Conformational analysis of m4(2)C-m4(2)C-m6(2)A: a chemically modified 3'-acceptor end of tRNA, studied by NMR and CD methods

1H NMR assignments and conformational analysis of the oligoribonucleotides CA, CAU, CAUG, ACAUG, and UCAUG: observation of pyrimidine H5-H1' long-range scalar couplings

Conformational analysis and 1H NMR spectral assignments have been carried out using COSY and RELAY methods for a series of related oligoribonucleotides including two pentamers with 5'-dangling bases. Intraresidue long-range five bond scalar coupling was observed between pyrimidine H5 and H1' protons in the COSY-45 spectra and this feature was useful for both assignment purposes and conformational analysis. The ribose ring conformations were predominantly C3'-endo with the C2'-endo population increasing at the 3'-terminus. The 5'-dangling bases were not stacked efficiently, exhibiting lower % C3'-endo values than their 3'-nearest neighbors. Backbone torsion angle population. beta t, gamma +, epsilon t, were determined using 1H-1H, 1H-31P, and 13C-31P coupling constants. From beta t and gamma + populations the U3-G4 step in CAUG was found to be less efficiently stacked than the C1-A2 and A2-U3 steps. This observation in solution is consistent with the fiber diffraction A-RNA model (S. Arnott, D.W.L. Hukins, S.D. Dover, W. Fuller and A.R. Hodgson, J. Mol. Biol. 81, 107-122, 1973) which also predicts poor stacking in a U-G dinucleotide. The epsilon t populations were greater than 65% for all C3'-O3' bonds and consistent with a right-handed A-RNA helix.

Sequence-dependent emission from stacked forms of ApC and CpA. Evidence for stacked base ('dimer') absorption and left-handed stacked conformation

The corrected and normalised emission spectrum, quantum yield and emission anisotropy are reported for partially stacked adenylyl-3',5'-cytidine (ApC) excited at 266 nm and are compared with cytidylyl-3',5'-adenosine (CpA). Utilizing characteristics determined independently for adenosine and cytidine-5'-monophosphate (CMP), the concurrent self-consistent resolution of emission spectrum and emission anisotropy has been carried out in two ways; first completely empirically as for CpA and second on the basis of a simple stacking model, with concordant results. The total emission spectrum of ApC is resolved into (i) components characteristic of the two monomers and (ii) a red-shifted complex emission. The complex emission spectrum, which is much stronger than from CpA and is complementary to it in bandshape, can also be satisfactorily described by the same components. The dimeric (A, C) system can exist in at least two luminescent stacked forms, proportions of which are determined by the overall stacked fraction and the population within this fraction of the various stacked conformers. The relation between the ratios of the components and the fractional absorption of the stacked forms indicates that the low-energy component is a (hetero-) dimer emission while the high energy component appears to be a true exciplex (hetero-excimer). Comparison with the circular dichroism and NMR literature shows a satisfactory semi-quantitative correlation with the hypothesis that the low energy (hetero-) dimer emission originates from a left-handed stacked conformation Mbb, while the higher energy hetero-excimer originates from the predominant right-handed stacked conformation Pba.

Conformational analysis of the dinucleotides 5'-methylphospho-N6-dimethyladenylyl-uridine (mpm62A-U) and 5'methylphospho-uridylyl-N6-dimethyladenosine (mpU-m62A) and of the trinucleotide U-m62A-U. A nuclear magnetic resonance and circular dichroic study

NMR and CD studies were carried out on the dinucleotides 5'-methylphospho-N6-dimethyladenylyl-uridine (mpm62-U) and 5'-methylphospho-uridylyl-N6-dimethyladenosine (mpU-m62A) and on the trinucleotide U-m62A-U. A detailed comparison is given of the conformational features of mpm62A-U and mpU-m62A with the corresponding 5'-nonphosphorylated dinucleotides m62A-U and U-m62A, respectively. The behaviour of the trinucleotide U-m62A-U is compared with the properties of the constituent dinucleotides U-m62A and mpm62A-U. Chemical-shift and CD data were used to determine the amount of stacking interactions. For each compound NMR spectra were recorded at two or three sample concentrations in order to separate intermolecular and intramolecular base-base interactions. The coupling constants of the ribose ring are interpreted in terms of the N/S equilibrium, and population distributions along the backbone angles beta, gamma and epsilon are presented. The combined data indicate a strong similarity between mpm62A-U and m62A-U both in degree and in mode of stacking. In contrast, the existence of different types of stacking interactions in mpU-m62A and U-m62A is suggested in order to explain the NMR and CD data. It is concluded that dinucleoside bisphosphates serve better as a model for the behaviour of trinucleotides than dinucleoside monophosphates. The trinucleotide U-m62A-U adopts a regular single-stranded stacked RNA structure with preference for N-type ribose and gamma+ and beta t backbone torsion angles. The difference in behaviour between the U-m62A- part of U-m62A-U and the dimer U-m62A is seen as a typical example of conformational transmission.

Conformational analysis of the deoxyribofuranose ring in DNA by means of sums of proton-proton coupling constants: a graphical method

A graphical method is presented for the conformational analysis of the sugar ring in DNA fragments by means of proton-proton couplings. The coupling data required for this analysis consist of sums of couplings, which are referred to as sigma 1' (= J1'2' + J1'2''), sigma 2' (= J1'2' + J2'3' + J2'2''), sigma 2'' (= J1'2'' + J2''3' + J2'2'') and sigma 3' (= J2'3' + J2''3' + J3'4'). These sums of couplings correspond to the distance between the outer peaks of the H1', H2', H2'' and H3' [31P] resonances, respectively, (except for sigma 2' and sigma 2'' in the case of a small chemical shift difference between the H2' and H2'' resonances) and can often be obtained from 1H-NMR spectra via first-order measurement, obviating the necessity of a computer-assisted simulation of the fine structure of these resonances. Two different types of graphs for the interpretation of the coupling data are discussed: the first type of graph serves to probe as to whether or not the sugar ring occurs as a single conformer, and if so to analyze the coupling data in terms of the geometry of this sugar ring. In cases where the sugar ring does not occur as a single conformer, but as a blend of N- and S-type sugar puckers, the second type of graph is used to analyze the coupling data in terms of the geometry and population of the most abundant form. It is shown that the latter type of analysis can be carried out on the basis of experimental values for merely sigma 1',sigma 2' and sigma 2'', without any assumptions or restrictions concerning a relation between the geometry of the N- and S-type conformer. In addition, the question is discussed as to how insight can be gained into the conformational purity of the sugar ring from the observed fine structure of the H1' resonance. Finally, a comparison is made between experimental coupling data reported for single-stranded and duplex DNA fragments and covalent RNA-DNA hybrids on the one hand and the predicted couplings and sums of couplings presented in this paper on the other hand.