Absence of correlation between base-pair sequence and RNA conformation

Crystal structures of two plasmid copy control related RNA duplexes: An 18 base pair duplex at 1.20 A resolution and a 19 base pair duplex at 1.55 A resolution

The structures of two RNA duplexes, whose sequences correspond to portions of the ColE1 plasmid copy control RNA I and RNA II, have been determined. Crystals containing the 18mers 5'-CA CCGUUGGUAGCGGUGC-3' and 5'-CACCGCUACCAACGGUGC-3' diffract to 1.20 A resolution while those containing the 19mers 5'-GCACCGUUGGUAGCGGUGC-3' and 5'-GCACCGCUACCAACGGUGC-3' diffract to 1.55 A resolution. Both duplexes are standard A form, with Watson-Crick base pairing throughout. Use of anisotropic atomic displacement factors in refinement of the 1.20 A structure dramatically improved refinement statistics, resulting in a final R(free) of 15.0% and a crystallographic R-factor of 11.6%. Perhaps surprisingly, these crystals of the 18 base pair RNA exhibit a 36-fold static disorder, resulting in a structure with a single sugar-phosphate backbone conformation and an averaged base composition at each residue. Since the sugar-phosphate backbone structure is identical in the 36 different nucleotides that are superimposed, there can be no sequence-dependent variation in the structure. The average ribose pucker amplitude is 45.8 degrees for the 18 base pair structure and 46.4 degrees for the 19 base pair structure; these values are respectively 19% and 20% larger than the average pucker amplitude reported from nucleoside crystal structures. A standard RNA water structure, based on analysis of the hydration of these crystal structures and that of the TAR RNA stem [Ippolito, J. A., and Steitz, T. A. (1998) Proc. Natl. Acad. Sci. U.S.A. 95, 9819-9824], has been derived, which has allowed us to predict water positions in lower resolution RNA crystal structures. We report a new RNA packing motif, in which three pro-S(p) phosphate oxygens interact with an ammonium ion.

The structure of an RNA "kissing" hairpin complex of the HIV TAR hairpin loop and its complement

We have used nuclear magnetic resonance (NMR) to obtain the structure of an RNA "kissing" hairpin complex formed between the HIV-2 TAR hairpin loop and a hairpin with a complementary loop sequence. Kissing hairpins are important in natural antisense reactions; their complex is a specific target for protein binding. The complex has all six nucleotides of each loop paired to form a bent quasicontinuous helix of three coaxially stacked helices: two stems plus a loop-loop interaction helix. Experimental constraints derived from heteronuclear and homonuclear NMR data on 13C and 15N-labeled RNA led to a structure for the loop-loop helix with an average root-mean-square deviation of 0.83 (+/-0.10) A for 33 converged structures relative to the average structure. The loop-loop helix of the kissing complex is distorted compared to A-form RNA. Its major groove is blocked by the phosphodiester bonds that connect the first loop residue of each hairpin with its own stem, and it is flanked by two negatively charged phosphate clusters. The loop-loop helix has alternating helical twists between adjacent base-pairs. The base-pairs at the helix junctions are overwound and three base-pairs near the helix junctions adopt high propeller twists. All these changes reduce the distance needed for the bridging phosphodiester bonds connecting each stem and loop to cross the major groove of the loop-loop helix, and result in a deformed RNA helix with localized perturbations in the minor groove surface. The alternating helical twist pattern, plus other distortions in the loop-loop helix may be important for Rom protein recognition of the kissing hairpin complex.

Substrate sequence effects on "hammerhead" RNA catalytic efficiency

The "hammerhead" RNA self-cleaving domain can be assembled from two RNA molecules: a large (approximately 34 nucleotide) ribozyme RNA containing most of the catalytically essential nucleotides and a small (approximately 13 nucleotide) substrate RNA containing the cleavage site. Four such hammerheads that contained identical catalytic core sequences but differed in the base composition of the helices that are involved in substrate binding had been reported to vary in cleavage rates by more than 70-fold under similar reaction conditions. Steady-state kinetic analyses reveal that kcat values are nearly the same for these hammerheads but Km values vary nearly 60-fold. The substrates for reactions having high Km values form aggregates that are virtually nonreactive. These observations demonstrate that the secondary structure of substrate RNA can be a major determinant of hammerhead catalytic efficiency.

Studies on the hammerhead RNA self-cleaving domain

Nine different hammerhead RNA self-cleaving domains consistent with the consensus secondary structure proposed by Keese and Symons (1987) were prepared and tested for cleavage. Each hammerhead was constructed from two oligoribonucleotides in two different configurations. Although cleavage was observed in all nine cases, the rates of cleavage varied by more than a thousand fold. The presence of RNA secondary structure incompatible with hammerhead formation in the individual oligos may be responsible for the large rate differences. We have also examined the degree of participation of a proposed dimer hammerhead intermediate in one case and conclude that, while such a four-stranded structure can form, it is not the preferred reaction intermediate.

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.

Base-stacking interactions in double-helical DNA structures: experiment versus theory

Atom-atom potential energy calculations have been undertaken for deriving stacking energies in double-helical structures. A comparison between the energy patterns of A- and B-type double-helical fragments determined by single-crystal X-ray diffraction methods versus idealized uniform models based on fibre diffraction data shows that the van der Waals stacking energy is largely sensitive to local changes in the relative orientation of adjacent base pairs. The sequence-dependent conformational variability observed in the high-resolution structures appears to be a consequence of the equipartitioning of the stacking energy along the double helix. The large energy variations expected for a uniform structure are dampened considerably in the observed structures by means of local changes in conformational features such as helix rotation and roll angles between base pairs.