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5-hydroxyuracil can form stable base pairs with all four bases in a DNA duplex.

NMR studies, UV-monitored melting experiments, and ab initio calculations show that 5-hydroxyuracil, produced by the oxidative de-amination of cytosines by reactive oxygen species, can form stable base-pairs with dA, dG, dC and dT residues in a DNA duplex, providing a basis for the in-vivo incorporation of 5-hydroxyuracil during DNA replication.

Base Pairing↗

Thermodynamics of RNA duplexes with tandem mismatches containing a uracil-uracil pair flanked by C.G/G.C or G.C/A.U closing base pairs.

The thermodynamics governing the denaturation of RNA duplexes containing 8 bp and a central tandem mismatch or 10 bp were evaluated using UV absorbance melting curves. Each of the eight tandem mismatches that were examined had one U-U pair adjacent to another noncanonical base pair. They were examined in two different RNA duplex environments, one with the tandem mismatch closed by G.C base pairs and the other with G.C and A.U closing base pairs. The free energy increments (Delta Gdegrees(loop)) of the 2 x 2 loops were positive, and showed relatively small differences between the two closing base pair environments. Assuming temperature-independent enthalpy changes for the transitions, (Delta Gdegrees(loop)) for the 2 x 2 loops varied from 0.9 to 1.9 kcal/mol in 1 M Na(+) at 37 degrees C. Most values were within 0.8 kcal/mol of previously estimated values; however, a few sequences differed by 1.2-2.0 kcal/mol. Single strands employed to form the RNA duplexes exhibited small noncooperative absorbance increases with temperature or transitions indicative of partial self-complementary duplexes. One strand formed a partial self-complementary duplex that was more stable than the tandem mismatch duplexes it formed. Transitions of the RNA duplexes were analyzed using equations that included the coupled equilibrium of self-complementary duplex and non-self-complementary duplex denaturation. The average heat capacity change (DeltaC(p)) associated with the transitions of two RNA duplexes was estimated by plotting DeltaH degrees and DeltaS degrees evaluated at different strand concentrations as a function of T(m) and ln T(m), respectively. The average DeltaC(p) was 70 +/- 5 cal K(-)(1) (mol of base pairs)(-)(1). Consideration of this heat capacity change reduced the free energy of formation at 37 degrees C of the 10 bp control RNA duplexes by 0.3-0.6 kcal/mol, which may increase Delta Gdegrees(loop) values by similar amounts.

Base Pair Mismatch↗

Substituent effects on the pairing and polymerase recognition of simple unnatural base pairs.

As part of an effort to develop stable and replicable unnatural base pairs, we have evaluated a large number of unnatural nucleotides with predominantly hydrophobic nucleobases. Despite its limited aromatic surface area, a nucleobase analog scaffold that has emerged as being especially promising is the simple phenyl ring. Modifications of this scaffold with methyl and fluoro groups have been shown to impact base pair stability and polymerase recognition, suggesting that nucleobase shape, hydrophobicity and electrostatics are important. To further explore the impact of heteroatom substitution within this nucleobase scaffold, we report the synthesis, stability and polymerase recognition of nucleoside analogs bearing single bromo- or cyano-derivatized phenyl rings. Both modifications are found to generally stabilize base pair formation to a greater extent than methyl or fluoro substitution. Moreover, polymerase recognition of the unnatural base pairs is found to be very sensitive to both the position and nature of the heteroatom substituent. The results help identify the determinants of base pair stability and efficient replication and should contribute to the effort to develop stable and replicable unnatural base pairs.

Base Pair Mismatch↗

Base-pairing properties of O-methylated bases of nucleic acids. Energetic and steric considerations.

Base-pairing properties of O-methylated nucleic-acid bases have been systematically investigated using both semi-empirical quantum-mechanical methods and a second-order perturbation formalism. The energetic, steric and electronic properties of (a) the individual methylated bases, (b) possible base-pairs formed between O-methylated and normal bases, and (c) mini-helices incorporating O-methylated bases were calculated. Two types of base-paired complexes were obtained: Those involving classical linear hydrogen bonds, and those involving bifurcated hydrogen-donor-hydrogen-acceptor interactions. In most complexes the presence of mispairs in the helical structure of nucleic acids is expected to create a local perturbation in the structure of the helix. Even though the most stable planar configurations of the mispairs may deviate markedly from those in the regular double helix, the induced deformations in the structure of the backbone are relatively small. Internal energies and geometries of mispairs are strongly affected by the conformation of the exocyclic group of the methylated bases. Another important contribution to the stability of various base-pairing schemes comes from stacking interactions.

Allosteric Site↗

Molecular dynamics of the frame-shifting pseudoknot from beet western yellows virus: the role of non-Watson-Crick base-pairing, ordered hydration, cation binding and base mutations on stability and unfolding.

Molecular dynamics simulations of the frame-shifting pseudoknot from beet western yellows virus (BWYV, NDB file UR0004) were performed with explicit inclusion of solvent and counterions. In all, 33 ns of simulation were carried out, including 10 ns of the native structure with protonation of the crucial cytosine residue, C8(N3+). The native structure exhibited stable trajectories retaining all Watson-Crick and tertiary base-pairs, except for fluctuations or transient disruptions at specific sites. The most significant fluctuations involved the change or disruption of hydrogen-bonding between C8(N3+) and bases G12, A25, and C26, as well as disruption of the water bridges linking C8(N3+) with A25 and C26. To increase sampling of rare events, the native simulation was continued at 400 K. A partial, irreversible unfolding of the molecule was initiated by slippage of C8(N3+) relative to G12 and continued by sudden concerted changes in hydrogen-bonding involving A23, A24, and A25. These events were followed by a gradual loss of stacking interactions in loop 2. Of the Watson-Crick base-pairs, only the 5'-terminal pair of stem 1 dissociated at 400 K, while the trans sugar-edge/sugar-edge A20.G4 interaction remained surprisingly stable. Four additional room-temperature simulations were carried out to obtain insights into the structural and dynamic effects of selected mutations. In two of these, C8 was left unprotonated. Considerable local rearrangements occurred that were not observed in the crystal structure, thus confirming N3-protonation of C8 in the native molecule. We also investigated the effect of mutating C8(N3+) to U8, to correlate with experimental and phylogenetic studies, and of changing the G4 x C17 base-pair to A4 x U17 to weaken the trans sugar-edge interaction between positions 4 and 20 and to test models of unfolding. The simulations indicate that the C8 x G12 x C26 base-triple at the junction is the most labile region of the frame-shifting pseudoknot. They provide insights into the roles of the other non-Watson-Crick base-pairs in the early stages of unfolding of the pseudoknot, which must occur to allow readthrough of the message by the ribosome. The simulations revealed several critical, highly ordered hydration sites with close to 100 % occupancies and residency times of individual water molecules of up to 5 ns. Sodium cation coordination sites with occupancies above 50 % were also observed.

Base Pairing↗

How much pi-stacking do DNA termini seek? Solution structure of a self-complementary DNA hexamer with trimethoxystilbenes capping the terminal base pairs.

The exposed terminal base pairs of DNA duplexes are nonclassical binding sites for small molecules. Instead, small molecules usually prefer intercalation or minor groove binding. Here we report the solution structure of the DNA duplex (TMS-TGCGCA)(2), where TMS denotes trimethoxystilbene carboxamides that are 5'-tethered to the DNA. The stilbenes, for which intercalation is conformationally accessible, stack on the terminal T:A base pairs of an undisturbed B-form duplex. Two conformations, differing by the orientation of the stilbene relative to the terminal base pair, are observed, indicating that the flip rate is slow for the pi-stacked aromatic ring system. The trimethoxystilbene is known to greatly increase base pairing fidelity at the terminus. Here we show that it gauges the size of the T:A base pair by embracing the 2'-methylene group of the terminal dA residue of the unmodified terminus with its methoxy "arms", but that it does not engage the entire base pair in pi-stacking. Mismatched base pairs with their altered geometry will not allow for the same embracing interaction. On the basis of the current structure, a trimethoxychrysene carboxamide is proposed as a ligand with increased pi-stacking surface and possible applications as improved fidelity-enhancing element.

Base Pairing↗

An efficiently extended class of unnatural base pairs.

A third DNA base pair, which is synthesized efficiently and selectively, would have wide ranging applications from synthetic organisms to nucleic acids biotechnology. Hydrophobic unnatural nucleobases offer a promising route to such a pair, but are often limited by inefficient extension, defined as synthesis immediately following the unnatural pair. Here, we describe a simple screen which enables the characterization of large numbers of previously uncharacterized hetero base pairs. From this screen, we identified a class of unnatural base pairs which are extended more efficiently than any unnatural base pair reported to date. Screening, when complemented by further kinetic analysis, can improve the understanding of the determinants of efficient extension as well as identify viable hetero base pairs.

Base Pairing↗

The first example of a Hoogsteen base-paired DNA duplex in dynamic equilibrium with a Watson-Crick base-paired duplex--a structural (NMR), kinetic and thermodynamic study.

A single-point substitution of the O4' oxygen by a CH2 group at the sugar residue of A6 (i.e. 2'-deoxyaristeromycin moiety) in a self-complementary DNA duplex, 5'-d(C1G2C3G4A5A6T7T8C9G10C11G12)2(-3), has been shown to steer the fully Watson-Crick basepaired DNA duplex (1A), akin to the native counterpart, to a doubly A6:T7 Hoogsteen basepaired (1B) B-type DNA duplex, resulting in a dynamic equilibrium of (1A)<==>(1B): Keq = k1/k(-1) = 0.56+/-0.08. The dynamic conversion of the fully Watson-Crick basepaired (1A) to the partly Hoogsteen basepaired (1B) structure is marginally kinetically and thermodynamically disfavoured [k1 (298K) = 3.9 0.8 sec(-1); deltaHdegrees++ = 164+/-14 kJ/mol; -TdeltaS degrees++ (298K) = -92 kJ/mol giving a deltaG degrees++ 298 of 72 kJ/mol. Ea (k1) = 167 14 kJ/mol] compared to the reverse conversion of the Hoogsteen (1B) to the Watson-Crick (1A) structure [k-1 (298K) = 7.0 0.6 sec-1, deltaH degrees++ = 153 13 kJ/mol; -TdeltaSdegrees++ (298K) = -82 kJ/mol giving a deltaGdegrees++(298) of 71 kJ/mol. Ea (k-1) = 155 13 kJ/mol]. Acomparison of deltaGdegrees++(298) of the forward (k1) and backward (k-1) conversions, (1A)<==>(1B), shows that there is ca 1 kJ/mol preference for the Watson-Crick (1A) over the double Hoogsteen basepaired (1B) DNA duplex, thus giving an equilibrium ratio of almost 2:1 in favour of the fully Watson-Crick basepaired duplex. The chemical environments of the two interconverting DNA duplexes are very different as evident from their widely separated sets of chemical shifts connected by temperature-dependent exchange peaks in the NOESY and ROESY spectra. The fully Watson-Crick basepaired structure (1A) is based on a total of 127 intra, 97 inter and 17 cross-strand distance constraints per strand, whereas the double A6:T7 Hoogsteen basepaired (1B) structure is based on 114 intra, 92 inter and 15 cross-strand distance constraints, giving an average of 22 and 20 NOE distance constraints per residue and strand, respectively. In addition, 55 NMR-derived backbone dihedral constraints per strand were used for both structures. The main effect of the Hoogsteen basepairs in (1B) on the overall structure is a narrowing of the minor groove and a corresponding widening of the major groove. The Hoogsteen basepairing at the central A6:T7 basepairs in (1B) has enforced a syn conformation on the glycosyl torsion of the 2'-deoxyaristeromycin moiety, A6, as a result of substitution of the endocyclic 4'-oxygen in the natural sugar with a methylene group in A6. A comparison of the Watson-Crick basepaired duplex (1A) to the Hoogsteen basepaired duplex (1B) shows that only a few changes, mainly in alpha, sigma and gamma torsions, in the sugar-phosphate backbone seem to be necessary to accommodate the Hoogsteen basepair.

Base Pairing↗

Structural modification of DNA by a DNA-binding motif SPKK: detection of changes in base-pair hydrogen bonding and base stacking by UV resonance Raman spectroscopy.

Interactions of a DNA-binding motif SPKK with polynucleotides have been investigated by uv resonance Raman spectroscopy. Analysis of the Raman spectra has shown that the tetrapeptide SPKK weakens the adenine-thymine base-pair hydrogen bonding in poly(dA-dT).poly(dA-dT) and reduces the adenine-adenine base stacking interactions in poly(dA).poly(dT), both effects being indicative of destabilization of the DNA double helical structure. On the other hand, poly(dG-dC).poly(dG-dC) and poly(dG).poly(dC) do not show any structural change in the presence of SPKK. The present observations confirm that the SPKK motif, which is frequently found in histone H1 proteins, specifically binds to A/T-rich regions of DNA and loosens the DNA double-helical structure. One of the roles of the SPKK motifs in histones may be to increase DNA flexibility so that DNA can wrap around core histones and be assembled into chromosomes more easily.

Amino Acid Sequence↗

Ionized and wobble base-pairing for bromouracil-guanine in equilibrium under physiological conditions. A nuclear magnetic resonance study on an oligonucleotide containing a bromouracil-guanine base-pair as a function of pH.

A one and two-dimensional nuclear magnetic resonance study of a non-selfcomplementary oligonucleotide containing a central 5-bromouracil-guanine pair is reported. For these two bases three types of hydrogen bonding schemes could exist; wobble, rare tautomer and ionized. The two-dimensional spectra of non-exchangeable protons together with one-dimensional spectra recorded in water show that at pH 7.0 the predominant species is a right-handed B-form DNA in which the brU.G pair has wobble geometry. On raising the pH we observe a transition monitored by proton chemical shift changes for the brU.G and adjacent base-pairs. The mid-point of the transition was observed at pH 8.6. Spectra recorded at pH 9.8 show that the helix remains intact with B form conformation. It is shown that this high pH form has an ionized brU.G base-pair now in Watson-Crick geometry. Thus under physiological conditions an equilibrium exists between wobble and ionized structures.

Base Composition↗

Nature of base stacking: reference quantum-chemical stacking energies in ten unique B-DNA base-pair steps.

Base-stacking energies in ten unique B-DNA base-pair steps and some other arrangements were evaluated by the second-order Møller-Plesset (MP2) method, complete basis set (CBS) extrapolation, and correction for triple (T) electron-correlation contributions. The CBS(T) calculations were compared with decade-old MP2/6-31G*(0.25) reference data and AMBER force field. The new calculations show modest increases in stacking stabilization compared to the MP2/6-31G*(0.25) data and surprisingly large sequence-dependent variation of stacking energies. The absolute force-field values are in better agreement with the new reference data, while relative discrepancies between quantum-chemical (QM) and force-field values increase modestly. Nevertheless, the force field provides good qualitative description of stacking, and there is no need to introduce additional pair-additive electrostatic terms, such as distributed multipoles or out-of-plane charges. There is a rather surprising difference of about 0.1 A between the vertical separation of base pairs predicted by quantum chemistry and derived from crystal structures. Evaluations of different local arrangements of the 5'-CG-3' step indicate a sensitivity of the relative stacking energies to the level of calculation. Thus, describing quantitative relations between local DNA geometrical variations and stacking may be more complicated than usually assumed. The reference calculations are complemented by continuum-solvent assessment of solvent-screening effects.

Base Pairing↗

Crystal structure of a 14 bp RNA duplex with non-symmetrical tandem GxU wobble base pairs.

Adjacent GxU wobble base pairs are frequently found in rRNA. Atomic structures of small RNA motifs help to provide a better understanding of the effects of various tandem mismatches on duplex structure and stability, thereby providing better rules for RNA structure prediction and validation. The crystal structure of an RNA duplex containing the sequence r(GGUAUUGC-GGUACC)2 has been solved at 2.1 A resolution using experimental phases. Novel refinement strategies were needed for building the correct solvent model. At present, this is the only short RNA duplex structure containing 5'-U-U-3'/3'-G-G-5' non-symmetric tandem GxU wobble base pairs. In the 14mer duplex, the six central base pairs are all displaced away from the helix axis, yielding significant changes in local backbone conformation, helix parameters and charge distribution that may provide specific recognition sites for biologically relevant ligand binding. The greatest deviations from A-form helix occur where the guanine of a wobble base pair stacks over a purine from the opposite strand. In this vicinity, the intra-strand phosphate distances increase significantly, and the major groove width increases up to 3 A. Structural comparisons with other short duplexes containing symmetrical tandem GxU or GxT wobble base pairs show that nearest-neighbor sequence dependencies govern helical twist and the occurrence of cross-strand purine stacks.

Base Pairing↗

OR3 operator of bacteriophage lambda in a 23 base-pair DNA fragment: sequence-specific 1H NMR assignments for the non-labile protons and comparison with the isolated 17 base-pair operator.

Sequence-specific 1H NMR assignments are presented for a non-selfcomplementary 23-base-pair DNA duplex of molecular weight 15,000 daltons, containing the OR3 repressor binding site of bacteriophage lambda as the central core. The NMR techniques used were mainly phase-sensitive two-dimensional NOE and 2Q spectroscopy, the latter to overcome overlap problems within the spectral region of the deoxyribose spin-systems. Direct sequential NOE connectivities are observed between adenine 2 H and deoxyribose 1' protons. We propose the use of these connectivities as a check of the assignments of C1' and A2 protons, which have independently been derived via other assignment pathways.

Bacteriophage lambda↗

SPR fingerprinting of mismatched base pair.

Discrimination of mismatched base pairs having various flanking sequence from normal Watson-Crick base pairs were examined using SPR sensor surface where mismatch binding ligand (MBL) were immobilized. CC, CT, and TT mismatched base pair are distinguishable from wild type DNA by means of diaminonaphthyndine dimer (damND) immobilized sensor surface. By comparing the component ratio of responses obtained by MLB immobilized sensors, distinct differences could be observed between mismatched base pairs having almost the same total SPR response.

Base Pair Mismatch↗

Structural studies of DNA and RNA containing AG base pairs by NMR.

Base pairing between A and G residues has been suggested in some ribozymes and the structure derived from this non-standard base pairing could play a crucial role in enzymatic actions of the ribozymes. We have studied the structures of three DNAs and an RNA that base sequences were modeled after the ribozymes by NMR. It was found that the A and G residues can form a basepair in a very unique fashion both in the DNAs and RNA. "Side" instead of "head to head" alignment of the two bases was found, where an amino proton instead of an imino proton of the G residue is involved in the hydrogen bonding. As a result of the unique basepairing, certain bases stack over the bases of the opposite strand instead of over the ones of the same strand. It was also shown that the formation and thermal stability of this unique AG basepair depend on the neighbouring base sequences. Moreover existence of the unique AG basepairs was suggested in a real small metalloribozyme itself.

Adenine↗

High-resolution NMR studies of chimeric DNA-RNA-DNA duplexes, heteronomous base pairing, and continuous base stacking at junctions.

Two symmetrical DNA-RNA-DNA duplex chimeras, d(CGCG)r(AAUU)d(CGCG) (designated rAAUU) and d(CGCG)r(UAUA)d(CGCG) (designated rUAUA), and a nonsymmetrical chimeric duplex, d(CGTT)r(AUAA)d(TGCG)/d(CGCA)r(UUAU)d(A ACG) (designated rAUAA), as well as their pure DNA analogues, containing dU instead of T, have been synthesized by solid-phase phosphoramidite methods and studied by high-resolution NMR techniques. The 1D imino proton NOE spectra of these d-r-d chimeras indicate normal Watson-Crick hydrogen bonding and base stacking at the junction region. Preliminary qualitative NOESY, COSY, and chemical shift data suggest that the internal RNA segment contains C3'-endo (A-type) sugar conformations except for the first RNA residues (position 5 and 17) following the 3' end of the DNA block, which, unlike the other six ribonucleotides, exhibit detectable H1'-H2' J coupling. The nucleosides of the two flanking DNA segments appear to adopt a fairly normal C2'-endo B-DNA conformation except at the junction with the RNA blocks (residues 4 and 16), where the last DNA residue appears to adopt an intermediate sugar conformation. The DNA-RNA junction residues exhibit quite different COSY, chemical shift, and NOE behavior, but these effects do not appear to propagate into the DNA or RNA segments. The circular dichroism spectra of these d-r-d chimeras also display a mixture of characteristic A-type and B-type absorption bands. The data indicate that A-type and B-type conformations can coexist in a single short continuous nucleic acid duplex, but our results differ somewhat from previous theoretical model studies.

Base Sequence↗

Imidazole-imidazole pair as a minor groove recognition motif for T:G mismatched base pairs.

The T:G mismatched base pair is associated with many genetic mutations. Understanding its biological consequences may be aided by studying the structural perturbation of DNA caused by a T:G base pair and by specific probing of the mismatch using small molecular ligands. We have shown previously that AR-1-144, a tri-imidazole (Im-Im-Im) minor groove binder, recognizes the sequence CCGG. NMR structural analysis of the symmetric 2:1 complex of AR-1-144 and GAACCGGTTC revealed that each AR-1-144 binds to four base pairs with the guanine N2 amino group forming a bifurcated hydrogen bond to a side-by-side Im/Im pair. We predicted that the free G-N2 amino group in a T:G wobble base pair can form two individual hydrogen bonds to a side-by-side Im/Im pair. Thus an Im/Im pair may be a good recognition motif for a T:G base pair in DNA. Cooperative and tight binding of an AR-1-144 homodimer to GAACTGGTTC permits a detailed structural analysis by 2D NOE NMR refinement and the refined structure confirms our prediction. Surprisingly, AR-1-144 does not bind to GAATCGGTTC. We further show that both the Im-Im-Im/Im-Py-Im heterodimer and the Im-Im-Im/Im-Im-Im homodimer bind strongly to the CACGGGTC + GACTCGTG duplex. These results together suggest that an Im/Im pair can specifically recognize a single T:G mismatch. Our results may be useful in future design of molecules (e.g. linked dimers) that can recognize a single T:G mismatch with specificity.

Base Pair Mismatch↗