Crystal structures of two forms of a 14-mer RNA/DNA chimer duplex with double UU bulges: a novel intramolecular U*(A x U) base triple.

The RNA/DNA 14-mer, (gguauuucgguaCc)2 with consecutive uridine bulges (underlined) on each strand has been determined in two crystal forms, spermine bound (Sp-form) and spermine free (Sp-free). The former was solved by the MAD method with three-wavelength data collected at Brookhaven National Laboratory (BNL); the later isomorphous structure was solved by the molecular replacement method using data collected on our Raxis IIc imaging plate system. The two crystal forms belong to the space group C2 with one molecule of double-stranded 14 mer in the asymmetric unit. The Sp-form has cell constants, a = 60.06, b = 29.10, c = 52.57 A, beta = 120.79 degrees and was refined to 1.7 A resolution with a final Rwork/Rfree of 19.8%/22.7% using 8,549 independent reflections. The Sp-free structure has cell constants, a = 60.06, b = 29.58, c = 52.50 A, beta = 120.85 degrees and was refined to 1.8 A with a final Rwork/ Rfree of 20.8%/23.2% using 6,285 unique reflections. The two structures are identical, except that the Sp-form has a spermine bound in the major groove, parallel to the RNA helical axis. One of the uridine bulges forms a novel intramolecular U*(A x U) base triple. The helices are in the C3'-endo conformation (A-form), but the bulges adopt the C2'-endo sugar pucker. Furthermore, the bulges induce a kink (30 degrees) in the helix axis and a very large twist (55 degrees) between the base pairs flanking the bulges. The Sp-form has one Mg2+ ion whereas the Sp-free form has two Mg2+ ions.     

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.     

Crystal structure of an adenine bulge in the RNA chain of a DNA.RNA hybrid, d(CTCCTCTTC).r(gaagagagag)

Crystal structure of a DNA.RNA hybrid, d(CTCCTCTTC).r(gaagagagag), with an adenine bulge in the polypurine RNA strand was determined at 2.3 A resolution. The structure was solved by the molecular replacement method and refined to a final R-factor of 19.9% (Rfree 22.2%). The hybrid duplex crystallized in the space group I222 with unit cell dimensions, a = 46.66 A, b = 47.61 A and c = 54.05 A, and adopts the A-form conformation. All RNA and DNA sugars are in the C3'-endo conformation, the glycosyl angles in anti conformation and the majority of the C4'-C5' torsion angles in g+ except two trans angles, in conformity with the C3'-endo rigid nucleotide hypothesis. The adenine bulge is looped out and it is also in the anti C3'-endo conformation. The bulge is involved in a base-triple (C.g)*a interaction with the end base-pair (C9.g10) in the minor groove of a symmetry-related molecule. The 2' hydroxyl group of g15 is hydrogen bonded to O2P and O5' of g17, skipping the bulged adenine a16 and stabilizing the sugar-phosphate backbone of the hybrid. The hydrogen bonding and the backbone conformation at the bulged adenine site is very similar to that found in the crystal structure of a protein-RNA complex.     

Bulge loops used to measure the helical twist of RNA in solution.

Bulge loops are commonly found in helical segments of cellular RNAs. When incorporated into long double-stranded RNAs, they may introduce points of flexibility or permanent bend that can be detected by the altered electrophoretic gel mobility of the RNA. We find that a single An or Un bulge loop near the middle of a long RNA helix significantly retards the RNA during polyacrylamide gel electrophoresis if n greater than or equal to 2. The mobility of an RNA containing two A2 bulges various periodically with the number of base pairs between the bulges. We interpret this to mean that A2 bulges varies periodically with the number of base pairs between the bulges. We interpret this to mean that Z2 bulges form torsionally stiff bends in the helix; the gel mobility reaches a minimum when the total helical twist between the bulges rotates the arms of the molecule into a cis conformation. The gel mobilities are proportional to the predicted end-to-end distance of the RNA if the average RNA helical repeat is 11.8 +/- 0.2 bp/turn and there is no helical twist (3 +/- 9 degrees) associated with the bulge (data obtained in 0.15 M Na+). Other sizes and sequences of bulges have very different effects on RNA helix conformation and flexibility. U2 bulges bend the helix to a much smaller degree than A2 bulges, while longer A or U bulge sequences probably allow bends of 90 degrees or more; all of these may be fairly flexible joints.(ABSTRACT TRUNCATED AT 250 WORDS)     

Solution structure of an LNA hybridized to DNA: NMR study of the d(CT(L)GCT(L)T(L)CT(L)GC):d(GCAGAAGCAG) duplex containing four locked nucleotides

We have used two-dimensional (1)H NMR spectroscopy at 750 MHz to determine a high-resolution solution structure of an oligonucleotide containing restricted nucleotides with a 2'-O, 4'-C-methylene bridge (LNA) hybridized to the complementary DNA strand. The LNA:DNA duplex examined contained four thymidine LNA modifications (T(L), d(C1T(L)2G3C4T(L)5T(L)6C7T(L)8G9C10):d( G11C12A13G14A15A16G17C 18A19G20). A total relaxation matrix approach was used to obtain interproton distance bounds from NOESY cross-peak intensities. These distance bounds were used as restraints in molecular dynamics (rMD) calculations. Forty final structures were generated for the duplex from A-form and B-form DNA starting structures. The root-mean-square deviation (RMSD) of the coordinates for the 40 structures of the complex was 0.6 A. The sugar puckerings are averaged values of a dynamic interchange between N- and S-type conformation except in case of the locked nucleotides that were found to be fixed in the C3'-endo conformation. Among the other nucleotides in the modified strand, the furanose ring of C7 and G9 is predominantly in the N-type conformation whereas that of G3 is in a mixed conformation. The furanose rings of the nucleotides in the unmodified complementary strand are almost exclusively in the S-type conformation. Due to these different conformations of the sugars in the two strands, there is a structural strain between the A-type modified strand and the B-type unmodified complementary strand. This strain is relaxed by decreasing the value of rise and compensating with tip, buckle, and propeller twist. The values of twist vary along the strand but for a majority of the base pairs a value even lower than that of A-DNA is observed. The average twist over the sequence is 32+/-1 degrees. On the basis of the structure, we conclude that the high stability of LNA:DNA duplexes is caused by a local change of the phosphate backbone geometry that favors a higher degree of stacking.     

Conformational transitions in RNA single uridine and adenosine bulge structures: a molecular dynamics free energy simulation study

Extra unmatched nucleotides (single base bulges) are common structural motifs in folded RNA molecules and can participate in RNA-ligand binding and RNA tertiary structure formation. Often these processes are associated with conformational transitions in the bulge region such as flipping out of the bulge base from an intrahelical stacked toward a looped out state. Knowledge of the flexibility of bulge structures and energetics of conformational transitions is an important prerequisite to better understand the function of this RNA motif. Molecular dynamics simulations were performed on single uridine and adenosine bulge nucleotides at the center of eight basepair RNA molecules and indicated larger flexibility of the bulge bases compared to basepaired regions. The umbrella sampling method was applied to study the bulge base looping out process and accompanying conformational and free energy changes. Looping out toward the major groove resulted in partial disruption of adjacent basepairs and was found to be less favorable compared to looping out toward the minor groove. For both uridine and adenosine bulges, a positive free energy change for full looping out was obtained which was approximately 1.5 kcal mol-1 higher in the case of the adenosine compared to the uridine bulge system. The simulations also indicated stable partially looped out states with the bulge bases located in the RNA minor groove and forming base triples with 5'-neighboring basepairs. In the case of the uridine bulge this state was more stable than the intrahelical stacked bulge structure. Induced looping out toward the minor groove involved crossing of an energy barrier of approximately 3.5 kcal mol-1 before reaching the base triple state. A continuum solvent analysis of intermediate bulge states indicated that electrostatic interactions stabilize looped out and base triple states, whereas van der Waals interactions and nonpolar contributions favor the stacked bulge conformation.     

Three-dimensional structures of bulge-containing DNA fragments.

The three-dimensional structure of a DNA tridecamer d(CGCAGAATTCGCG)2 containing bulged adenine bases was determined by single crystal X-ray diffraction methods, at 120 K, to 2.6 A resolution. The structure is a B-DNA type double helix with a single duplex in the asymmetric unit. One of the bulged adenine bases loops out from the double helix, while the other stacks in to it. This is in contrast to our preliminary finding, which indicated that both adenine bases were looped out. This revised model was confirmed by the use of a covalently bound heavy-atom derivative. The conformation of the looped-out bulge hardly disrupts base stacking interactions of the bases flanking it. This is achieved by the backbone making a "loop-the-loop" curve with the extra adenine flipping over with respect to the other nucleotides in the strand. The looped-out base intercalates into the stacked-in bulge site of a symmetrically related duplex. The looped-out and stacked-in bases form an A.A reversed Hoogsteen base-pair that stacks between the surrounding base-pairs, thus stabilizing both bulges. The double helix is frayed at one end with the two "melted" bases participating in intermolecular interactions. A related structure, of the same tridecamer, after soaking the crystals with proflavin, was determined to 3.2 A resolution. The main features of this B-DNA duplex are basically similar to the native tridecamer but differ in detail especially in the conformation of the bulged-out base. Accommodation of a large perturbation such as that described here with minimal disruption of the double helix shows both the flexibility and resiliency of the DNA molecule.     

Solution structure of [d(GCGTATACGC)]2.

The solution structure of the alternating pyrimidine-purine DNA duplex [d(GCGTATACGC)]2 has been determined using two-dimensional nuclear magnetic resonance techniques and distance geometry methods. Backbone distance constraints derived from experimental nuclear Overhauser enhancement and J-coupling torsion angle constraints were required to adequately define the conformation of the inter-residue backbone linkages and to avoid underwinding of the duplex. The distance geometry structures were further refined by back-calculation of the two-dimensional nuclear Overhauser enhancement spectra to correct spin-diffusion distance errors. Fifteen final structures for [d(GCGTATACGC)]2 were generated from the refined experimental distance bounds. These structures all exhibit fully wound B-form geometry with small penalty values (< 1.5 A) against the distance bounds and small pair-wise root-mean-square deviation values (typically 0.6 A to 1.5 A). The final structures exhibit positive base-pair inclination with respect to the helix axis, a marked alternation in rise and twist, and are shorter and wider than classical fiber B-form DNA. The purines were found to adopt a sugar pucker close to the C-2'-endo conformation while pyrimidine sugars exhibited significantly lower pseudorotation phase angles in the C-1'-exo to C-2'-endo range. The minor groove cross-strand steric clashes at pyrimidine-purine steps that would exist in pure B-DNA are attenuated by an increased rise at these steps (and an increased roll angle at TpA steps). Concomitantly the backbone torsion angles of the pyrimidine moieties have larger gamma values, larger epsilon values, and smaller zeta values than the purines. The structures generated by distance geometry methods were also compared with those obtained from restrained molecular dynamics with empirical force-field potentials. The results indicate that the nuclear magnetic resonance/distance geometry approach alone is capable of elucidating most of the salient structural features of double-stranded helical nucleic acids in solution without resorting to empirical energy potentials and without using any structural assumptions from crystallographic data.     

Crystal structure of the highly distorted chimeric decamer r(C)d(CGGCGCCG)r(G).spermine complex--spermine binding to phosphate only and minor groove tertiary base-pairing.

The crystal structure of the self-complementary chimeric decamer duplex r(C)d(CGGCGCCG)r(G), with RNA base pairs at both termini, has been solved at 1.9 A resolution by the molecular replacement method and refined to an R value of 0.145 for 2,314 reflections. The C3'-endo sugar puckers of the terminal riboses apparently drive the entire chimeric duplex into an A-DNA conformation, in contrast to the B-DNA conformation adopted by the all-deoxy decamer of the same sequence. Five symmetry related duplexes encapsulate a spermine molecule which interacts with ten phosphate groups, both directly and through water molecules to form multiple ionic and hydrogen bonding interactions. The spermine interaction severely bends the duplexes by 31 degrees into the major groove at the fourth base pair G(4).C(17), jolts it and slides the 'base plate' into the minor groove. This base pair, together with the adjacent base pair in the top half and the corresponding pseudo two-fold related base pairs in the bottom half, form four minor groove base-paired multiples with the terminal base pairs of two neighboring duplexes.     

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.     

The crystal structure of the dimerization initiation site of genomic HIV-1 RNA reveals an extended duplex with two adenine bulges

BACKGROUND: An important step in retroviral replication is dimerization of the genomic RNA prior to encapsidation. Dimerization is initiated by the formation of a transient 'kissing-loop complex' that is thought to be subsequently matured into an extended duplex by the nucleocapsid protein (NCp). Although chemical probing and nuclear magnetic resonance spectroscopy have provided insight into the structure of the kissing-loop structure, no structural information concerning the extended-duplex state is available so far. RESULTS: The structure of a minimal HIV-1 RNA dimerization initiation site has been solved at 2.3 A resolution in two different space groups. It reveals a 22 base pair extended duplex with two noncanonical Watson-Crick-like G-A mismatches, each adjacent to a bulged-out adenine. The structure shows significant asymmetry in deep groove width and G-A base-pair conformations. A network of eight magnesium cations was clearly identified, one being unusually chelated by the 3' phosphate of each bulge across an extremely narrowed deep major groove. CONCLUSIONS: These crystal structures represent the putative matured form of the initial kissing-loop complex. They show the ability of this self-complementary RNA hairpin loop to acquire a more stable extended duplex structure. Both bulged adenines form a striking 'base grip' that could be a recognition signal, either in cis for another viral RNA sequence, or in trans for a protein, possibly the NCp. Magnesium binding might be important to promote and stabilize the observed extrahelical conformation of these bulges.     

Recognition of bulged DNA by a neocarzinostatin product via an induced fit mechanism

The binding of the wedge-shaped isostructural analogue of the biradical species of the chromphore of antitumor antibiotic neocarzinostatin to sequence-specific bulged DNAs results in alterations in ellipticity of the DNAs. Circular dichroism (CD) spectroscopic results suggest that the drug specifically recognizes bulges of DNA via a combination of conformational selection and induced fit, not by binding to a preorganized site. Analysis of circular dichroism spectra indicates that the degree of induced fit observed is primarily a consequence of optimising van der Waals contacts with the walls of the bulge cavity. The effective recognition of the bulge site on duplex DNA appears to depend to a significant extent on the bent groove space being flexible enough to be able to adopt the geometrically optimal conformation compatible with the wedge-shaped drug molecule, rather than involving 'lock and key' recognition. The spectroscopic results indicate a change of DNA conformation, consistent with an allosteric binding model. Spectroscopic studies with various bulged DNAs also reveal that the binding strength directly correlates with the stability of the bulge structures.     

Proton nuclear magnetic resonance assignments and structural characterization of an intramolecular DNA triplex.

Two-dimensional 1H n.m.r. spectroscopy has been used to study the 31-base DNA oligonucleotide 5'-dAGAGAGAACCCCTTCTCTCTTTTTCTCTCTT-3', which folds to form a stable intramolecular triplex in solution at acidic pH. This structure is considerably more difficult to assign than short B-DNA duplexes and requires new assignment methods. The assignment strategy and assignments of almost all of the exchangeable and nonexchangeable resonances are presented. Seven base triplets and one Watson-Crick base-pair form the core of the structure and are connected by a four C and four T loop at either end. The second pyrimidine "strand" (bases 24 to 31) in this intramolecular pyrimidine-purine-pyrimidine triplex binds via Hoogsteen base-pairs in the major groove and is parallel to the purine "strand" (bases 1 to 8). Analysis of the sugar puckers reveals that, contrary to widely accepted belief, the triplex sugars are not predominantly in the N-type (close to C3'-endo) conformation. Except for some of the C nucleotides, all sugars are predominantly S-type (close to C2'-endo). Thus, the duplex DNA does not assume N-type sugar conformations to accommodate a third strand in the major groove. A preliminary model of the triplex structure is presented.     

Solution conformation of a bulged adenosine base in an RNA duplex by relaxation matrix refinement

Bulges are common structural motifs in RNA secondary structure and are thought to play important roles in RNA-protein and RNA-drug interactions. Adenosine bases are the most commonly occurring unpaired base in double helical RNA secondary structures. The solution conformation and dynamics of a 25-nucleotide RNA duplex containing an unpaired adenosine, r(GGCAGAGUGCCGC): r(GCGGCACCUGCC) have been studied by NMR spectroscopy and MORASS iterative relaxation matrix structural refinement. The results show that the bulged adenosine residue stacks into the RNA duplex with little perturbation around the bulged region. Most of the bases in the RNA duplex adopt C(3)'-endo conformation, exhibiting the N-type sugar pucker as found in the A form helices. The sugars of the bulged residue and the 5' flanking residue to it are found to exhibit C(2)'-endo conformation. None of the residues are in syn conformation.     

Crystal structure of a bulged RNA tetraplex at 1.1 a resolution: implications for a novel binding site in RNA tetraplex

Bulges are an important structural motif in RNA and can be used as recognition and interaction sites in RNA-protein interaction and RNA-RNA interaction. Here we report the first crystal structure of a bulged RNA tetraplex at 1.1 A resolution. The hexamer r(U)(BrdG)r(UGGU) forms a parallel tetraplex with the uridine sandwiched by guanines bulging out. The bulged uridine adopts the syn glycosidic conformation and its O2 and N3 atoms face outwards, serving as an effective recognition and interaction site. The bulge formation both widens the groove width and changes the groove hydrogen-bonding pattern on its 5' side. However, the bulge does not make any bends or kinks in the tetraplex structure. The present study demonstrates the dramatic difference between uridine and guanine in forming tetraplex structure. In addition, both G(syn) tetrad and G(anti) tetrad have been observed. They display the same base-pairing pattern and similar C1'-C1' distance but different hydrogen-bonding patterns in the groove.     

The conformations of locked nucleic acids (LNA)

We have used 2D NMR spectroscopy to study the sugar conformations of oligonucleotides containing a conformationally restricted nucleotide (LNA) with a 2'-O, 4'-C-methylene bridge. We have investigated a modified 9-mer single stranded oligonucleotide as well as three 9- and 10-mer modified oligonucleotides hybridized to unmodified DNA. The single-stranded LNA contained three modifications whereas the duplexes contained one, three and four modifications, respectively. The LNA:DNA duplexes have normal Watson-Crick base-pairing with all the nucleotides in anti-conformation. By use of selective DQF-COSY spectra we determined the ratio between the N-type (C3'-endo) and S-type (C2'-endo) sugar conformations of the nucleotides. In contrast to the corresponding single-stranded DNA (ssDNA), we found that the sugar conformations of the single-stranded LNA oligonucleotide (ssLNA) cannot be described by a major S-type conformer of all the nucleotides. The nucleotides flanking an LNA nucleotide have sugar conformations with a significant population of the N-type conformer. Similarly, the sugar conformations of the nucleotides in the LNA:DNA duplexes flanking a modification were also shown to have significant contributions from the N-type conformation. In all cases, the sugar conformations of the nucleotides in the complementary DNA strand in the duplex remain in the S-type conformation. We found that the locked conformation of the LNA nucleotides both in ssLNA and in the duplexes organize the phosphate backbone in such a way as to introduce higher population of the N-type conformation. These conformational changes are associated with an improved stacking of the nucleobases. Based on the results reported herein, we propose that the exceptional stability of the LNA modified duplexes is caused by a quenching of concerted local backbone motions (preorganization) by the LNA nucleotides in ssLNA so as to decrease the entropy loss on duplex formation combined with a more efficient stacking of the nucleobases.     

Investigation of potential RNA bulge stabilizing elements

As a part of our interest in recognition and cleavage of RNA we carried out thermal melting studies with the aim of screening a number of simple oligonucleotide modifications for their potential as modifying elements for RNA bulge stabilizing oligonucleotides. A specific model system from our studies on oligonucleotide-based artificial nuclease (OBAN) systems was chosen and the bulge size was varied from one to five nucleotides. Introduction of single 2'-modified nucleoside moieties (2'-O-methyl, 2'-deoxy and 2'-deoxy-2'-amino) with different conformational preferences adjacent to the bulge revealed that a higher preference for the north conformers gave more stable bulges across the whole range of bulge sizes. Changing a bulge closing a G-U wobble base pair to a G-C pair resulted in the interesting observation that, although the fully complementary complex and small bulges were highly stabilized, there was little difference in the stability of the larger bulges. The wobble base pair even gave a slight stabilization of the 5 nt bulge system. Introduction of a uridine C-5 linker with a single ammonium group was clearly bulge stabilizing (DeltaT(m) + 4.6 to + 5.4 degrees C for the three most stabilized bulges), although with limited selectivity for different bulge sizes since the fully complementary duplex was also stabilized. Introduction of a naphthoyl group on a 2'-aminolinker mostly gave a destabilizing effect, while introduction of a 5-aminoneocuproine moiety on the same linker resulted in stabilization of all bulges, in particular those with two or four unpaired nucleotides (DeltaT(m) + 3.6 and + 2.9 degrees C respectively). The aromatic groups destabilize the fully complementary duplex, resulting in higher selectivity towards stabilization of bulges. A combination of the studied partial element should be suitable for future designs of modified oligonucleotides that, apart from standard base pairing, can also provide additional non-Watson-Crick recognition of RNA.     

Effects of bulge composition and flanking sequence on the kinking of DNA by bulged bases

We recently showed that bulged bases kink duplex DNA, with the degree of kinking increasing in roughly equal increments as the number of bases in the bulge increases from one to four [Hsieh, C.-H., & Griffith, J.D. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 4833-4837]. Here we have examined the kinking of DNA by single A, C, G, or T bulges with different neighboring base pairs. Synthetic 30 base pair (bp) duplex DNAs containing 2 single-base bulges spaced by 10 bp were ligated head to tail, and their electrophoretic behavior in highly cross-linked gels was examined. All bulge-containing DNAs showed marked electrophoretic retardations as compared to non-bulge-containing DNA. Regardless of the sequence of the flanking base pairs, purine bulges produced greater retardations than pyrimidine bulges. Furthermore, C and T bulges produced the same retardations as did G and A bulges. Bulged DNA containing different flanking base pairs showed marked differences in electrophoretic mobility. For C-bulged DNA, the greatest retardations were observed with G.C neighbors, the least with T.A neighbors, and an intermediate amount with a mixture of neighboring base pairs. For A-bulged DNA, the retardations were greatest with G.C neighbors, less with T.A neighbors, even less with a mixture of neighboring base pairs, and finally least with C.G neighbors. Thus flanking base pairs affect C-bulged DNA and A-bulged DNA differently, and G.C and C.G flanking base pairs were seen to have very different effects. These results imply an important role of base stacking in determining how neighboring base pairs influence the kinking of DNA by a single-base bulge.