Thermodynamic stabilities of internal loops with GU closing pairs in RNA

Many internal loops that form tertiary contacts in natural RNAs have GU closing pairs; examples include the tetraloop receptor and P1 helix docking site in group I introns. Thus, thermodynamic parameters of internal loops with GU closing pairs can contribute to the prediction of both secondary and tertiary structure. Oligoribonucleotide duplexes containing small internal loops with GU closing pairs were studied by optical melting, one-dimensional imino proton NMR, and one-dimensional phosphorus NMR. The thermodynamic stabilities of asymmetric internal loops with GU closing pairs relative to those of loops with GC closing pairs may be explained by hydrogen bonds. In contrast, the free energy increments for symmetric internal loops of two noncanonical pairs with GU closing pairs relative to loops with GC closing pairs show much more sequence dependence. Imino proton and phosphorus NMR spectra suggest that some GA pairs adjacent to GU closing pairs may form an overall thermodynamically stable but non-A-form conformation.     

Conformational determinants of tandem GU mismatches in RNA: insights from molecular dynamics simulations and quantum mechanical calculations

Structure and energetic properties of base pair mismatches in duplex RNA have been the focus of numerous investigations due to their role in many important biological functions. Such efforts have contributed to the development of models for secondary structure prediction of RNA, including the nearest-neighbor model. In RNA duplexes containing GU mismatches, 5'-GU-3' tandem mismatches have a different thermodynamic stability than 5'-UG-3' mismatches. In addition, 5'-GU-3' mismatches in some sequence contexts do not follow the nearest-neighbor model for stability. To characterize the underlying atomic forces that determine the structural and thermodynamic properties of GU tandem mismatches, molecular dynamics (MD) simulations were performed on a series of 5'-GU-3' and 5'-UG-3' duplexes in different sequence contexts. Overall, the MD-derived structural models agree well with experimental data, including local deviations in base step helicoidal parameters in the region of the GU mismatches and the model where duplex stability is associated with the pattern of GU hydrogen bonding. Further analysis of the simulations, validated by data from quantum mechanical calculations, suggests that the experimentally observed differences in thermodynamic stability are dominated by GG interstrand followed by GU intrastrand base stacking interactions that dictate the one versus two hydrogen bonding scenarios for the GU pairs. In addition, the inability of 5'-GU-3' mismatches in different sequence contexts to all fit into the nearest-neighbor model is indicated to be associated with interactions of the central four base pairs with the surrounding base pairs. The results emphasize the role of GG and GU stacking interactions on the structure and thermodynamics of GU mismatches in RNA.     

Pronounced instability of tandem IU base pairs in RNA

Optical melting was used to determine the stabilities of three series of RNA oligomers containing tandem XU base pairs, GGCXUGCC (5′XU3′), GGCUXGCC (5′UX3′) and GGCXXGGC/CCGUUCCG (5′XX3′), where X is either A, G or I (inosine). The helices containing tandem AU base pairs were the most stable in the first two series (5′XU3′ and 5′UX3′), with an average melting temperature ~11°C higher than the helices with tandem 5′GU3′ base pairs and 25°C higher than the helices with tandem 5′IU3′ base pairs. For the third series (5′XX3′), the helix containing tandem GG is the most stable, with an average melting temperature ~2°C higher than the helix with tandem AA base pairs and ~24°C higher than the helix with tandem II base pairs. The thermodynamic stability of the oligomers with tandem IU base pairs was also investigated as a function of magnesium ion concentration. As with normal A–U or G–U tandem duplexes, the data could best be interpreted as non-specific binding of magnesium ions to the inosine-containing RNA oligonucleotides.     

NMR structures of (rGCUGAGGCU)2 and (rGCGGAUGCU)2: probing the structural features that shape the thermodynamic stability of GA pairs

The NMR structures of [see text] and [see text] are reported. The internal loop, [see text], is about 2 kcal/mol more stable than [see text] at 37 degrees C. The duplexes assemble into similar global folds characterized by the formation of tandem sheared GA pairs. The different stabilities of the loops are accompanied by differences in the local structure of the closing GU pairs. In the [see text] internal loop, the GU pairs form canonical wobble configurations with two hydrogen bonds, whereas in [see text], the GU pairs form a single hydrogen bond involving the amino group, GH22, and the carbonyl group, UO4. This pairing is similar to the GU closing pair of the 690 hairpin loop found in E. coli 16S rRNA. The [see text] and [see text] structures reveal how the subtle interplay between stacking and hydrogen bonding determines sequence dependent conformation and thermodynamic stability. Thus, this work provides structural and thermodynamic benchmarks for theoreticians in the ongoing effort to understand the sequence dependence of RNA physicochemical properties.     

Helix Capping in RNA Structure

Helices are an essential element in defining the three-dimensional architecture of structured RNAs. While internal basepairs in a canonical helix stack on both sides, the ends of the helix stack on only one side and are exposed to the loop side, thus susceptible to fraying unless they are protected. While coaxial stacking has long been known to stabilize helix ends by directly stacking two canonical helices coaxially, based on analysis of helix-loop junctions in RNA crystal structures, herein we describe helix capping, topological stacking of a helix end with a basepair or an unpaired nucleotide from the loop side, which in turn protects helix ends. Beyond the topological protection of helix ends against fraying, helix capping should confer greater stability onto the resulting composite helices. Our analysis also reveals that this general motif is associated with the formation of tertiary structure interactions. Greater knowledge about the dynamics at the helix-junctions in the secondary structure should enhance the prediction of RNA secondary structure with a richer set of energetic rules and help better understand the folding of a secondary structure into its three-dimensional structure. These together suggest that helix capping likely play a fundamental role in driving RNA folding.     

Identification and assignment of base pairs in three helical stems of Torulopsis utilis ribosomal 5S RNA and its RNase T1 and RNase T2 cleaved fragments via 500-MHz proton homonuclear overhauser enhancements

Imino proton resonances in the downfield region (10-14 ppm) of the 500-MHz 1H NMR spectrum of Torulopsis utilis 5S RNA are identified (A X U, G X C, or G X U) and assigned to base pairs in helices I, IV, and V via analysis of homonuclear Overhauser enhancements (NOE) from intact T. utilis 5S RNA, its RNase T1 and RNase T2 digested fragments, and a second yeast (Saccharomyces cerevisiae) 5S RNA whose nucleotide sequence differs at only six residues from that of T. utilis 5S RNA. The near-identical chemical shifts and NOE behavior of most of the common peaks from these four RNAs strongly suggest that helices I, IV, and V retain the same conformation after RNase digestion and that both T. utilis and S. cerevisiae 5S RNAs share a common secondary and tertiary structure. Of the four G X U base pairs identified in the intact 5S RNA, two are assigned to the terminal stem (helix I) and the other two to helices IV and V. Seven of the nine base pairs of the terminal stem have been assigned. Our experimental demonstration of a G X U base pair in helix V supports the 5S RNA secondary structural model of Luehrsen and Fox [Luehrsen, K. R., & Fox, G.E. (1981) Proc. Natl. Acad. Sci. U.S.A. 78, 2150-2154]. Finally, the base-pair proton peak assigned to the terminal G X U in helix V of the RNase T2 cleaved fragment is shifted downfield from that in the intact 5S RNA, suggesting that helices I and V may be coaxial in intact T. utilis 5S RNA.     

Stability of XGCGCp, GCGCYp, and XGCGCYp helixes: an empirical estimate of the energetics of hydrogen bonds in nucleic acids

The stabilizing effects of dangling ends and terminal base pairs on the core helix GCGC are reported. Enthalpy and entropy changes of helix formation were measured spectrophotometrically for AGCGCU, UGCGCA, GGCGCCp, CGCGCGp, and the corresponding pentamers XGCGCp and GCGCYp containing the GCGC core plus a dangling end. Each 5' dangling end increases helix stability at 37 degrees C roughly 0.2 kcal/mol and each 3' end from 0.8 to 1.7 kcal/mol. The free energy increments for dangling ends on GCGC are similar to the corresponding increments reported for the GGCC core [Freier, S. M., Alkema, D., Sinclair, A., Neilson, T., & Turner, D. H. (1985) Biochemistry 24, 4533-4539], indicating a nearest-neighbor model is adequate for prediction of stabilization due to dangling ends. Nearest-neighbor parameters for prediction of the free energy effects of adding dangling ends and terminal base pairs next to G.C pairs are presented. Comparison of these free energy changes is used to partition the free energy of base pair formation into contributions of "stacking" and "pairing". If pairing contributions are due to hydrogen bonding, the results suggest stacking and hydrogen bonding make roughly comparable favorable contributions to the stability of a terminal base pair. The free energy increment associated with forming a hydrogen bond is estimated to be -1 kcal/mol of hydrogen bond.     

Close packing of helices 3 and 12 of 16 S rRNA is required for the normal ribosome function

The along-groove packing motif is a quasi-reciprocal arrangement of two RNA double helices in which a backbone of each helix is closely packed within the minor groove of the other helix. At the center of the inter-helix contact, a GU base pair in one helix packs against a Watson-Crick base pair in the other helix. Here, based on in vivo selection from a combinatorial gene library of 16 S rRNA and on functional characterization of the selected clones, we demonstrate that the normal ribosome performance requires that helices 3 and 12 be closely packed. In some clones the Watson-Crick and GU base pairs exchange in their positions between the two helices, which affects neither the quality of the helix packing, nor the ribosome function. On the other hand, perturbations in the close packing usually lead to a substantial drop in the ribosome activity. The functionality of the clones containing such perturbations may depend on the presence of particular elements in the vicinity of the area of contact between helices 3 and 12. Such cases do not exist in natural 16 S rRNA, and their selection enriches our knowledge of the constraints imposed on the structure of ribosomal RNA in functional ribosomes.     

Sequence dependence for the energetics of dangling ends and terminal base pairs in ribonucleic acid

Stability increments of terminal unpaired nucleotides (dangling ends) and terminal base pairs on the core helixes AUGCAU and UGCGCA are reported. Enthalpy, entropy, and free energy changes of helix formation were measured spectrophotometrically for 18 oligoribonucleotides containing the core sequences. The results indicate 3' dangling purines add more stability than 3' dangling pyrimidines. In most cases, the additional stability from a 3' dangling end on an AU base pair is less than that on a GC base pair [Freier, S.M., Burger, B.J., Alkema, D., Neilson, T., & Turner, D.H. (1985) Biochemistry 22, 6198-6206]. The sequence dependence provides a test for the importance of dangling ends for various RNA interactions. Correlations are suggested with codon context effects and with the three-dimensional structure of yeast phenylalanine transfer RNA. In the latter case, all terminal unpaired nucleotides having stability increments more favorable than -1 kcal/mol are stacked on the adjacent base pair. All terminal unpaired nucleotides having stability increments less favorable than -0.3 kcal/mol are not stacked on the adjacent base pair. In several cases, this lack of stacking is associated with a turn in the sugar-phosphate backbone. This suggests stability increments measured on oligoribonucleotides may be useful for predicting tertiary structure in large RNA molecules. Comparison of the stability increments for terminal dangling ends and base pairs, and of terminal GC and AU base pairs, indicates the free energy increment associated with forming a hydrogen bond can be about -1 kcal/mol of hydrogen bond.     

Thermodynamics of single mismatches in RNA duplexes

The thermodynamic properties and structures of single mismatches in short RNA duplexes were studied in optical melting and imino proton NMR experiments. The free energy increments at 37 degrees C measured for non-GU single mismatches range from -2.6 to 1.7 kcal/mol. These increments depend on the identity of the mismatch, adjacent base pairs, and the position in the helix. UU and AA mismatches are more stable close to a helix end, but GG mismatch stability is essentially unaffected by the position in the helix. Approximations are suggested for predicting stabilities of single mismatches in short RNA duplexes.     

Secondary structure of 5S RNA: NMR experiments on RNA molecules partially labeled with nitrogen-15

A method has been found for reassembling fragment 1 of Escherichia coli 5S RNA from mixtures containing strand III (bases 69-87) and the complex consisting of strand II (bases 89-120) and strand IV (bases 1-11). The reassembled molecule is identical with unreconstituted fragment 1. With this technique, fragment 1 molecules have been constructed 15N-labeled either in strand III or in the strand II-strand IV complex. Spectroscopic data obtained with these partially labeled molecules show that the terminal helix of 5S RNA includes the GU and GC base pairs at positions 9 and 10 which the standard model for 5S secondary structure predicts [see Delihas, N., Anderson, J., & Singhal, R. P. (1984) Prog. Nucleic Acid Res. Mol. Biol. 31, 161-190] but that these base pairs are unstable both in the fragment and in native 5S RNA. The data also assign three resonances to the helix V region of the molecule (bases 70-77 and 99-106). None of these resonances has a "normal" chemical shift even though two of them correspond to AU or GU base pairs in the standard model. The implications of these findings for our understanding of the structure of 5S RNA and its complex with ribosomal protein L25 are discussed.     

RNA helix stability in mixed Na+/Mg2+ solution

A recently developed tightly bound ion model can account for the correlation and fluctuation (i.e., different binding modes) of bound ions. However, the model cannot treat mixed ion solutions, which are physiologically relevant and biologically significant, and the model was based on B-DNA helices and thus cannot directly treat RNA helices. In the present study, we investigate the effects of ion correlation and fluctuation on the thermodynamic stability of finite length RNA helices immersed in a mixed solution of monovalent and divalent ions. Experimental comparisons demonstrate that the model gives improved predictions over the Poisson-Boltzmann theory, which has been found to underestimate the roles of multivalent ions such as Mg2+ in stabilizing DNA and RNA helices. The tightly bound ion model makes quantitative predictions on how the Na+-Mg2+ competition determines helix stability and its helix length-dependence. In addition, the model gives empirical formulas for the thermodynamic parameters as functions of Na+/Mg2+ concentrations and helix length. Such formulas can be quite useful for practical applications.     

The effect of base mismatches in the substrate recognition helices of hammerhead ribozymes on binding and catalysis.

The ability of the hammerhead ribozyme to distinguish between matched and mismatched substrates was evaluated using two kinetically defined ribozymes that differed in the length and sequence of the substrate recognition helices. A mismatch in the innermost base pair of helix I affected k2, the chemical cleavage step, while more distal mismatches had no such effect. In contrast, mismatches in any of the four innermost base pairs of helix III affected k2. Chase experiments indicated that mismatches also increased the rate of substrate dissociation by at least 20-100-fold, as expected from the stabilities of RNA helices.     

Is there a special function for U.G basepairs in ribosomal RNA?

U.G basepairs are well-established elements of RNA structure. The geometry of this pair is different, however, from classical Watson-Crick basepairs. This leads to an unusual stacking of the basepair: overlap with the basepair at the 5' side of the U (and the 3' side of the G) is strong (stacked) while it is weak with the basepair on the other side (destacked). The closure of an RNA helix by a U.G pair will be energetically unfavourable when the U residue occupies the 5' end. In transfer RNA there is a strong selection against a 'destacked' U.G pair at helix ends. In the 16S rRNA model of Escherichia coli there are 72 U.G pairs of which 36 or 22 occupy a helix end, depending on how such an end is defined. There is a slight preference for 'stacked' U.G's in these positions. It is remarkable, however, that of 13 very conserved U.G pairs in the 16S (-like) rRNA, 7 occur at helix ends and that 5 of these have the 'destacked' configuration. It is suggested that these pairs, if they exist at all in a hydrogen-bounded form, are stabilized by co-axial stacking with other helices or by interaction with a protein.     

Contributions of dangling end stacking and terminal base-pair formation to the stabilities of XGGCCp, XCCGGp, XGGCCYp, and XCCGGYp helixes

The role of stacking in terminal base-pair formation was studied by comparison of the stability increments for dangling ends to those for fully formed base pairs. Thermodynamic parameters were measured spectrophotometrically for helix formation of the hexanucleotides AGGCCUp, UGGCCAp, CGGCCGp, GCCGGCp, and UCCGGAp and for the corresponding pentanucleotides containing a 5'-dangling end on the GGCCp or CCGGp core helix. In 1 M NaCl at 1 X 10(-4) M strands, a 5'-dangling nucleotide in this series increases the duplex melting temperature (Tm) only 0-4 degrees C, about the same as adding a 5'-phosphate. In contrast, a 3'-dangling nucleotide increases the Tm at 1 X 10(-4) M strands 7-23 degrees C, depending on the sequence [Freier, S. M., Burger, B. J., Alkema, D., Neilson, T., & Turner, D. H. (1983) Biochemistry 22, 6198-6206]. These results are consistent with stacking patterns observed in A-form RNA. The stability increments from terminal A.U, C.G, or U.A base pairs on GGCC or a terminal U.A pair on CCGG are nearly equal to the sums of the stability increments from the corresponding dangling ends. This suggests stacking plays a large role in nucleic acid stability. The stability increment from the terminal base pairs in GCCGGCp, however, is about 5 times the sum of the corresponding dangling ends, suggesting hydrogen bonding can also make important contributions.     

Free energy of imperfect nucleic acid helices. 3. Small internal loops resulting from mismatches

Physical studies of enzymioally synthesized oligoribonucleotides of defined sequence are used to evaluate quantitatively the destabilizing influence of mismatched bases in a double helix. The series (A-)₄G(-C)_n(-U)₄, N = 1 to 6, exist as imperfect dimer helices when N is equal to or less than 4, and as monomolecular hairpin helices when N is 5 and 6. Internal loops become progressively more destabilizing as their size increases from 2 to 4 to 6 nucleotides resulting from 1, 2 and 3 consecutive mismatched base pairs. However, the stability of a helix will generally be greater if a given number of mismatched pairs occur consecutively rather than in isolation from one another.These data may be used for improved calculations of stability of RNA secondary structure, to estimate the frequency of structural fluctuations in a double helix and to assess the stability of modified polynucleotide helices. An unmodified double helix of one million randomly arranged base pairs should contain on the time average approximately 10 G.C and 500 A.U pairs in non-hydrogen bonded, unstacked conformations at 25 °C. Our estimate of the effect of mismatching on T_m values of high polymers is less precise because of the long temperature extrapolation required. However, we estimate that DNA or RNA treated with mutagens which interrupt up to 20% of the nucleotide pairs will show a drop of about 1.2 deg. C in melting temperature with each unit per cent of modification.     

Polymer-supported RNA synthesis and its application to test the nearest-neighbor model for duplex stability

A solid-phase method using a phosphoramidite approach is described for synthesis of oligoribonucleotides. The method was used to synthesize pairs of oligomers with identical nearest neighbors but different sequences. Comparison of thermodynamic parameters for these pairs provides a test of the nearest-neighbor hypothesis for prediction of helix stability. In general, pairs of sequences with identical nearest neighbors have enthalpy and entropy changes for helix formation that differ by 8% on average, delta Go37 that differ by 6% on average, and melting temperatures within 0-5 degrees C of each other. These limits are typical of the accuracy that should be expected from nearest-neighbor predictions of RNA helix stability. UCAUGA and UGAUCA have the same nearest neighbors but melting temperatures that differ by 7 degrees C. This suggests some sequences will not be approximated well by the nearest-neighbor model.     

Secondary structure at the 3' terminal region of RNA coliphages: comparison with tRNA

Secondary structure models for the 3' non-coding region of the four groups of coliphage RNA are proposed based on comparative sequence analysis and on previously published data on the sensitivity of nucleotides in MS2 RNA to chemical modification and enzymes. We report the following observations. (1) In contrast to the coding regions, the structure at the 3' terminus is characterized by stable regular helices. We note the occurrence of the loop sequences 5'-GUUCGC and 5'-CGAAAG, that are reported to confer exceptional stability to stem structures. These features are probably present to promote the segregation of mother and daughter strands during replication. (2) Comparison of homologous helices indicates that only those base pair substitutions are allowed that maintain the thermodynamic stability. (3) We have compared the structure of phage RNA with tRNA. Overall similarity is low, but one common element may exist. It is a quasi-continuous helix of 12 basepairs that could be the equivalent of the 12 basepair long coaxially stacked helix, formed by the T psi C arm and the aminoacyl acceptor arm in tRNA. As in tRNA, this structure element starts after the fourth nucleotide from the 3' end. (4) Phage RNA contains a large variable region of about 35 nucleotides bulging out from the quasi-continuous helix. We speculate that the variable loop in present-day tRNA could be the remnant of the variable region found in phage RNA. The variable region contains overlapping binding sites for the replicase enzyme and the maturation protein. This common binding site may serve as a switch from replication to packaging.     

Sequence dependence for the energetics of terminal mismatches in ribooligonucleotides

Stability increments of terminal mismatches on the core helixes AUGCAU and UGCGCA are reported. Enthalpy, entropy, and free energy changes of helix formation were measured spectrophotometrically for 15 oligoribonucleotides containing the core sequences and various mismatches. Free energy increments for mismatches in this series range from -0.5 to -1.1 kcal/mol. These increments for mismatches on AU base pairs are smaller than those measured previously on GC base pairs [Freier, S.M., Kierzek, R., Caruthers, M.H., Neilson, T., & Turner, D.H. (1986) Biochemistry 25, 3209-3213]. The terminal GU mismatches in the sequences GAUGCAUUp and UAUGCAUGp add approximately the same stability increment as the corresponding terminal AU mismatch. The stability increments for pyrimidine-pyrimidine and pyrimidine-purine mismatches can be approximated within 0.3 kcal/mol by adding the stability increments for the corresponding 3' and 5' unpaired nucleotides (dangling ends). Stability increments for purine-purine mismatches are approximated well by the stability increment for the corresponding 3' dangling end made more favorable by 0.2 kcal/mol. These approximations are used to provide a table of stability increments for all 48 possible sequences of mismatches.