RNA double helices generated from crystal structures of double helical dinucleoside phosphates.

The dinucleoside phosphates ApU and GpC form right-handed anti-parallel double helical fragments within their crystal lattices. Using a least squares procedure, we have generated the extended double helices which these fragments represent. ApU corresponds to a double helix with 11.9 residues per turn and a pitch of 28. 1Å. The GpC double helix has 10.4 residues per turn and a pitch of 26. 9Å.     

Polymorphism of DNA double helices

Native DNA duplexes in fibers exist usually in one of three well-known (A, B and C) forms depending on relative humidity, type of cations and the amount of retained salt. To determine the precise influence of these factors and the effect of base composition, as well as base sequence, on DNA secondary structure, X-ray diffraction methods have been used to study all four synthetic DNA duplexes with repeated dinucleotide sequences, eight of the 12 with repeated trinucleotide sequences and seven analogues in which guanine was replaced with hypoxanthine. The results indicate that there are at least six additional allomorphs denoted by B′, C′, C″, D, E and S.The B′ form (h = 0.329 nm) observed for poly(dA) · poly(dT), poly(dI) · poly(dC) and poly[d(A-I)] · poly[d(C-T)] is a minor variant of the traditional B form (h = 0.338 nm) of native DNA. The two C-like forms C′ for poly[d(A-G-C)] · poly-[d(G-C-T)] and poly[d(G-G-T)] · poly[d(A-C-C)] and C″ for poly[d(A-G)] · poly-[d(C-T)] have, respectively, 9₁ and 9₂ symmetries which reflect repetition of trinucleotide and dinucleotide sequences, respectively. Although isocompositional with poly(dA) · poly(dT), the existence of the rather different D form (8₁) for poly[d(A-T)] · poly[d(A-T)] or for poly[d(A-A-T)] · poly[d(A-T-T)] is a clear demonstration of the sequence effect. The I · C pair generally mimics an A · T pair, but poly[d(I-I-T)] · poly[d(A-C-C)] provides a new (E) form with approximately 15₂ screw symmetry and with 〈h〉 = 0.325 nm and 〈t〉 = 48 dg per nucleotide. The S form (6₅) observed for poly[d(G-C)] · poly[d(G-C)] and poly[d(A-C)] · poly[d(G-T)] is an unusual left-handed polydinucleotide helix and is accessible to any alternating purine-pyrimidine sequence. In it the two nucleotides have quite different conformations and involve syn purine and anti pyrimidine nucleosides.     

Recognition of nucleic acid double helices by homopyrimidine 2', 5'-linked RNA.

We have studied the effect of a 2',5'-RNA third strand backbone on the stability of triple helices with a 'pyrimidine motif' targeting the polypurine strand of duplex DNA, duplex RNA and DNA/RNA hybrids. Comparative experiments were run in parallel with DNA and the regioisomeric RNA as third strands adopting the experimental design of Roberts and Crothers. The results reveal that 2',5'-RNA is indeed able to recognize double helical DNA (DD) and DNA (purine):RNA (pyrimidine) hybrids (DR). However, when the duplex purine strand is RNA and the duplex pyrimidine strand is DNA or RNA (i.e. RD or RR), triplex formation is not observed. These results exactly parallel what is observed for DNA third strands. Based on T m data, the affinities of 2',5'-RNA and DNA third strands towards DD and DR duplexes were similar. The RNA third strand formed triplexes with all four hairpins, as previously demonstrated. In analogy to the arabinose and 2'-deoxyribose third strands, the possible C2'- endo pucker of 2',5'-linked riboses together with the lack of an alpha-2'-OH group are believed to be responsible for the selective binding of 2',5'-RNA to DD and DR duplexes, over RR and RD duplexes. These studies indicate that the use of other oligonucleotide analogues will prove extremely useful in dissecting the contributions of backbone and/or sugar puckering to the recognition of nucleic acid duplexes.     

Dynamics of the B-A transition of DNA double helices

Although the transition from the B-DNA double helix to the A-form is essential for biological function, as shown by the existence of the A-form in many protein–DNA complexes, the dynamics of this transition has not been resolved yet. According to molecular dynamics simulations the transition is expected in the time range of a few nanoseconds. The B–A transition induced by mixing of DNA samples with ethanol in stopped flow experiments is complete within the deadtime, showing that the reaction is faster than ~0.2 ms. The reaction was resolved by an electric field jump technique with induction of the transition by a dipole stretching force driving the A- to the B-form. Poly[d(A-T)] was established as a favourable model system, because of a particularly high cooperativity of the transition and because of a spectral signature allowing separation of potential side reactions. The time constants observed in the case of poly[d(A-T)] with ~1600 bp are in the range around 10 µs. An additional process with time constants of ~100 µs is probably due to nucleation. The same time constants (within experimental accuracy ±10%) were observed for a poly[d(A-T)] sample with ~70 bp. Under low salt conditions commonly used for studies of the B–A transition, the time constants are almost independent of the ionic strength. The experimental data show that a significant activation barrier exists in the B–A transition and that the helical states are clearly separated from each other, in contrast to predictions by molecular dynamics simulations.     

A guanine-linked end-effect is a sensitive reporter of charge flow through DNA and RNA double helices

The property of charge (electron hole) flow in DNA duplexes has been the subject of intensive study. RNA-DNA heteroduplexes have also been investigated; however, little information exists on the conductive properties of purely RNA duplexes. In investigating the relative conductive properties of a three molecule DNA-DNA duplex design, using piperidine and aniline to break strands at modified bases, we observed that duplexes with guanine-rich termini generated a large oxidative end-effect, which could serve as a highly sensitive reporter of charge flow through the duplexes. The end-effect was found faithfully to report attenuations in charge flow due to certain single-base mismatches within a duplex. Comparative charge flow experiments on DNA-DNA and RNA-RNA duplexes found large end-effects from both, suggesting that the A and B family of double helices conduct charge comparably. The sheer magnitude of the end-effect, and its high sensitivity to helical imperfections, suggest that it may be exploited as a sensitive reporter for DNA mismatches, as well as a versatile device for studying the structure, folding, and dynamics of complexly folded RNAs and DNAs.     

Phosphorus-31 nuclear magnetic resonance of highly oriented DNA fibers. 1. Static geometry of DNA double helices

The static geometry of the phosphodiesters in oriented fibers of DNA and a variety of polynucleotides was investigated by solid-state 31P nuclear magnetic resonance (NMR) spectroscopy. The structural parameters of the phosphodiester backbone expressed by two Euler angles beta and gamma were estimated on the basis of the NMR spectra of natural DNA, poly(dA).poly(dT), poly(rA).poly(dT), and poly-(rA).poly(rU). The Euler angles were calculated by using the known single crystal structures of a decamer, r(GCG)d(TATACGC), and a dodecamer, d(CGCGAATTCGCG). The distribution pattern of the Euler angles was quite different between these two oligonucleotides due to the different types of conformation, and it was fully consistent with the 31P NMR results, showing that the conformation of the B form DNA is very heterogeneous while that of the A or A' form is much more invariable with regard to the base composition. The structural parameters were also calculated by using various structures determined by the X-ray fiber diffraction studies, and they were evaluated on the basis of the 31P NMR data. Notably, poly(dA).poly(dT) fibers exhibited abnormal 31P NMR spectra which were very broad in line width and were not appreciably perturbed by hydration; a coiled double-helical structure is proposed as the most plausible model for this polymer.     

T4 RNA ligase catalyzes the synthesis of dinucleoside polyphosphates.

T4 RNA ligase has been shown to synthesize nucleoside and dinucleoside 5'-polyphosphates by displacement of the AMP from the E-AMP complex with polyphosphates and nucleoside diphosphates and triphosphates. Displacement of the AMP by tripolyphosphate (P3) was concentration dependent, as measured by SDS/PAGE. When the enzyme was incubated in the presence of 0.02 mm [alpha-32P] ATP, synthesis of labeled Ap4A was observed: ATP was acting as both donor (Km, microm) and acceptor (Km, mm) of AMP from the enzyme. Whereas, as previously known, ATP or dATP (but not other nucleotides) were able to form the E-AMP complex, the specificity of a compound to be acceptor of AMP from the E-AMP complex was very broad, and with Km values between 1 and 2 mm. In the presence of a low concentration (0.02 mm) of [alpha-32P] ATP (enough to form the E-AMP complex, but only marginally enough to form Ap4A) and 4 mm of the indicated nucleotides or P3, the relative rate of synthesis of the following radioactive (di)nucleotides was observed: Ap4X (from XTP, 100); Ap4dG (from dGTP, 74); Ap4G (from GTP, 49); Ap4dC (from dCTP, 23); Ap4C (from CTP, 9); Ap3A (from ADP, 5); Ap4ddA, (from ddATP, 1); p4A (from P3, 200). The enzyme also synthesized efficiently Ap3A in the presence of 1 mm ATP and 2 mm ADP. The following T4 RNA ligase donors were inhibitors of the synthesis of Ap4G: pCp > pAp > pA2'p.     

GU receptors of double helices mediate tRNA movement in the ribosome

A new RNA structural motif consisting of two double helices closely packed via minor grooves is found in many places in the ribosome structure. The packing requires that a GU base pair in one helix be packed against a Watson-Crick pair in the other helix. Two such motifs mediate the interaction of the P- and E-tRNA with the large ribosomal subunit. Analysis of the particular positions of these two motifs in view of the available data on occupancy of tRNA-binding sites and structural changes in the ribosome during the elongation cycle suggests a distinct role for each motif in tRNA translocation.     

Synthesis of dinucleoside tetraphosphates by RNA polymerase B (II) from calf thymus

Highly purified RNA polymerase B (II) from calf thymus catalyses the synthesis of dinucleoside tetraphosphates from ribonucleoside triphosphates in the absence of an oligonucleotide primer or additional protein factors. The reaction requires a DNA template and bivalent cations such as Mn2+ or Mg2+. It is strongly inhibited by heparin and high concentrations of alpha-amanitin but not by rifampicin. On a given template various dinucleoside tetraphosphates of different sequence are formed although the yield depends on the nature of the template.     

Parallel double helices of DNA. Conformational analysis of regular helices with the second order symmetry axis

We have performed a conformational analysis of DNA double helices with parallel directed backbone strands connected with the second order symmetry axis being at the same time the helix axis. The calculations were made for homopolymers poly(dA).poly(dA), poly(dC).poly(dC), poly(dG) poly(dG), and poly(dT).poly(dT). All possible variants of hydrogen bonding of base pairs of the same name were studied for each polymer. The maps of backbone chain geometrical existence were constructed. Conformational and helical parameters corresponding to local minima of conformational energy of "parallel" DNA helices, calculated at atom-atom approximation, were determined. The dependence of conformational energy on the base pair and on the hydrogen bond type was analysed. Two major conformational advantageous for "parallel" DNA's do not depend much on the hydrogen-bonded base pair type were indicated. One of them coincided with the conformational region typical for "antiparallel" DNA, in particular for the B-form DNA. Conformational energy of "parallel" DNA depends on the base pair type and for the most part is similar to the conformational energy of "antiparallel" B-DNA.     

Variability in the Geometry of RNA Double Helices Generated from Dinucleoside Building-Blocks

Abstract

A graphical method is presented for the generation of helical parameters from single-crystal structures of RNA nucleic acid fragments that are minimally dinucleosides. The method is compared with other published procedures, for a number of text examples. The RNA double helices generated from three different salts of the dinucleoside monophosphate GpC are examined in relation to the variations in helix morphology that are produced. It is shown that small differences between these GpC salts can be amplified to very distinct helix characteristics.     

Spectroscopic studies on the interaction of aristololactam-beta-D-glucoside with DNA and RNA double and triple helices: A comparative study.

The interaction of aristololactam-beta-D-glucoside (ADG), a DNA intercalating alkaloid, with the DNA triplexes, poly(dT). poly(dA)xpoly(dT) and poly(dC).poly(dG)xpoly(dC+), and the RNA triplex poly(rU).poly(rA)xpoly(rU) was investigated by circular dichroic, UV melting profile, spectrophotometric, and spectrofluorimetric techniques. Comparative interaction with the corresponding Watson-Crick duplexes has also been examined under identical experimental conditions. Triplex formation has been confirmed from biphasic thermal melting profiles and analysis of temperature-dependent circular dichroic measurements. The binding of ADG to triplexes and duplexes is characterized by the typical hypochromic and bathochromic effects in the absorption spectrum, quenching of steady-state fluorescence intensity, a decrease in fluorescence quantum yield, an increase or decrease of thermal melting temperatures, and perturbation in the circular dichroic spectrum. Scatchard analysis indicates that ADG binds both to the triplexes and the duplexes in a noncooperative manner. Binding parameters obtained from spectrophotometric measurements are best fit by the neighbor exclusion model. The binding affinity of ADG to the DNA triplexes is substantially stronger than to the RNA triplex. Thermal melting study further indicates that ADG stabilizes the Hoogsteen base-paired third strand of the DNA triplexes whereas it destabilizes the same strand of RNA triplex but stabilizes its Watson-Crick strands. Comparative data reveal that ADG exhibits a stronger binding to the triple helical structures than to the respective double helical structures.     

The mechanism of ion polarisation along DNA double helices

The orientation curves of short DNA fragments induced by electric field pulses are measured with high time resolution and analysed by efficient deconvolution techniques. A small, but clearly detectable delay of the 'on-field' orientation can be described accurately by the superposition of two exponential processes with opposite amplitudes. The time constant of the faster process is around 10 ns and the slower one in the range 50-1000 ns depending upon the electric field strength and chain length of the DNA fragment. The relation between amplitudes and time constants observed for each curve corresponds exactly to that expected for a convolution of two processes, where the first process is without optical response and becomes detectable only via the optical response of the second process. These results indicate that the first process reflects the polarisation of the ion atmosphere required for the second process of the orientation. Measurements at different ion concentrations c demonstrate that the reciprocal time constant of the fast process is a linear function of c and thus is consistent with an association reaction. The association rate constant evaluated from this dependence according to a simple bimolecular reaction model is 8 X 10(9) M-1 s-1 for a 95 base-pair fragment and is consistent with binding of Na+ to the helix, a reaction close to the limit of diffusion control. The association rate constant is almost independent of the electric field strength E, while the dissociation rate constant k- strongly increases with E, indicating dissociation of ions at high E values. The data suggest a linear correlation between log(k-) and E2 corresponding to a reaction driven by a dipole change. The apparent dipole change evaluated from this dependence is in the order of magnitude estimated for an elementary step of ion dissociation at one end of the helices. The combined results obtained from the polarisation and the orientation mechanism can be explained by dissociation of surprisingly few counterions biased towards one end of the helices. The experimental data obtained for a 76 base-pair fragment are analogous to those for the 95 base-pair fragment, whereas the 'slow' ion polarisation has not been detected for a fragment with 27 base-pairs. This result together with those obtained for the longer fragments at low field strengths indicate that there is a fast polarisation mechanism without 'ion dissociation' at low chain lengths and for low electric field strengths. This mechanism is replaced at high chain lengths and/or high electric field strengths by the ion dissociation mechanism.(ABSTRACT TRUNCATED AT 400 WORDS)     

Parallel double stranded helices and the tertiary structure of nucleic acids

Thermal denaturation of four oligonucleotides, viz. 3'-d(AT)5pO(CH2)6Opd(AT)5-3'(par(AT], 3'-d(AT)5pO(CH2)6Opd(AT)5-5'(anti(AT],3'-d(A)10pO(CH2) 6Op(T)10-3'(par(A-T], and 3'-d(A)10pO(CH2)6Opd(T)10-5' (anti(A-T], was studied in 0.01 M phosphate buffer, pH 7, in the presence of 0.1, 0.25, 0.5 and 1.0 M NaCl. All the oligomers were found to exist at a lower temperature (0 to 20 degrees C) as complexes composed either of two oligomer molecules (a canonical duplex) or of more oligomer molecules whereas, at a higher temperature (30 to 70 degrees C), they formed hairpins with a parallel (par(AT) and par(A-T] or antiparallel (anti(AT) and anti(A-T) orientation of the chains. Melting curves (A260(T] were used to calculate thermodynamic parameters for the formation of hairpins and "low-temperature" duplexes. Experiments on ethidium bromide binding to the oligonucleotides have shown that the oligomer anti(A-T) exists, at a low ionic strength, as a four stranded complex ("quadruplex") contains two antiparallel helices, d(A).d(T), which have a parallel orientation and are bound to one another owing to the formation of additional hydrogen bonds between nucleic acid bases. The possible biological function of quadruplexes is discussed.     

Interaction of the ruthenium red cation with nucleic acid double helices

The hexapositive complex cation ruthenium red very effectively stabilizes DNA and RNA double helices against thermal denaturation. In the presence of nucleic acid helices, this symmetric cation acquires an extrinsic CD spectrum near the wavelength of the dye's maximum absorbance. Competition experiments with single-stranded polyd(T) show this induced CD to be the result of selective binding to helical sites. The preferential affinity of ruthenium red for double helical binding sites is so great that it brings about biphasic absorbance- temperature profiles of polyd(A-T) at low [cation]: [polynucleotide phosphate]. The visible CD signal and fraction of helix melting at the upper transition increases with ruthenium red concentration until approximate charge neutrality is reached. These interactions, which have been studied in detail with the poly(U-U) helix as well as polyd(A-T), are likely largely electrostatic, since sufficient [NaCl] eliminates the bipliasic melting of polyd(A-T), renders the ultraviolet absorbance of poly (U) insensitive to ruthenium red, and abolishes the induced CD effects. The bipliasic melting of polyd(A-T) at intermediate [dye] is attributed to saturation of remaining double helical segments by cation migration from newly melted regions- Furthermore, virtually no change was observed in the induced CD upon melting through the first transition, whereas the effect is destroyed upon inciting through the second transition. A quantitative treatment of the data is used to obtain binding site size and association constant for the complex. The induced effect may prove useful in the exploration of exposed nucleic acid helical structure in such complex particles as nucleosomes or ribosomes.