solvent medium, exh
ibit a rigid, highly compact arrangement, owing to both the 3(10)-helix con
formation of the backbone chain and the very few peptide-to-chromophore cov
alent linkages. As a result, only one or two stable conformations for each
peptide were theoretically found, in full agreement with the time-resolved
fluorescence data. Orientational effects between the probes must be taken i
nto account for a correct interpretation of the fluorescence decay results,
which implies that interconversion among conformational substates of the N
linkages is slower than 10 ns, corresponding to the upper limit of the ene
rgy transfer characteristic time.