Backbone conformation in nucleic acids: an analysis of local helicity through heminucleotide scheme and a proposal for a unified conformational plot

A relationship has been established to express the local helicity of a polynucleotide backbone directly in terms of the virtual bonds spanning the conformationally equivalent heminucleotide repeats, with a view to provide a better understanding of the cumulative effects of all the chemical bond rotational variations on local helicity. Using this, an analysis made with a few oligodeoxynucleotide crystal structures clearly brings forth that it is the concerted movements manifested in the near neighbour correlations between the pair of chemical bonds C4'-C5' and P-O5' and C4'-C3' and P-O3' of the 5' and 3' heminucleotides respectively that are primarily responsible for the observed non-uniform helical twists both in A and B type helical backbones. That these need not be restricted to oligodeoxynucleotides but may be a feature of oligoribonucleotides backbone also is shown from an analysis of helical segments of yeast tRNA(Phe). A proposal of a unified or a grand two dimensional conformational plot which would help visualise succinctly the overall effect of the variations in all the repeating six chemical bonds of a polynucleotide backbone is made. Apart from considerable simplification, the plot affords identification on it regions characteristic of helical, and loop and bend conformations of nucleic acid backbone chain.     

Polynucleotide folding in yeast tRNAPhe: elucidation of short-, medium-, and long-range interactions of sugar-phosphate-sugar backbone and base using a "blocked" nucleotide probe

It has recently been proposed that the repeating backbone nucleotide may be regarded as consisting of two blocks of equal magnitude representable by two virtual bonds. Implicit consideration of the nucleotide (ψ,ψ) and internucleotide (ω′,ω) geometry that generate variety in polynucleotide conformations, and of the constancy of the repeating structural moieties (P-C4′ and C4′-P) independent of the above rotations, has enabled us to utilize this scheme in the study of ordered structures such as di-, oligonucleotides and, most significantly, tRNA. The polynucleotide folding dictated by short-, intermediate-, and long-range interactions in the monoclinic and orthorhombic forms is described and compared through circular plots depicting the virtual bond torsions and distance plots constructed independently for backbone as well as bases. The torsions and the bond angles associated with the virtual bonds afford a clear distinction between ordered helical segments from loops and bends of tRNA. Lower virtual bond torsions (?60° to 60°) concomitant with higher values of virtual bond angles characterize various bend regions, while torsions around 160°–210° typify ordered helical strands. The distance plot elucidates the type of interaction associated with various sub-structures (helix–helix, helix–loop, and loop–loop) that form the constituents of different structural domains. Several other features such as the manifestation of the P₁₀ loop and the approximate twofold symmetry in the tRNA molecule are conspicuous on the distance plot.     

A Renaissance Man: In Memoriam of Jon Widom (1955–2011)

Abstract

Assignment of the ¹H and ³¹P resonances of a decamer DNA duplex, d(CGCTTAAGCG)₂ was determined by two-dimensional COSY, NOESY and ¹H- ³¹P Pure Absorption phase Constant time (PAC) heteronuclear correlation spectroscopy. The solution structure of the decamer was calculated by an iterative hybrid relaxation matrix method combined with NOESY-distance restrained molecular dynamics. The distances from the 2D NOESY spectra were calculated from the relaxation rate matrix which were evaluated from a hybrid NOESY volume matrix comprising elements from the experiment and those calculated from an initial structure. The hybrid matrix-derived distances were then used in a restrained molecular dynamics procedure to obtain a new structure that better approximates the NOESY spectra. The resulting partially refined structure was then used to calculate an improved theoretical NOESY volume matrix which is once again merged with the experimental matrix until refinement is complete. J_H3′-P coupling constants for each of the phosphates of the decamer were obtained from ¹H-³¹P J-resolved selective proton flip 2D spectra. By using a modified Karplus relationship the C4′-C3′-03′-P torsional angles (?) were obtained. Comparison of the ³¹P chemical shifts and J_H3′-P coupling constants of this sequence has allowed a greater insight into the various factors responsible for ³¹P chemical shift variations in oligonucleotides. It also provides an important probe of the sequence-dependent structural variation of the deoxyribose phosphate backbone of DNA in solution. These correlations are consistent with the hypothesis that changes in local helical structure perturb the deoxyribose phosphate backbone. The variation of the ³¹P chemical shift, and the degree of this variation from one base step to the next is proposed as a potential probe of local helical conformation within the DNA double helix. The pattern of calculated ? and ζ torsional angles from the restrained molecular dynamics refinement agrees quite well with the measured J_H3′-P coupling constants. Thus, the local helical parameters determine the length of the phosphodiester backbone which in turn constrains the phosphate in various allowed conformations.     

Mechanisms of chain folding in nucleic acids. The (omega, omega) plot and its correlation to the nucleotide geometry in yeast tRNAPhe1.

The (omega', omega) polot depicting the internucleotide P-O bond rotation angles in yeast phenylalanyl transfer RNA has established the interdependence of the phosphodiesters and the nucleotide geometries in the folding of the polynucleotide backbone. The plot distinguishes the regions characteristic of secondary helical structures and tertiary structural loops and bends. The folding of the polynucleotide chain is accomplished either solely by rotations around the P-O bonds or in concert with rotations around the nucleotide C4'-C5' bond with or without changes in the sugar ring pucker. In spite of differences in nucleotide sequence and intraloop tertiary interactions in the anticodon and pseudouridine loops, a characteristic repeating structural unit is found for the sugar-phosphate backbone of the tetranucleotide segment around the sharp turns.     

Conformational features of 2′-O-methyl-adenosylyl-adenosine

In order to obtain information about the conformational features of a 2′-O-methylated polyribonucleotide at the nearest neighbor level, a detailed nuclear magnetic resonance study of AmpA was undertaken. AmpA was isolated from alkali hydrolysates of yeast RNA, and proton spectra were recorded at 100 MHz in the Fourier transform mode in D₂O solutions, 0.01 M, pH 5.4 and 1.5 at 25°C. ³¹P spectra were recorded at 40.48 MHz. Complete, accurate sets of nmr parameters derived for each nucleotidyl unit by simulation iteration methods. The nmr data were translated into conformational parameters for all the bonds using procedures developed in earlier studies from these laboratories. It is shown that AmpA exists in aqueous solution with a flexible molecular framework, which shows preferences for certain orientations. The ribose rings exist as a ²E ? ³E equilibrium with the —pA ribose showing a bias for the ³E pucker. The C(4′)—C(5′) bonds of both nucleotidyl units show significant preference (75–80%) to exist in gg conformation. The dominant conformer (80%) about C(5′)—O(5′) of the 5′-nucleotidyl unit is g′g′. Even though an unambiguous determination of the orientation of the 3′-phosphate group cannot be made, tentative evidence shows that it preferentially occupies g⁺ domains [O(3′)—P trans to C(3′)—C(2′)] in which the H(3′) —C(3′)—O(3′)—P(3′) dihedral angle is about 31°. There is reasonable evidence that the 2′-O-methyl preferentially occupies the domain in which the O(2′)—CH₃ bond is trans to C(2′)—C(1′). Lowering of pH to 1.5, which results in protonation of both the adenine moieties, causes destacking of AmpA. Such destacking is accompanied by small, but real, perturbations in the conformations about most of the bonds in the backbone. A detailed comparison of the solution conformations of ApA and AmpA clearly shows that 2′-O-methylation strongly influences the conformational preference about the C(3′)—O(3′) bond of the 3′-nucleotidyl unit, in addition to inducing small changes in the overall ribophosphate backbone conformational equilibria. The effect of 2′-O-methylation is such that the C(3′)—O(3′) is forced to occupy preferentially the g⁺ domain rather than the normally preferred g^? domain [O(3′)—P trans to C(3′)—C(4′)] in ApA. The data on ApA and AmpA further reveal that the extent of stacking interaction is less in AmpA compared to ApA. It is suggested that stacked species of AmpA exist as right-handed stacks where the magnitude of ω and ω′ about O(5′)—P and P—O(3′) is about 290°. The reason for the lesser degree of stacking in AmpA compared to ApA is intramolecular interaction between 2′-O-methyl and the flexible O(3′)—P—O(5′) bridge, the interaction causing some perturbation in the magnitudes of ω/ω′, causing destacking. The destacking will lead to an increase in _χCN by a few degrees, causing an increase in ²E populations; the latter in turn will shift the 3′ phosphate group from g^? to g⁺ domains. In short, a coupled series of conformational events is envisioned at the onset of destacking, made feasible by the interaction between the 2′-O-methyl group and the swivel O(3′)—P—O(5′) bridge.     

The occurrence of the syn-C3′ endo conformation and the distorted backbone conformations for C4′-C5′ and P-O5′ in oligo and polynucleotides

Abstract

The nucleoside constituents of nucleic acids prefer the anti conformation (1). When the sugar pucker is taken into account the nucleosides prefer the C2′endo-anti conformation. Of the nearly 300 nucleosides known, about 250 are in the anti conformation and 50 are in the syn-conformation, i.e., anti to syn conformation is 5:1. The nucleotide building blocks of nucleic acids show the same trend as nucleosides. Both the deoxy-guanosine and ribo- guanosine residues in nucleosides and nucleotides prefer the syn-C2′endo conformation with an intra-molecular hydrogen bond (for nucleosides) between the O5′- H and the N3 of the base and, a few syn-C3′endo conformations are also observed. Evidence is presented for the occurrence of the C3′endo-syn conformation for guanines in mis-paired double helical right-handed structures with the distorted sugar phosphate C4′-C5′ and P-O5′ bonds respectively, from g+ (gg) and g- to trans. Evidence is also provided for guanosine nucleotides in left-handed double-helical (Z-DNA) oligo and polynucleotides which has the same syn-C3′endo conformation and the distorted backbone sugar-phosphate bonds (C4′-C5′ and P- O5′) as in the earlier right-handed case.     

Intramolecular steric effects and hydrogen bonding in regular conformations of polyamino acids

A survey has been made, by using computer methods, of the types of helices which polypeptide chains can form, taking into account steric requirements and intramolecular hydrogen-bonding interactions. The influence on these two requirements, of small variations in the bond angles of the peptide residues, or of small changes in the overall dimensions of the helix (pitch and residues per turn), have been assessed for the special case of the α-helix. Criteria for the formation of acceptable hydrogen bonds have also been applied to helices of other types, viz., the 3, γ^?, ω^?, and π-helices. It was shown that the N? H … O and H … O? C angles in hydrogen bonds are sensitive to changes in either the NC^αC′ bond angle or in the rotational angles about the N? C^α and C^α? C′ bonds. However, the variants of the α-helix observed experimentally in myoglobin can all be constructed without distortion of the hydrogen bonds. For α-helices, the steric and hydrogen bonding requirements are more easily fulfilled with an NC^αC′ bond angle of 111°, rather than 109.5°. The decreased stability observed for the left-handed α-helix relative to the right-handed one for L -amino acids is due essentially only to interactions of the C^β atom of the side chains with atoms in adjacent peptide units in the backbone, and interactions with atoms in adjacent turns of the helical backbone are not significantly different in the two helices. Restrictions in the freedom of rotation of bulky side chains may have significant kinetic effects during the formation of the α-helix from the “random coil” state.     

Index to Subjects,Vol. 27

Abstract

A constrained model building procedure is used to generate nucleic acid structures of the familiar A-, B-, and Z-DNA duplexes. Attention is focused upon the multiple structural solutions associated with the arrangements of nucleic acid base pairs rather than the optimum sugar-phosphate structure. The glycosyl (χ) and sugar torsions (both the ring puckering and the exocyclic C5′-C4′ (ψ) torsion) are treated as independent variables and the resulting O3′…O5′ distances are used as closure determinants. When such distances conform to the known geometry of phosphate chemical bonding, an intervening phosphorus atom with correct C-O-P valence angles can be located. Four sequential torsion angles- φ,ω,ω,ω and φ about the C3′-O3′-P-O5′-C5′ bonds are then obtained as dependent variables. The resulting structures are categorized in terms of conformation, ranked in potential energy, and analyzed for torsional correlations. The numerical results are quite interesting with implications regarding nucleic acid models constructed to fit less than ideal experimental data. The multiple solutions to the problem are useful for comprehending the conformational complexities of thelocal sugar-phosphate backbone and for understanding the transitions between different helical forms. According to these studies, unique characterization of a nucleic acid duplex involves more than the determination of its base pair morphology, its sugar puckering preferences, or its groove binding features.     

Conformation and Configuration at the Central Amine Nitrogen of a Nucleotide Adduct of the Carcinogen 2-(Acetylamino)flourene as Studied by 13C and 15N NMR Spectroscopy

Abstract

The conformation and configuration at the central nitrogen of the adduct 8-(N-fluoren-2-ylamino)-2′-deoxyguanosine 5′-monophosphate has been investigated by high-field ¹³C and ¹⁵N NMR spectroscopy. One-bond nitrogen-hydrogen coupling constants and ¹³C chemical shifts for the adduct as well as for the model compounds diphenylamine, 4-nitrodiphenylamine and 2-aminofluorene have been measured in nonaqueous solutions. The data indicate a near planar configuration at the amine nitrogen that links the guanine and fluorene rings of the adduct. The orientations about the guanyl-nitrogen and fluorenyl-nitrogen bonds place the two ring systems in either perpendicular (Type A) or helical (Type B) conformations. It is suggested, based on structural similarities to diarylamines, that the C-N-C bond angle of the adduct is greater than 120° in order to reduce unfavorable steric interactions between the two ring systems. Space-filling molecular models of the adduct in duplex DNA show that the aminofluorene moiety can be oriented into both Type A and Type B conformations within the major groove. The configuration at nitrogen of diphenylamine, 4-nitrodiphenylamine and 2-aminofluorene has also been examined.     

Random coil conformations of polynucleotides: a study incorporating long-range correlations due to dynamics of the sugar residue

A novel virtual bond scheme joining the atoms P-C4′ and C4′-P of a nucleotide repeat, consistent with the stereochemistry of polynucleotide chains, has been developed. The scheme, with its inherent feature to account for all the major sources of flexibility, could also consider effectively the short range and long range interactions, thereby simplifying the analysis of random coil and ordered structures. Using this scheme, unperturbed end-to-end dimensions and persistence lengths of polynucleotide chains have been computed incorporating the dynamical aspects of the sugar ring as well as the C4′ C5′ bond and the correlated changes in phosphodiester conformations. Calculated unperturbed dimensions are in excellent agreement with experimental values. Results show that the random coil is characterized by a large proportion of helical segments of the A-form.     

Major groove width variations in RNA structures determined by NMR and impact of <Superscript>13</Superscript>C residual chemical shift anisotropy and <Superscript>1</Superscript>H–<Superscript>13</Superscript>C residual dipolar coupling on refinement

Ribonucleic acid structure determination by NMR spectroscopy relies primarily on local structural restraints provided by ¹H– ¹H NOEs and J-couplings. When employed loosely, these restraints are broadly compatible with A- and B-like helical geometries and give rise to calculated structures that are highly sensitive to the force fields employed during refinement. A survey of recently reported NMR structures reveals significant variations in helical parameters, particularly the major groove width. Although helical parameters observed in high-resolution X-ray crystal structures of isolated A-form RNA helices are sensitive to crystal packing effects, variations among the published X-ray structures are significantly smaller than those observed in NMR structures. Here we show that restraints derived from aromatic ¹H– ¹³C residual dipolar couplings (RDCs) and residual chemical shift anisotropies (RCSAs) can overcome NMR restraint and force field deficiencies and afford structures with helical properties similar to those observed in high-resolution X-ray structures.     

Crystallographic studies of drug-nucleic acid interactions: Proflavine intercalation between the non-complementary base-pairs of cytidilyl-3′,5′-adenosine

In order to get insights into the binding of dyes and mutagens with denatured and single-stranded nucleic acids and the possible implications in frameshift mutagenesis, a 1:1 complex between the non-self-complementary dinucleoside monophosphate cytidilyl-3′,5′-adenosine (CpA) and proflavine was crystallized. The crystals belong to the tetragonal space group P4₂2₁2 with cell constants $\text{a = b = 19.38(1)}\text{A}\text{?}\text{and}\text{c = 27.10(1)}\text{A}\text{?}$. The asymmetric unit contains one CpA, one proflavine and nine water molecules by weight. The structure was determined using Patterson and direct methods and refined to an R-value of 11% using 2454 diffractometer intensities.The non-self-complementary dinucleoside monophosphate CpA forms a selfpaired parallel chain dimer with a proflavine molecule intercalated between the protonated cytosine-cytosine (C · C) pair and the neutral adenine-adenine (A · A) pair. The dimer complex exhibits a right-handed helical twist and an irregular girth. The neutral A · A pair is doubly hydrogen-bonded through the N(6) and N(7) sites (C(1′)C(1′) distance: 10.97(2) Å) and the protonated C · C pair is triply hydrogen-bonded with a proton shared between the N(3) sites (C(1′)C(1′) distance: 9.59(2) Å). To accommodate the intercalating dye, the sugars of successive nucleotide residues adopt the two fundamental conformations (5′ end: 3′-endo, 3′ end: 2′-endo), the backbone adopts torsion angle values that fluctuate within their preferred conformational domains: the PO bonds (ω, ω′) adopt the characteristic helical (gauche^?-gauche^?) conformation, the CO bonds (φ, φ′) are both in the trans domain and the C(4′)C(5′) bonds (ψ) are in the gauche⁺ region. The bases of both residues are disposed in the preferred anti domain with the glycosyl torsion angles (χ) correlated to the puckering mode of the sugar so that the cytidine residue is C(3′)-endo, low χ (12 dg), and the adenosine residue is C(2′)-endo, high χ (84 °). The intercalated proflavine stacks more extensively with the C · C pair than the A · A pair. Between 4₂-related CpA proflavine units there is a second proflavine which stacks well with both the A · A and the C · C pairs sandwiching it. Both proflavine molecules are positionally disordered. In each of its two disordered sites, the intercalated proflavine forms hydrogen-bonded interactions with only one sugar-phosphate backbone. A total of 26 water sites has been characterized of which only two are fully occupied. These hydration sites are involved in an intricate network of hydrogen bonds with both the dye and CpA and provide insights on the various modes of interactions between water molecules and between water molecules and nucleic acids.The structure of the proflavine-CpA complex shows that intercalation of planar drugs can occur between non-complementary base-pairs. This result can be relevant for understanding the strong binding of acridine dyes to denatured DNA, single-stranded RNA, and single-stranded polynucleotides. Also, the ability of proflayine to promote self-pairs of adenine and cytosine bases could provide a chemical basis for an alternative mechanism of frameshift mutagenesis.     

Conformational dependence of the Raman scattering intensities from polynucleotides. 3. Order-disorder changes in helical structures

Raman spectra are presented on ordered and presumably helical structures of DNA and RNA as well as the poly A·poly U helical complex, polydAT, and the helical aggregates of 5′-GMP and 3′-GMP. The changes in the frequency and the intensity of the Raman bands as these structures undergo order-disorder transitions have been measured. In general the changes we have found can be placed into three categories: (1) A reduction in the intensities of certain ring vibrations of the polynucleotide bases is observed when stacking or ordering occurs (Raman hypochromism). Since the ring vibrational frequencies are different for each type of base, we have been able to obtain some estimate of average amount of order of each type of base in partially ordered helical systems. (2) A very large increase in the intensity of a sharp, strongly polarized band at about 815 cm^?1 is observed when polyriboA and polyriboU are formed into a helical complex. Although this band is not present in the separated chains at high temperature, a broad diffuse band at about 800 cm^?1 is present. The 815 cm^?1 band undoubtedly arises from the vibrations of the phosphate-sugar portions of the molecule and provides a sensitive handle to the back-bone conformation of the polymer. This band also appears upon ordering of RNA, formation of the helical aggregate of 5′-riboGMP, and to some extent in the selfstacking of the polyribonucleotides polyA, polyU in the presence of Mg⁺⁺, PolyC, and polyG. No such intense, polarized band is found, however, in ordered DNA, polydAT, or the 3′-riboGMP aggregate, although there is a conformationally independent band at about 795 cm^?1 in DNA and polydAT. (3) Numerous frequency changes occur during Conformational changes. In particular the 1600–1700 cm^?1 region in D₂O shows significant conformationally dependent changes in the C?O stretching region analogous to the changes in this region which have been observed in these substances in the infrared. Thus, Raman scattering appears to provide a technique for simultaneously observing the effects of base stacking, backbone conformation and carbonyl hydrogen bonding in nucleic acids in moderately dilute (10–25 mg/ml) aqueous solutions.     

Ab-inito Quantum Mechanical Calculations of NMR Chemical Shifts in Nucleic Acids Constituents II Conformational Dependence of the lH and 13C Chemical Shifts in the Ribose

Abstract

The magnetic shielding constant of the different ¹³C and ¹³H nuclei of a deoxyribose are calculated for the C2′ endo and C3′ endo puckerings of the furanose ring as a function of the conformation about the C4′C5′ bond. For the carbons the calculated variations are of several ppm, the C3′ endo puckering corresponding in most cases to a larger shielding than the C2′ endo one. For the protons the calculated variations of chemical shifts are all smaller than 1.3 ppm, that is of the order of magnitude of the variation of the geometrical shielding produced on these protons by the other units of a DNA double helix, with a change of the overall structure of the helix. The computations carried out on the deoxyribose ?3′ and 5′ phosphates for several conformations of the phosphate group tend to show that the changes of conformation of the charged group of atoms produce chemical shift variations smaller than the two conformational parameters of the deoxyribose itself. The calculations carried out for a ribose do give the general features of the differences between the carbon and proton spectra of deoxynucleosides and nucleosides.

The comparison of the measured and calculated phosphorylation shifts tend to show that the counterion contributes significantly, for some nuclei of the deoxyribose, to the shifts measured. The calculated magnitude of this polarization effect on carbon shifts suggests a tentative qualitative interpretation of carbon spectra of the ribose part of DNA double helices.     

On the conformational dependence of the proton chemical shifts in nucleosides and nucleotides III. Proton chemical shifts of 5′-nucleotides as a function of different conformational parameters

The variation of the chemical shift of the protons of 5′-UMP and 5′-AMP is calculated as a function of χ_CN, ψ and ? torsion angles. The shift of H8 of 5′-AMP and H6 of 5′-UMP is found to be very sensitive to the value of χ_CN. For the anti conformations the shift of these protons is more sensitive to the value of the rotation about CS′-05′ than about C4′-CS′. For the protons of the ribose the calculations show that for the C2′-endo pucker H3′ and H2′ undergo the largest chemical shift variations when ? and ψ vary. The calculated variations are considered in relation with the role of the conformation of the nucleotides in the chemical shift variation between mono and polynucleotides and between the different helical structures of polynucleotides.     

Secondary and tertiary structural foldings in tRNA. A diagonal plot analysis using the blocked nucleotide scheme.

A distance plot obtained using the blocked nucleotide concept, which regards the repeating nucleotide moieties to be made up of two blocks of nearly equal magnitude, has permitted us to visualize the polynucleotide backbone folding in yeast tRNAPhe. The plot clearly manifests medium- and long-range tertiary interactions involving various structural domains. Apart from the well known T psi-D loop interactions, other long-range interactions associated with the variable loop as well as the D loop are explicitly seen. Most importantly, the plot reveals an approximate two-fold symmetry in the molecule between the domains related to the tertiary interactions in addition to the symmetry between long helical domains. The different patterns on the plot are interpreted in terms of helix-helix, loop-helix and loop-loop interactions.     

Crystal Structure of 1-(2′,3′,5′-Tri -O-Acetyl-β-D-ribofuranosyl)-3-acetoxy-2-pyridone: An Antitumour Agent

Abstract

1–C3′, 3′, 5′–Tri—O—acetyl— β—D—ribof uranosyll)—3—acetoxy —2—pyridone,crystallised in space group P2 with z=2 and cell parameters a=12. 446(2), b=10. 415(2), c=7. 600(2) A, β=03. 3O(4). The structure was solved by direct methods and refined by full—matrix least—squares to a final R value of 0·251 for 1847 observed reflections. The sugar—pucker is found to be ³ECC3′ endo) with P = 17.7° and x_CN=170. 2(2)° in the range. The C4′-C5′ conformation is gauche minus. Because of the absence of H—bond donor atoms. the crystal structure is stabilised by a network of C-H—-O close contacts. No base stacking is observed.     

Conformational Analysis of a Hybrid DNA-RNA Double Helical Oligonucleotide in Aqueous Solution: d(CG)r(CG)d(CG) Studied by 1D- and 2D-1H NMR Spectroscopy

Abstract

The double helical structure of the self-complementary DNA-RNA-DNA hybrid d(CG)r(CG) d(CG) was studied in solution by 500 MHz ¹H-NMR spectroscopy. The non-exchangeable base protons and the (deoxy)ribose H1′, H2′ and H2″ protons were unambiguously assigned using 2D-J-correlated (COSY) and 2D-NOE (NOESY) spectroscopy techniques. A general strategy for the sequential assignment of ¹H-NMR spectra of (double) helical DNA and RNA fragments by means of 2D-NMR methods is presented.

Conformational analysis of the sugar rings of d(CG)r(CG)d(CG) at 300 K shows that the central ribonucleotide part of the helix adopts an A-type double helical conformation. The 5′- and 3′-terminal deoxyribose base pairs, however, take up the normal DNA-type conformation. The A-to-B transition in this molecule involves only one (deoxyribose) base pair. It is shown that this A-to-B conformational transition can only be accomodated by two specific sugar pucker combinations for the junction base pair, i.e. N·S (C3′-endo-C2′-endo, 60%, where the pucker given first is that assigned to the junction nucleotide residue of the strand running 5′ → 3′ from A-RNA to B-DNA) and S·S (C2′-endo-C2′-endo, 40%).     

The Structure of Triple Helical Poly(U)·Poly(A)·Poly(U) Studied by Raman Spectroscopy

Abstract

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U)·poly(A) ·poly(U) triple helix. We compared the Raman spectra of poly(U)·poly(A)·poly(U) in H₂O and D₂O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A)·poly(U). The presence of a Raman band at 863 cm^?1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3′ endo; that of the second poly(U) chain may be C2′ endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A)·poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.