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.     

Crystal structure of an RNA helix recognized by a zinc-finger protein: an 18-bp duplex at 1.6 A resolution

The crystal structure of the 19-mer RNA, 5'-GAAUGCCUGCGAGCAUCCC-3' has been determined from X-ray diffraction data to 1.6 A resolution by the multiwavelength anomalous diffraction method from crystals containing a brominated uridine. In the crystal, this RNA forms an 18-mer self-complementary double helix with the 19th nucleotide flipped out of the helix. This helix contains most of the target stem recognized by the bacteriophage Mu Com protein (control of mom), which activates translation of an unusual DNA modification enzyme, Mom. The 19-mer duplex, which contains one A.C mismatch and one A.C/G.U tandem wobble pair, was shown to bind to the Com protein by native gel electrophoresis shift assay. Comparison of the geometries and base stacking properties between Watson-Crick base pairs and the mismatches in the crystal structure suggest that both hydrogen bonding and base stacking are important for stabilizing these mismatched base pairs, and that the unusual geometry adopted by the A.C mismatch may reveal a unique structural motif required for the function of Com.     

The 2 A structure of helix 6 of the human signal recognition particle RNA

BACKGROUND: The mammalian signal recognition particle (SRP) is an essential cytoplasmic ribonucleoprotein complex involved in targeting signal-peptide-containing proteins to the endoplasmic reticulum. Assembly of the SRP requires protein SRP19 to bind first to helix 6 of the SRP RNA before the signal-peptide-recognizing protein, SRP54, can bind to helix 8 of the RNA. Helix 6 is closed by a GGAG tetraloop, which has been shown to form part of the SRP19-binding site. RESULTS: The high-resolution (2.0 A) structure of a fragment of human SRP RNA comprising 29 nucleotides of helix 6 has been determined using the multiple anomalous dispersion (MAD) method and bromine-labelled RNA. In the crystal the molecule forms 28-mer duplexes rather than the native monomeric hairpin structure, although two chemically equivalent 11 base pair stretches of the duplex represent the presumed native structure. The duplex has highly distorted A-RNA geometry caused by the occurrence of several non-Watson-Crick base pairs. These include a 5'-GGAG-3'/3'-GAGG-5' purine bulge (which replaces the tetraloop) and a 5'-AC-3'/3'-CA-5' tandem mismatch that, depending on the protonation state of the adenine bases, adopts a different conformation in the two native-like parts of the structure. The structure also shows the 2'3'-cyclic phosphate reaction product of the hammerhead ribozyme cleavage reaction. CONCLUSIONS: The 29-mer RNA is the first RNA structure of the human SRP and provides some insight into the binding mode of SRP19. The observed strong irregularities of the RNA helix make the major groove wide enough and flat enough to possibly accommodate an alpha helix of SRP19. The variety of non-canonical base pairs observed enlarges the limited repertoire of irregular RNA folds known to date and the observed conformation of the 2'3'-cyclic phosphate containing Ade29 is consistent with the current understanding of the hammerhead ribozyme reaction mechanism.     

Solution structure of an RNA internal loop with three consecutive sheared GA pairs

Internal loops in RNA are important for folding and function. Many folding motifs are internal loops containing GA base pairs, which are usually thermodynamically stabilizing, i.e., contribute favorable free energy to folding. Understanding the sequence dependence of folding stability and structure in terms of molecular interactions, such as hydrogen bonding and base stacking, will provide a foundation for predicting stability and structure. Here, we report the NMR structure of the oligonucleotide duplex, 5'GGUGGAGGCU3'/3'PCCGAAGCCG5' (P = purine), containing an unusually stable and relatively abundant internal loop, 5'GGA3'/3'AAG5'. This loop contains three consecutive sheared GA pairs (trans Hoogsteen/Sugar edge AG) with separate stacks of three G's and three A's in a row. The thermodynamic consequences of various nucleotide substitutions are also reported. Significant destabilization of approximately 2 kcal/mol at 37 degrees C is found for substitution of the middle GA with AA to form 5'GAA3'/3'AAG5'. This destabilization correlates with a unique base stacking and hydrogen-bonding network within the 5'GGA3'/3'AAG5' loop. Interestingly, the motifs, 5'UG3'/3'GA5' and 5'UG3'/3'AA5', have stability similar to 5'CG3'/3'GA5' even though UG and UA pairs are usually less stable than CG pairs. Consecutive sheared GA pairs in the 5'GGA3'/3'AAG5' loop are preorganized for potential tertiary interactions and ligand binding.     

An NMR structural study of deaminated base pairs in DNA.

The structurally aberrant base pairs TG, UG and TI may occur in DNA as a consequence of deamination of 5-methylcytosine, cytosine and adenine respectively. Results of NMR spectroscopic studies are reported here for these deaminated base pairs in a model seven base pair long oligonucleotide duplex. We find that in all three cases, the DNA helix is a normal B form and both mispaired bases are intrahelical and hydrogen bonded with one another in a wobble geometry. Similarly, in all three cases, all sugars are found to be normal C2' endo in conformation. Symmetric structural perturbations are observed in the helix twist on the 3' side of the mispaired pyrimidine and on the 5' side of the mispaired purine. In all three cases, the amino group of the G residue on the 3' side of the mispaired pyrimidine shows hindered rotation. Although less thermodynamically stable than helices containing only Watson-Crick base pairs, these helices melt normally from the ends and not from the mispair outwards.     

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.     

Unusual duplex formation in purine rich oligodeoxyribonucleotides

The purine rich oligodeoxyribonucleotides 1C, d(ATGACGGAATA) and 2C, d(ATGAGCGAATA) alone exhibit highly cooperative melting transitions. Analysis of the concentration dependence of melting, and electrophoretic studies indicate that these oligomers can form an unusual purine rich offset double helix. The unusual duplex is predicted to contain four A.T, two G.C, and four G.A mismatch base pairs as well as a single A base stacked on the 3' end of each chain of the helix. Other possible models for the duplex are unlikely because they are predicted to contain many base pairs of low stability. Changing the central sequence to CGG or GGG should destabilize the duplex and this is observed. The unusual duplex of 2C is more stable than the duplex of 1C indicating that the stability of G.A base pairs is quite sensitive to the surrounding sequence. Addition of 1C and 2C to their complementary pyrimidine strands results in normal duplexes of similar stability. We feel that the unusual duplexes are significantly stabilized by the intrinsic stacking tendency of purine bases.     

Thermodynamic analysis of 5' and 3' single- and 3' double-nucleotide overhangs neighboring wobble terminal base pairs

Thermodynamic parameters are reported for duplex formation of 40 self-complementary RNA duplexes containing wobble terminal base pairs with all possible 3′ single and double-nucleotide overhangs, mimicking the structures of short interfering RNAs (siRNA) and microRNAs (miRNA). Based on nearest neighbor analysis, the addition of a single 3′ dangling nucleotide increases the stability of duplex formation up to 1 kcal/mol in a sequence-dependent manner. The addition of a second dangling nucleotide increases the stability of duplexes closed with wobble base pairs in an idiosyncratic manner. The results allow for the development of a nearest neighbor model, which improves the predication of free energy and melting temperature for duplexes closed by wobble base pairs with 3′ single or double-nucleotide overhangs. Phylogenetic analysis of naturally occurring miRNAs was performed. Selection of the effector miR strand of the mature miRNA duplex appears to be dependent on the orientation of the GU closing base pair rather than the identity of the 3′ double-nucleotide overhang. Thermodynamic parameters for the 5′ single terminal overhangs adjacent to wobble closing base pairs are also presented.     

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.     

NMR studies on an oligodeoxynucleotide containing 2-aminopurine opposite adenine

A heteroduplex containing the mismatch 2-aminopurine (AP)-adenine has been synthesized and studied by proton NMR. The mismatch was incorporated into the sequence d[CGG(AP)GGC].d-(GCCACCG). One-dimensional nuclear Overhauser effect measurements in H2O and two-dimensional nuclear Overhauser effect spectra in D2O show AP.A base pairs in a wobble structure in which both bases are in the anti conformation. The adenine is stacked well in the helix, but the helix twist between the adenine and neighboring cytosine in the 3' direction is unusually small. As a result, the aminopurine on the opposite strand is somewhat pushed out of the helix. From the measurements of the imino proton line widths, the two adjacent G.C base pairs are not found to be significantly destabilized by the presence of the purine-purine wobble pair.     

The dynamic structural basis of differential enhancement of conformational stability by 5'- and 3'-dangling ends in RNA

Unpaired bases at the end of an RNA duplex (dangling ends) can stabilize the core duplex in a sequence-dependent manner and are important determinants of RNA folding, recognition, and functions. Using 2-aminopurine as a dangling end purine base, we have employed femtosecond time-resolved fluorescence spectroscopy, combined with UV optical melting, to quantitatively investigate the physical and structural nature of the stacking interactions between the dangling end bases and the terminal base pairs. A 3'-dangling purine base has a large subpopulation that stacks on the guanine base of the terminal GC or UG pair, either intrastrand or cross-strand depending on the orientation of the pair, thus providing stabilization of different magnitudes. On the contrary, a 5'-dangling purine base only has a marginal subpopulation that stacks on the purine of the same strand (intrastrand) but has little cross-strand stacking. Thus a 5'-dangling purine does not provide significant stabilization. These stacking structures are not static, and a dangling end base samples a range of stacked and unstacked conformations with respect to the terminal base pair. Femtosecond time-resolved anisotropy decay reveals certain hindered base conformational dynamics that occur on the picosecond to nanosecond time scales, which allow the dangling base to sample these substates. When the dangling purine is opposite to a U and is able to form a potential base pair at the end of the duplex, there is an interplay of base stacking and hydrogen-bonding interactions that depends on the orientation of the base pair relative to the adjacent GC pair. By resolving these populations that are dynamically exchanging on fast time scales, we elucidated the correlation between dynamic conformational distributions and thermodynamic stability.     

Crystal structure of a model branchpoint-U2 snRNA duplex containing bulged adenosines

Bulged nucleotides play a variety of important roles in RNA structure and function, frequently forming tertiary interactions and sometimes even participating in RNA catalysis. In pre-mRNA splicing, the U2 snRNA base pairs with the intron branchpoint sequence (BPS) to form a short RNA duplex that contains a bulged adenosine that ultimately serves as the nucleophile that attacks the 5' splice site. We have determined a 2.18-A resolution crystal structure of a self-complementary RNA designed to mimic the highly conserved yeast (Saccharomyces cerevisiae) branchpoint sequence (5'-UACUAACGUAGUA with the BPS italicized and the branchsite adenosine underlined) base paired with its complementary sequence from U2 snRNA. The structure shows a nearly ideal A-form helix from which two unpaired adenosines flip out. Although the adenosine adjacent to the branchsite adenosine is the one bulged out in the structure described here, either of these adenosines can serve as the nucleophile in mammalian but not in yeast pre-mRNA splicing. In addition, the packing of the bulged RNA helices within the crystal reveals a novel RNA tertiary interaction in which three RNA helices interact through bulged adenosines in the absence of any divalent metal ions.     

Structure of the DNA interstrand cross-link of 4,5',8-trimethylpsoralen.

4,5',8-Trimethylpsoralen (TMP) cross-links a 5' TpA or a 5' ApT site by photoreacting with one thymine moiety in each DNA strand. We are interested in whether psoralen interstrand cross-links all share one structure or whether there are significant differences. In this paper, we employed a rapid method for probing the structure of the cross-link by making a series of TMP cross-linked duplexes containing specific base-pair mismatches. The relative stability provided by a base pair can be correlated with neighboring base pairs by comparing the extents of gel retardation when base-pair mismatches happen in each position. From our studies, we infer that with respect to the furan-side strand, the 5'T.A base pair of the two T.A base pairs in the TpA site is not hydrogen bonded. Immediately on each side of the cross-linked TpA site is a highly stabilized base pair. Next, a region of decreased stability occurs in each arm of a cross-linked duplex and these base pairs of least stability are located farther away from the cross-linked thymines as the lengths of the arms of the cross-linked helix increase. Finally, even in 7 M urea at 49 degrees C the cross-linked helix is hydrogen bonded at both ends of a duplex of 22 base pairs. We propose that the structures of interstrand cross-links in DNA vary appreciably with the DNA sequence, the length of the DNA duplex, and the structures of the DNA cross-linking agents.     

Wobble dG X dT pairing in right-handed DNA: solution conformation of the d(C-G-T-G-A-A-T-T-C-G-C-G) duplex deduced from distance geometry analysis of nuclear Overhauser effect spectra

We report below on features of the three-dimensional structure of the d(C-G-T-G-A-A-T-T-C-G-C-G) self-complementary duplex (designated 12-mer GT) containing symmetrical G X T mismatches in the interior of the helix. The majority of the base and sugar protons in the 12-mer GT duplex were assigned by two-dimensional nuclear Overhauser effect (NOESY) spectra in H2O and D2O solution. A set of 92 short (less than 4.5-A) proton-proton distances defined by lower and upper bounds for one symmetrical half of the 12-mer GT duplex were estimated from NOESY data sets recorded as a function of mixing time. These experimental distances combined with nucleotide bond length parameters were embedded into Cartesian space; several trial structures were refined to minimize bond geometry and van der Waals and chirality error. Confidence in this approach is based on the similarity of the refined structures for the solution conformation of the 12-mer GT duplex. The G and T bases pair through two imino-carbonyl hydrogen bonds, and stacking is maintained between the G X T wobble pair and adjacent Watson-Crick G X C pairs. The experimental distance information is restricted to base and sugar protons, and hence structural features such as base pair overlap, glycosidic torsion angles, and sugar pucker are well-defined by this combination of NMR and distance geometry methods. By contrast, we are unable to define the torsion angles about the bonds C3'-O3'-P-O5'-C5'-C4' in the backbone of the nucleic acid.     

Structural studies of DNA fragments: the G.T wobble base pair in A, B and Z DNA; the G.A base pair in B-DNA

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G.T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with O2 of T and O6 of G with N3 of T. The X-ray analyses establish that the G.T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G.A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.     

Thermodynamics of DNA duplexes with adjacent G.A mismatches.

The sequence 5'-d(ATGAGCGAAT) forms a very stable self-complementary duplex with four G.A mismatch base pairs (underlined) out of ten total base pairs [Li et al. (1991) Proc. Natl. Acad. Sci. U.S.A. 88, 26-30]. The conformation is in the general B-family and is stabilized by base-pair hydrogen bonding of an unusual type, by favorable base dipole orientations, and by extensive purine-purine stacking at the mismatched sites. We have synthesized 13 decamers with systematic variations in the sequence above to determine how the flanking sequences, the number of G.A mismatches, and the mismatch sequence order (5'-GA-3' or 5'-AG-3') affect the duplex stability. Changing A.T to G.C base pairs in sequences flanking the mismatches stabilizes the duplexes, but only to the extent observed with B-form DNA. The sequence 5'-pyrimidine-GA-purine-3', however, is considerably more stable than 5'-purine-GA-pyrimidine-3'. The most stable sequences with two pairs of adjacent G.A mismatches have thermodynamic parameters for duplex formation that are comparable to those for fully Watson-Crick base-paired duplexes. Similar sequences with single G.A pairs are much less stable than sequences with adjacent G.A mismatches. Reversing the mismatch order from 5'-GA-3' to 5'-AG-3' results in an oligomer that does not form a duplex. These results agree with predictions from the model derived from NMR and molecular mechanics and indicate that the sequence 5'-pyrimidine-GA-purine-3' forms a stable conformational unit that fits quite well into a B-form double helix.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structural Studies of DNA Fragments: The G·T Wobble Base Pair in A,B and Z DNA; The G·A Base Pair in B-DNA

Abstract

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G·T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with 02 of T and 06 of G with N3 of T. The X-ray analyses establish that the G·T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G·A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.     

Solution structure of DAPI selectively bound in the minor groove of a DNA T.T mismatch-containing site: NMR and molecular dynamics studies.

The solution structure of the complex between 4', 6-diamidino-2-phenylindole (DAPI) and DNA oligomer [d(GCGATTCGC)]2, containing a central T.T mismatch, has been characterized by combined use of proton one- and two-dimensional NMR spectroscopy, molecular mechanics and molecular dynamics computations including relaxation matrix refinement. The results show that the DAPI molecule binds in the minor groove of the central region 5'-ATT-3' of the DNA oligomer, which predominantly adopts a duplex structure with a global right-handed B-like conformation. In the final models of the complex, the DAPI molecule is located nearly isohelical with its NH indole proton oriented towards the DNA helix axis and forming a bifurcated hydrogen bond with the carbonyl O2 groups of a mismatched T5 and the T6 residue of the opposite strand. Mismatched thymines adopt a wobble base pair conformation and are found stacked between the flanking base pairs, inducing only minor local conformational changes in global duplex structure. In addition, no other binding mechanisms were observed, showing that minor groove binding of DAPI to the mismatch-containing site is favoured in comparison with any other previously reported interaction with G.C sequences.