Stability of single-nucleotide bulge loops embedded in a GAAA RNA hairpin stem

Forty-six RNA hairpins containing combinations of 3' or 5' bulge loops and a 3' or 5' fluorescein label were optically melted in 1 M NaCl, and the thermodynamic parameters ΔH°, ΔS°, ΔG°(37), and T(M) for each hairpin were determined. The bulge loops were of the group I variety, in which the identity of the bulge is known, and the group II variety, in which the bulged nucleotide is identical to one of its nearest neighbors, leading to ambiguity as to the exact position of the bulge. The fluorescein label at either the 3' end or 5' end of the hairpin did not significantly influence the stability of the hairpin. As observed with bulge loops inserted into a duplex motif, the insertion of a bulge loop into the stem of a hairpin loop was destabilizing. The model developed to predict the influence of bulge loops on the stability of duplex formation was extended to predict the influence of bulge loops on hairpin stability. Specifically, the influence of the bulge is related to the stability of the hairpin stem distal from the hairpin loop.     

Non-nearest-neighbor dependence of stability for group III RNA single nucleotide bulge loops

Thirty-five RNA duplexes containing single nucleotide bulge loops were optically melted and the thermodynamic parameters for each duplex determined. The bulge loops were of the group III variety, where the bulged nucleotide is either a AG/U or CU/G, leading to ambiguity to the exact position and identity of the bulge. All possible group III bulge loops with Watson–Crick nearest-neighbors were examined. The data were used to develop a model to predict the free energy of an RNA duplex containing a group III single nucleotide bulge loop. The destabilization of the duplex by the group III bulge could be modeled so that the bulge nucleotide leads to the formation of the Watson–Crick base pair rather than the wobble base pair. The destabilization of an RNA duplex caused by the insertion of a group III bulge is primarily dependent upon non-nearest-neighbor interactions and was shown to be dependent upon the stability of second least stable stem of the duplex. In-line structure probing of group III bulge loops embedded in a hairpin indicated that the bulged nucleotide is the one positioned further from the hairpin loop irrespective of whether the resulting stem formed a Watson–Crick or wobble base pair. Fourteen RNA hairpins containing group III bulge loops, either 3′ or 5′ of the hairpin loop, were optically melted and the thermodynamic parameters determined. The model developed to predict the influence of group III bulge loops on the stability of duplex formation was extended to predict the influence of bulge loops on hairpin stability.     

Non-nearest-neighbor dependence of the stability for RNA bulge loops based on the complete set of group I single-nucleotide bulge loops

Fifty-nine RNA duplexes containing single-nucleotide bulge loops were optically melted in 1 M NaCl, and the thermodynamic parameters DeltaH degrees, DeltaS degrees, DeltaG 37 degrees, and TM for each sequence were determined. Sequences from this study were combined with sequences from previous studies [Longfellow, C. E., et al. (1990) Biochemistry 29, 278-285; Znosko, B. M., et al. (2002) Biochemistry 41, 10406-10417], thus examining all possible group I single-nucleotide bulge loop and nearest-neighbor sequence combinations. The free energy increments at 37 degrees C for the introduction of a group I single-nucleotide bulge loop range between 1.3 and 5.2 kcal/mol. The combined data were used to develop a model for predicting the free energy of a RNA duplex containing a single-nucleotide bulge. For bulge loops with adjacent Watson-Crick base pairs, neither the identity of the bulge nor the nearest-neighbor base pairs had an effect on the influence of the bulge loop on duplex stability. The proposed model for prediction of the stability of a duplex containing a bulged nucleotide was primarily affected by non-nearest-neighbor interactions. The destabilization of the duplex by the bulge was related to the stability of the stems adjacent to the bulge. Specifically, there was a direct correlation between the destabilization of the duplex and the stability of the less stable duplex stem. The stability of a duplex containing a bulged nucleotide adjacent to a wobble base pair also was primarily affected by non-nearest-neighbor interactions. Again, there was a direct correlation between the destabilization of the duplex and the stability of the less stable duplex stem. However, when one or both of the bulge nearest neighbors was a wobble base pair, the free energy increment for insertion of a bulge loop is dependent upon the position and orientation of the wobble base pair relative the bulged nucleotide. Bulge sequences of the type ((5'UBX)(3'GY)), ((5'GBG)(3'UU)) and ((5'UBU)(3'GG)) are less destabilizing by 0.6 kcal/mol, and bulge sequences of the type ((5'GBX)(3'UY)) and ((5'XBU)(3'YG)) are more destabilizing by 0.4 kcal/mol than bulge loops adjacent to Watson-Crick base pairs.     

Determination of the secondary structure of group II bulge loops using the fluorescent probe 2-aminopurine

Eleven RNA hairpins containing 2-aminopurine (2-AP) in either base-paired or single nucleotide bulge loop positions were optically melted in 1 M NaCl; and, the thermodynamic parameters ΔH°, ΔS°, ΔG°₃₇, and T_M for each hairpin were determined. Substitution of 2-AP for an A (adenosine) at a bulge position (where either the 2-AP or A is the bulge) in the stem of a hairpin, does not affect the stability of the hairpin. For group II bulge loops such as AA/U, where there is ambiguity as to which of the A residues is paired with the U, hairpins with 2-AP substituted for either the 5′ or 3′ position in the hairpin stem have similar stability. Fluorescent melts were performed to monitor the environment of the 2-AP. When the 2-AP was located distal to the hairpin loop on either the 5′ or 3′ side of the hairpin stem, the change in fluorescent intensity upon heating was indicative of an unpaired nucleotide. A database of phylogenetically determined RNA secondary structures was examined to explore the presence of naturally occurring bulge loops embedded within a hairpin stem. The distribution of bulge loops is discussed and related to the stability of hairpin structures.     

Thermal stability of RNA hairpins containing a four-membered loop and a bulge nucleotide

Fourteen RNA hairpins containing a four-membered loop and a bulge nucleotide were synthesized and their thermal stabilities determined. The combined contribution of a four-membered loop and bulge A to the free energy of a hairpin is calculated to be 9.3 kcal/mol at 37 degrees C and successfully predicts the stability of an independent RNA hairpin. The introduction of a bulge nucleotide to the helical stem of an RNA hairpin destabilizes the molecule in a sequence-dependent manner. The individual thermodynamic contributions of a four-membered loop and bulge A, G, and U residues to the stability of an RNA hairpin loop are presented.     

A minimal RNA promoter for minus-strand RNA synthesis by the brome mosaic virus polymerase complex

The approximately 150 nt tRNA-like structure present at the 3' end of each of the brome mosaic virus (BMV) genomic RNAs is sufficient to direct minus-strand RNA synthesis. RNAs containing mutations in the tRNA-like structure that decrease minus-strand synthesis were tested for their ability to interact with RdRp (RNA-dependent RNA polymerase) using a template competition assay. Mutations that are predicted to disrupt the pseudoknot and stem B1 do not affect the ability of the tRNA-like structure to interact with RdRp. Similarly, the +1 and +2 nucleotides are not required for stable template-RdRp interaction. Mutations in the bulge and hairpin loops of stem C decreased the ability of the tRNA-like structure to interact with RdRp. Furthermore, in the absence of the rest of the BMV tRNA, stem C is able to interact with RdRp. The addition of an accessible initiation sequence containing ACCA3' to stem C created an RNA capable of directing RNA synthesis. Synthesis from this minimal minus-strand template is dependent on sequences in the hairpin and bulged loops.     

Solution structure of dAATAA and dAAUAA DNA bulges

The NMR structure analysis is described for two DNA molecules of identical stem sequences with a five base loop containing a pyrimidine, thymin or uracil, in between purines. These five unpaired nucleotides are bulged out and are known to induce a kink in the duplex structure. The dAATAA bulge DNA is kinked between the third and the fourth nucleotide. This contrasts with the previously studied dAAAAA bulge DNA where we found a kink between the fourth and fifth nucleotide. The total kinking angle is ~104° for the dAATAA bulge. The findings were supported by electrophoretic data and fluorescence resonance energy transfer measurements of a similar DNA molecule end-labeled by suitable fluorescent dyes. For the dAAUAA bulge the NMR data result in a similar structure as reported for the dAATAA bulge with a kinking angle of ~87°. The results are discussed in comparison with a rAAUAA RNA bulge found in a group I intron. Generally, the sequence-dependent structure of bulges is important to understand the role of DNA bulges in protein recognition.     

Comparative NMR study of A(n)-bulge loops in DNA duplexes: intrahelical stacking of A, A-A, and A-A-A bulge loops.

We have prepared a series of deoxyoligonucleotide duplexes of the sequence d(G-C-A-T-C-G-X-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-G-C), in which X represents either one (A), two (A-A), or three (A-A-A) unpaired adenine basis. Using two-dimensional proton and phosphorus NMR spectroscopy, we have characterized conformational features of these bulge-loop duplexes in solution. We find that Watson-Crick hydrogen bonding is intact for all 12 base pairs, including the GC bases that flank the bulge loop. Observation of NOE connectivities in both H2O and D2O allows us to unambiguously localize all of the bulged adenine residues to intrahelical positions within the duplex. This is in contrast to an earlier model for multiple-base bulge loops in DNA [Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840], in which all but the most 5' bulged base are looped out into solution. We find that insertion of two or three bases into the duplex results in the disruption of specific sequential NOEs for the base step across from the bulge loop site on the opposite strand. This disruption is characterized by a partial shearing apart of these bases, such that certain sequential NOEs for this base step are preserved. We observe a downfield-shifted phosphorus resonance, which we assign in the A-A-A bulge duplex to the 3' side of the last bulged adenine residue. Proton and phosphorus chemical shift trends within the An-bulge duplex series indicate that there is an additive effect on the structural perturbations caused by additional unpaired bases within the bulge loop. This finding parallels previous observations [Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840; Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 4833-4837] on the magnitude of the induced bending of DNA duplexes by multiple-base bulge loops.     

Thermodynamic parameters for an expanded nearest-neighbor model for the formation of RNA duplexes with single nucleotide bulges

Thirty-four RNA duplexes containing single nucleotide bulges were optically melted, and the thermodynamic parameters deltaH degrees, deltaS degrees, deltaG degrees (37), and T(M) for each sequence were determined. Data from this study were combined with data from previous thermodynamic data [Longfellow, C. E., Kierzek, R., and Turner, D. H. (1990) Biochemistry 29, 278-85] to develop a model that will more accurately predict the free energy of an RNA duplex containing a single nucleotide bulge. Differences between purine and pyrimidine bulges as well as differences between Group I duplexes, those in which the bulge is not identical to either neighboring nucleotide, and Group II duplexes, those in which the bulge is identical to at least one neighboring nucleotide, were considered. The length of the duplex, non-nearest-neighbor effects, and bulge location were also examined. A model was developed which divides sequences into two groups: those with pyrimidine bulges and those with purine bulges. The proposed model for pyrimidine bulges predicts deltaG degrees (37,bulge) = 3.9 kcal/mol + 0.10deltaG degrees (37,nn) + beta, while the model for purine bulges predicts deltaG degrees (37,bulge) = 3.3 kcal/mol - 0.30deltaG degrees (37,nn) + beta, where beta has a value of 0.0 and -0.8 kcal/mol for Group I and Group II sequences, respectively, and deltaG degrees (37,nn) is the nearest-neighbor free energy of the base pairs surrounding the bulge. The conformation of bulge loops present in rRNA was examined. Three distinct families of structures were identified. The bulge loop was either extrahelical, intercalated, or in a "side-step" conformation.     

Thermodynamic examination of trinucleotide bulged RNA in the context of HIV-1 TAR RNA

RNA structures contain many bulges and loops that are expected to be sites for inter- and intra-molecular interactions. Nucleotides in the bulge are expected to influence the structure and recognition of RNA. The same stability is assigned to all trinucleotide bulged RNA in the current secondary structure prediction models. In this study thermal denaturation experiments were performed on four trinucleotide bulged RNA, in the context of HIV-1 TAR RNA, to determine whether the bulge sequence affects RNA stability and its divalent ion interactions. Cytosine-rich bulged RNA were more stable than uracil-rich bulged RNA in 1 M KCl. Interactions of divalent ions were more favorable with uracil-rich bulged RNA by ~2 kcal/mol over cytosine-rich bulged RNA. The UCU-TAR RNA (wild type) is stabilized by 1.7 kcal/mol in 9.5 mM Ca²⁺ as compared with 1 M KCl, whereas no additional gain in stability is measured for CCC-TAR RNA. These results have implications for base substitution experiments traditionally employed to identify metal ion binding sites. To our knowledge, this is the first systematic study to quantify the effect of small sequence changes on RNA stability upon interactions with divalent ions.     

Bulged adenosine influence on the RNA duplex conformation in solution

The RNA single bulge motif is an unpaired residue within a strand of several complementary base pairs. To gain insight into structural changes induced by the presence of the adenosine bulge on RNA duplex, the solution structures of RNA duplex containing a single adenine bulge (5'-GCAGAAGAGCG-3'/5'-CGCUCUCUGC-3') and a reference duplex with all Watson-Crick base pairs (5'-GCAGAGAGCG-3'/5'-CGCUCUCUGC-3') have been determined by NMR spectroscopy. The reference duplex structure is a regular right-handed helix with all of the attributes of an A-type helix. In the bulged duplex, single adenine bulge stacks into the helix, and the bulge region forms a well-defined structure. Both structures were analyzed by the use of calculated helical parameters. Distortions induced by the accommodation of unpaired residue into the helical structure propagate over the entire structure and are manifested as the reduced base pairs inclination and x-displacement. Intrahelical position of bulged adenine A5 is stabilized by efficient stacking with 5'-neighboring residues G4.     

Solution structure of the pseudo-5' splice site of a retroviral splicing suppressor

Control of Rous sarcoma virus RNA splicing depends in part on the interaction of U1 and U11 snRNPs with an intronic RNA element called the negative regulator of splicing (NRS). A 23mer RNA hairpin (NRS23) of the NRS directly binds U1 and U11 snRNPs. Mutations that disrupt base-pairing between the loop of NRS23 and U1 snRNA abolish its negative control of splicing. We have determined the solution structure of NRS23 using NOEs, torsion angles, and residual dipolar couplings that were extracted from multidimensional heteronuclear NMR spectra. Our structure showed that the 6-bp stem of NRS23 adopts a nearly A-form duplex conformation. The loop, which consists of 11 residues according to secondary structure probing, was in a closed conformation. U913, the first residue in the loop, was bulged out or dynamic, and loop residues G914-C923, G915-U922, and U916-A921 were base-paired. The remaining UUGU tetraloop sequence did not adopt a stable structure and appears flexible in solution. This tetraloop differs from the well-known classes of tetraloops (GNRA, CUYG, UNCG) in terms of its stability, structure, and function. Deletion of the bulged U913, which is not complementary to U1 snRNA, increased the melting temperature of the RNA hairpin. This hyperstable hairpin exhibited a significant decrease in binding to U1 snRNP. Thus, the structure of the NRS RNA, as well as its sequence, is important for interaction with U1 snRNP and for splicing suppression.     

Discovering ligands for a microRNA precursor with peptoid microarrays

We have screened peptoid microarrays to identify specific ligands for the RNA hairpin precursor of miR-21, a microRNA involved in cancer and heart disease. Microarrays were printed by spotting a library of 7680 N-substituted oligoglycines (peptoids) onto glass slides. Two compounds on the array specifically bind RNA having the sequence and predicted secondary structure of the miR-21 precursor hairpin and have specific affinity for the target in solution. Their binding induces a conformational change around the hairpin loop, and the most specific compound recognizes the loop sequence and a bulged uridine in the proximal duplex. Functional groups contributing affinity and specificity were identified, and by varying a critical methylpyridine group, a compound with a dissociation constant of 1.9 μM for the miR-21 precursor hairpin and a 20-fold discrimination against a closely-related hairpin was created. This work describes a systematic approach to discovery of ligands for specific pre-defined novel RNA structures. It demonstrates discovery of new ligands for an RNA for which no specific lead compounds were previously known by screening a microarray of small molecules.     

Structure of the 5'' untranslated regulatory region of ferritin mRNA studied in solution.

Ferritin mRNAs are the first eukaryotic mRNAs for which a conserved, translational regulatory sequence has been identified. The sequence of twenty-eight nucleotides, called the IRE (iron regulatory element), is found in the 5'-noncoding region and is required for enhanced translation of ferritin mRNA by excess cellular iron; regulation occurs at initiation. The prediction of secondary structure in the IRE is a hairpin loop. We now report an analysis of the IRE structure in solution studied in natural ferritin mRNAs [H and H'(M) subunits] by primer extension, after modification or cleavage by dimethyl sulfate, RNAases T1 and V1, and the chemical nuclease 1, 10-phenanthroline-copper (OPCu) which cleaves single-stranded and bulged regions of RNA. Overall, the structure in solution of the ferritin mRNA regulatory region is a hairpin loop, with magnesium-sensitive features, in which half the stem is provided by the IRE and half by flanking regions; only secondary structure is conserved in the flanking regions. Predicted bulges or internal loops along the stem were clearly detected by OPCu but were missed by the more bulky probe RNAase T1, indicating the efficacy of OPCu in probing subtle features of RNA structure. Magnesium-dependent deviations from the predicted structure were observed in the stem between the hairpin loop and the bulge at C6. The location of the IRE in relation to the initiator AUG or the cap is variable in different ferritin mRNAs. However, the number of nucleotides in the base-paired flanking regions of known ferritin mRNAs is proportional to the distance of the IRE from the cap and places the secondary/tertiary structure 8-10 nucleotides from the cap where interference with initiation is likely.     

RNA binding properties of the coat protein from bacteriophage GA.

The coat protein of bacteriophage GA, a group II RNA phage, binds to a small RNA hairpin corresponding to its replicase operator. Binding is specific, with a Ka of 71 microM -1. This interaction differs kinetically from the analogous coat protein-RNA hairpin interactions of other RNA phage and also deviates somewhat in its pH and salt dependence. Despite 46 of 129 amino acid differences between the GA and group I phage R17 coat proteins, the binding sites are fairly similar. The essential features of the GA coat protein binding site are a based-paired stem with an unpaired purine and a four nucleotide loop having an A at position -4 and a purine at -7. Unlike the group I phage proteins, the GA coat protein does not distinguish between two alternate positions for the unpaired purine and does not show high specificity for a pyrimidine at position -5 of the loop.     

Solution structure of a trinucleotide A-T-A bulge loop within a DNA duplex.

We have synthesized an oligodeoxynucleotide duplex, d(G-C-A-T-C-G-A-T-A-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-C-G), with a three-base bulge loop (A-T-A) at a central site in the first strand. Nuclear Overhauser experiments (NOESY) in H2O indicate that the GC base pairs flanking the bulge loop are intact between 0 and 25 degrees C. Nuclear Overhauser effects in both H2O and D2O indicate that all bases within the bulge loop are stacked into the helix. These unpaired bases retain an anti conformation about their glycosidic bonds as they stack within the duplex. The absence of normal sequential connectivities between the two cytosine residues flanking the bulge site on the opposite strand indicates a disruption in the geometry of this base step upon insertion of the bulged bases into the helix. This conformational perturbation is more akin to a shearing apart of the bases, which laterally separates the two halves of the molecule, rather than the "wedge" model often invoked for single-base bulges. Using molecular dynamics calculations, with both NOE-derived proton-proton distances and relaxation matrix-calculated NOESY cross peak volumes as restraints, we have determined the solution structure of an A-T-A bulge loop within a DNA duplex. The bulged bases are stacked among themselves and with the guanine bases on either side of the loop. All three of the bulged bases are displaced by 2-3 A into the major groove, increasing the solvent accessibility of these residues. The ATA-bulge duplex is significantly kinked at the site of the lesion, in agreement with previously reported electron microscopy and gel retardation studies on bulge-containing duplexes [Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A 86, 4833-4837; Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840]. Bending occurs in a direction away from the bulge-containing strand, and we find a significant twist difference of 84 degrees between the two base pairs flanking the bulge loop site. This value represents 58% of the twist difference for base pairs four steps apart in B-DNA. These results suggest a structural mechanism for the bending of DNA induced by unpaired bases, as well as accounting for the effect bulge loops may have on the secondary and tertiary structures of nucleic acids.     

Effects of single-base bulges on intercalator binding to small RNA and DNA hairpins and a ribosomal RNA fragment

The way in which a single-base bulge might affect the structure of an RNA helix has been examined by preparing a series of six RNA hairpins, all with seven base pairs and a four-nucleotide loop. Five of the hairpins have single-base bulges at different positions. The intercalating cleavage reagent (methidiumpropyl)-EDTA-Fe(II) [MPE-Fe(II)] binds preferentially at a CpG sequence in the helix lacking a bulge and in four of the five hairpins with bulges. Hairpins with a bulge one or two bases to the 3' side of the CpG sequence bind ethidium 4-5-fold more strongly than the others. V1 RNase, which is sensitive to RNA backbone conformation in helices, detects a conformational change in all of the helices when ethidium binds; the most dramatic changes, involving the entire hairpin stem, are in one of the two hairpins with enhanced ethidium affinity. Only a slight conformational change is detected in the hairpin lacking a bulge. A bulge adjacent to a CpG sequence in a 100-nucleotide ribosomal RNA fragment enhances MPE-Fe(II) binding by an order of magnitude. These results extend our previous observations of bulges at a single position in an RNA hairpin [White, S. A., & Draper, D.E. (1987) Nucleic Acids Res. 15, 4049] and show that (1) a structural change in an RNA helix may be propagated for several base pairs, (2) bulges tend to increase the number of conformations available to a helix, and (3) the effects observed in small RNA hairpins are relevant to larger RNAs with more extensive structure. A bulge in a DNA hairpin identical in sequence with the RNA hairpins does not enhance MPE-Fe(II) binding affinity, relative to a control DNA hairpin. The effects of bulges on ethidium intercalation are evidently modulated by helix structure.     

A conserved hairpin structure in Alfamovirus and Bromovirus subgenomic promoters is required for efficient RNA synthesis in vitro

The coat protein gene in RNA 3 of alfalfa mosaic virus (AMV; genus Alfamovirus, family Bromoviridae) is translated from the subgenomic RNA 4. Analysis of the subgenomic promoter (sgp) in minus-strand RNA 3 showed that a sequence of 37 nt upstream of the RNA 4 start site (nt +1) was sufficient for full sgp activity in an in vitro assay with the purified viral RNA-dependent RNA-polymerase (RdRp). The sequence of nt -6 to -29 could be folded into a potential hairpin structure with a loop represented by nt -16, -17, and -18, and a bulge involving nt -23. By introducing mutations that disrupted base pairing and compensatory mutations that restored base pairing, it was shown that base pairing in the top half of the putative stem (between the loop and bulge) was essential for sgp activity, whereas base pairing in the bottom half of the stem was less stringently required. Deletion of the bulged residue A-23 or mutation of this residue into a C strongly reduced sgp activity, but mutation of A-23 into U or G had little effect on sgp activity. Mutation of loop residues A-16 and A-17 affected sgp activity, whereas mutation of U-18 did not. Using RNA templates corresponding to the sgp of brome mosaic virus (BMV; genus Bromovirus, family Bromoviridae) and purified BMV RdRp, evidence was obtained indicating that also in BMV RNA a triloop hairpin structure is required for sgp activity.