N1...N3 hydrogen bonds of A:U base pairs of RNA are stronger than those of A:T base pairs of DNA

Trans-hydrogen-bond deuterium isotope effects of Watson-Crick A:U and A:T base pairs of 10 homologous RNA and DNA duplexes are compared. The isotope effect at 13C2 of adenosine residues due to deuterium/protium substitution at the imino H3 site, 2hDelta13C2, is larger in RNA than in DNA. The virtually consistent larger isotope effects in RNA suggest that the N1...N3 hydrogen bonds of A:U base pairs of RNA are stronger than those of the A:T base pairs of DNA.     

The recognition of a noncanonical RNA base pair by a zinc finger protein.

BACKGROUND: The zinc finger (ZF) is the most abundant nucleic-acid-interacting protein motif. Although the interaction of ZFs with DNA is reasonably well understood, little is known about the RNA-binding mechanism. We investigated RNA binding to ZFs using the Zif268-DNA complex as a model system. Zif268 contains three DNA-binding ZFs; each independently binds a 3 base pair (bp) subsite within a 9 bp recognition sequence. RESULTS: We constructed a library of phage-displayed ZFs by randomizing the alpha helix of the Zif268 central finger. Successful selection of an RNA binder required a noncanonical base pair in the middle of the RNA triplet. Binding of the Zif268 variant to an RNA duplex containing a G.A mismatch (rG.A) is specific for RNA and is dependent on the conformation of the mismatched middle base pair. Modeling and NMR analyses revealed that the rG.A pair adopts a head-to-head configuration that counterbalances the effect of S-puckered riboses in the backbone. We propose that the structure of the rG.A duplex is similar to the DNA in the original Zif268-DNA complex. CONCLUSIONS: It is possible to change the specificity of a ZF from DNA to RNA. The ZF motif can use similar mechanisms in binding both types of nucleic acids. Our strategy allowed us to rationalize the interactions that are possible between a ZF and its RNA substrate. This same strategy can be used to assess the binding specificity of ZFs or other protein motifs for noncanconical RNA base pairs, and should permit the design of proteins that bind specific RNA structures.     

High‐Resolution Crystal Structure of a Silver(I)–RNA Hybrid Duplex Containing Watson–Crick‐like C?Silver(I)?C Metallo‐Base Pairs

Metallo‐base pairs have been extensively studied for applications in nucleic acid‐based nanodevices and genetic code expansion. Metallo‐base pairs composed of natural nucleobases are attractive because nanodevices containing natural metallo‐base pairs can be easily prepared from commercially available sources. Previously, we have reported a crystal structure of a DNA duplex containing T Hg^II T base pairs. Herein, we have determined a high‐resolution crystal structure of the second natural metallo‐base pair between pyrimidine bases C Ag^I C formed in an RNA duplex. One Ag^I occupies the center between two cytosines and forms a C Ag^I C base pair through N3 Ag^I N3 linear coordination. The C Ag^I C base pair formation does not disturb the standard A‐form conformation of RNA. Since the C Ag^I C base pair is structurally similar to the canonical Watson–Crick base pairs, it can be a useful building block for structure‐based design and fabrication of nucleic acid‐based nanodevices.     

High‐Resolution Crystal Structure of a Silver(I)–RNA Hybrid Duplex Containing Watson–Crick‐like CSilver(I)C Metallo‐Base Pairs

Metallo‐base pairs have been extensively studied for applications in nucleic acid‐based nanodevices and genetic code expansion. Metallo‐base pairs composed of natural nucleobases are attractive because nanodevices containing natural metallo‐base pairs can be easily prepared from commercially available sources. Previously, we have reported a crystal structure of a DNA duplex containing T? Hg^II? T base pairs. Herein, we have determined a high‐resolution crystal structure of the second natural metallo‐base pair between pyrimidine bases C? Ag^I? C formed in an RNA duplex. One Ag^I occupies the center between two cytosines and forms a C? Ag^I? C base pair through N3? Ag^I? N3 linear coordination. The C? Ag^I? C base pair formation does not disturb the standard A‐form conformation of RNA. Since the C? Ag^I? C base pair is structurally similar to the canonical Watson–Crick base pairs, it can be a useful building block for structure‐based design and fabrication of nucleic acid‐based nanodevices.     

Preopening of the DNA base pairs

The lower‐energy stable structures of the A?T base pair are revealed under a search of its potential energy surface in the vicinity of its Watson–Crick configuration performed at the PM3 computational level. Their properties and the mutual position of the nucleic acid bases A and T in these structures allow to partition them into three classes: partially preopened, stretched, and fully preopened. The preferable monohydration sites of the preopened, stretched, and fully preopened pairs are also determined. It is demonstrated, first, that the monohydration of the A?T pair at particular sites favors a base pair preopeness and, second, that a binding of the water molecule to the preopened A?T base pair on the major groove side enhances its stabilization. It is also shown that water molecule placing in the vicinity of the central H bond of the A?T pair significantly facilitates its preopening. © 2001 John Wiley & Sons, Inc. Int J Quant Chem 82: 193–204, 2001     

Biocomplementary interaction behavior in DNA‐like and RNA‐like polymers

A series of nucleobased polymers and copolymers were synthesized through atom transfer radical polymerization (ATRP). Biocomplementary DNA‐ and RNA‐like supramolecular complexes are formed in dilute DMSO solution through nucleobase recognition. ¹H NMR titration studies of these complexes in CDCl₃ indicated that thymine‐adenine (T‐A) and uracil‐adenine (U‐A) complexes form rapidly on the NMR time scale with high association constants (up to 534 and 671 M^–1, respectively) and result in significant T_g increase. WAXD and differential scanning calorimetry analyzes in the bulk state indicate the presence of highly physical cross‐linked structures and provide further details into the nature of the self‐assembly of these systems. Furthermore, this study is of discussion on the difference in the hydrogen bond strength between T‐A and U‐A base pairs within polymer systems, indicating that the strength of hydrogen bonds in RNA U‐A pairs is stronger than that in DNA T‐A base pairs. © 2009 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 47: 6388–6395, 2009     

The structure of a mixed LNA/DNA:RNA duplex is driven by conformational coupling between LNA and deoxyribose residues as determined from 13C relaxation measurements

A study of the internal dynamics of an LNA/DNA:RNA duplex has been performed to further characterize the conformational changes associated with the incorporation of locked nucleic acid (LNA) nucleotides in a DNA:RNA duplex. In general, it was demonstrated that the LNA/DNA:RNA duplex has a very high degree of order compared to dsDNA and dsRNA duplexes. The order parameters of the aromatic carbon atoms in the LNA/DNA strand are uniformly high, whereas a sharp drop in the degree of order was seen in the RNA strand in the beginning of the AUAU stretch in the middle of the strand. This can be related to a return to normal dsRNA dynamics for the central A:U base pair. The high order of the heteroduplex is consistent with preorganization of the chimera strand for an A-form duplex conformation. These results partly explain the dramatic increase in T(m) of the chimeric heteroduplex over dsDNA and DNA:RNA hybrids of the same sequence.     

Leading RNA tertiary interactions: structures, energies, and water insertion of A-minor and P-interactions. A quantum chemical view

Complex molecular shapes of ribosomal RNA molecules are stabilized by recurrent types of tertiary interactions involving highly specific and conserved non-Watson-Crick base pairs, triplets, and quartets. We analyzed the intrinsic structure and stability of the P-motif and the four basic types of A-minor interactions (types I, II, III, and 0), which represent the most prominent RNA tertiary interaction patterns refined in the course of evolution. In the studied interactions, the electron correlation component of the stabilization usually exceeds the Hartree-Fock (HF) term, leading to a strikingly different balance of forces as compared to standard base pairing stabilized primarily by the HF term. In other words, the A-minor and P-interactions are considerably more influenced by the dispersion energy as compared to canonical base pairs, which makes them particularly suitable to zip the folded RNA structures that are substantially hydrated even in their interior. Continuum solvent COSMO calculations confirm that the stability of the canonical GC base pair is affected (reduced) by the continuum solvent screening considerably more than the stability of the A-minor interaction. Among the studied systems, the strong A-minor II and weak A-minor III interactions require water molecules to stabilize the experimental geometry. Gas-phase optimization of the canonical A-minor II A/CG triplet without water results in a geometry that is clearly inconsistent with the RNA structure. The gas-phase structure of the P-interaction and the most stable A-minor I interaction nicely agrees with the geometries occurring in the ribosome. A-minor I can also adopt an alternative water-mediated substate rather often observed in X-ray and molecular dynamics studies. The A-minor I water bridge, however, does not appear to stabilize the tertiary contact, and its role is to provide structural flexibility to this binding pattern within the context of the RNA structure. Interestingly, the insertion of a polar water molecule in the A-minor I A/CG tertiary contact occurring in the A/C tertiary pair is stabilized primarily by the HF (electrostatic) interaction energy, while the dispersion-controlled A/G contact remains firmly bound. Thus, the intrinsic balance of forces as revealed by quantum mechanics (QM) calculations nicely correlates with many behavioral aspects of the studied interactions inside RNA. The comparison of interaction energies computed using quantum chemistry and an AMBER force field reveals that common molecular mechanics calculations perform rather well, except that the strength of the P-interaction is modestly overestimated. We also briefly discuss the non-negligible methodological differences when evaluating simple base-base nucleic acids base pairs and the complex RNA tertiary base pairing patterns using QM procedures.     

Understanding hydrogenation of the adenine‐thymine base pairs and their anions: A density functional study

The B3LYP/DZP++ approach has been used to investigate the properties of hydrogenated radicals and anions of adenine‐thymine (A‐T) base pairs. Our calculations show that the hydrogenated radicals and anions have relatively high stabilities compared with the single adenine and thymine base. The conformations and hydrogen‐bond interactions of A‐T base pairs have obviously changed once the hydrogen atoms attached to the A‐T base pairs and their anion. As for the hydrogenated A‐T radicals, all of them exhibit relatively high electron affinities and different hydrogenation properties with respect to their components. The process of the bond formations of (C6)‐H (adenine) and (C6)‐H (thymine) are the most favorable in energetics. The two hydrogenation channels have the reaction Gibbs free energies (ΔG°) of ?51.8 and ?54.2 kcal mol^?1, respectively. Also, the calculations on the basis of CPCM model imply that the solvent effect plays an important role in the electron attachment and hydrogenation reactions, and can stabilize the hydrogenated A‐T anions. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2012     

1JNH values show that N1...N3 hydrogen bonds are stronger in dsRNA A:U than dsDNA A:T base pairs

Here, we show that 1JNH values are on average 0.4 Hz less negative for double-stranded RNA A:U than for DNA A:T base pairs, which, according to existing theory, suggests that RNA N1...N3 hydrogen bond distances are about 0.02 A shorter than those of DNA. Also, there is a statistically relevant trend between 1JNH and 2hDelta13C2 values, which supports the original hypothesis that 2hDelta13C2 values are also sensitive to hydrogen bond distances. Finally, a context dependence is observed for these values, which suggests that hydrogen-bonding and base-stacking interactions are coupled.     

7‐Iodo‐5‐aza‐7‐deazaguanine ribonucleoside: crystal structure,physical properties,base‐pair stability and functionalization

The positional change of nitrogen‐7 of the RNA constituent guanosine to the bridgehead position‐5 leads to the base‐modified nucleoside 5‐aza‐7‐deazaguanosine. Contrary to guanosine, this molecule cannot form Hoogsteen base pairs and the Watson–Crick proton donor site N3—H becomes a proton‐acceptor site. This causes changes in nucleobase recognition in nucleic acids and has been used to construct stable `all‐purine' DNA and DNA with silver‐mediated base pairs. The present work reports the single‐crystal X‐ray structure of 7‐iodo‐5‐aza‐7‐deazaguanosine, C<sub>10</sub>H<sub>12</sub>IN<sub>5</sub>O<sub>5</sub> ( 1 ). The iodinated nucleoside shows an anti conformation at the glycosylic bond and an N conformation (O4′‐endo) for the ribose moiety, with an antiperiplanar orientation of the 5′‐hydroxy group. Crystal packing is controlled by interactions between nucleobase and sugar moieties. The 7‐iodo substituent forms a contact to oxygen‐2′ of the ribose moiety. Self‐pairing of the nucleobases does not take place. A Hirshfeld surface analysis of 1 highlights the contacts of the nucleobase and sugar moiety (O—H…O and N—H…O). The concept of pK‐value differences to evaluate base‐pair stability was applied to purine–purine base pairing and stable base pairs were predicted for the construction of `all‐purine' RNA. Furthermore, the 7‐iodo substituent of 1 was functionalized with benzofuran to detect motional constraints by fluorescence spectroscopy.     

Extended Peptide Nucleic Acid Nucleobases Based on Isoorotic Acid for the Recognition of A–U Base Pairs in Double-Stranded RNA

Peptide nucleic acids (PNA) with extended isoorotamide containing nucleobases ( I _o ) were designed for binding A–U base pairs in double-stranded RNA. Isothermal titration calorimetry and UV thermal melting experiments revealed improved affinity for A–U using the Io scaffold in PNA. PNAs having four sequential Io extended nucleobases maintained high binding affinity.     

A DFT study of the interresidue dependencies of scalar J-coupling and magnetic shielding in the hydrogen-bonding regions of a DNA triplex.

Scalar coupling constants and magnetic shieldings in the imino hydrogen-bonding region of Hoogsteen-Watson-Crick T.A-T and C(+).G-C triplets have been calculated as a function of the distance between proton donor and acceptor nitrogen atoms. The Fermi contact contributions to (h2)J((15)N-H...(15)N), (1)J((15)N-(1)H), and (h1)J((1)H...(15)N) were computed using density functional theory/finite perturbation theory (DFT/FPT) methods for the full base triplets at the unrestricted B3PW91/6-311G level. Chemical shifts delta((1)H) and delta((15)N) were obtained at the same level using the gauge including atomic orbital (GIAO) method for magnetic shielding. All three scalar couplings and all three chemical shifts are strongly interrelated and exhibit monotonic changes with base pair separation. These correlations are in conformity with experimental data for a 32-nucleotide DNA triplex. The results suggest that both chemical shifts and coupling constants can be used to gain information on H-bond donor-acceptor distances in nucleic acids. In addition to the DFT/FPT calculations, a simple three-orbital model of the N-H...H bond and a sum-over-states analysis is presented. This model reproduces the basic features of the H-bond coupling effect. In accordance with this model and the DFT calculations, a positive sign for the (h2)J(NN) coupling is determined from an E.COSY experiment.     

Caffeine interactions with nucleic acids. Molecular mechanics calculations of model systems for explanation of mechanisms of biological actions

To understand the molecular mechanisms of the influence of caffeine (CAF) on DNA functioning, molecular mechanics calculations of the interaction energy of CAF with nucleic acid bases and base pairs have been performed. The calculations reveal three types of mutual CAF–base (and CAF–base pair) arrangements corresponding to minima of the interaction energy. Besides well-known stacking mutual positions of the molecules, two other types of arrangements are revealed and studied. One of these arrangements corresponds to the nearly in-plane position of CAF and base (or base pair) and the formation of a single hydrogen bond. Another type of minimum corresponds to nearly perpendicular arrangements of the molecular planes and the formation of intermolecular hydrogen bonds. These two arrangements are possible both for individual nucleic acid monomers and for DNA duplexes. The calculations suggest the molecular mechanisms of the influence of CAF on DNA interactions with other biologically active molecules.From the Proceedings of the 28th Congreso de Químicos Teóricos de Expresión Latina (QUITEL 20002).     

Hydrogen bonds of RNA are stronger than those of DNA, but NMR monitors only presence of methyl substituent in uracil/thymine

Recently, Vakonakis and LiWang (J. Am. Chem. Soc. 2004, 126, 5688) reported experimental evidence for stronger hydrogen bonds in RNA A:U than in DNA A:T base pairs, which was based on differences in NMR shielding for adenine C2. We have analyzed the proposed correlation between NMR shielding and hydrogen-bond strength using density functional theory. Although we agree with the conclusion that A:U is more strongly bound, we find no correlation between the hydrogen-bond strength and the NMR shielding of C2. Our study shows that NMR merely probes the presence/absence of the methyl group in thymine/uracil, without any relation to the strength of the hydrogen bonds involved. In other words, one cannot infer the Watson-Crick hydrogen-bond strength from the NMR shielding constant of adenine C2.     

A Novel DNA Helical Wire Containing HgII‐Mediated T:T and T:G Pairs

Numerous applications of metal‐mediated base pairs (metallo‐base‐pairs) to nucleic acid based nanodevices and genetic code expansion have been extensively studied. Many of these metallo‐base‐pairs are formed in DNA and RNA duplexes containing Watson–Crick base pairs. Recently, a crystal structure of a metal–DNA nanowire with an uninterrupted one‐dimensional silver array was reported. We now report the crystal structure of a novel DNA helical wire containing Hg^II‐mediated T:T and T:G base pairs and water‐mediated C:C base pairs. The Hg‐DNA wire does not contain any Watson–Crick base pairs. Crystals of the Hg‐DNA wire, which is the first DNA wire structure driven by Hg^II ions, were obtained by mixing the short oligonucleotide d(TTTGC) and Hg^II ions. This study demonstrates the potential of metallo‐DNA to form various structural components that can be used for functional nanodevices.     

The crystal structure of the CeNA:RNA hybrid ce(GCGTAGCG):r(CGCUACGC)

Cyclohexenyl nucleic acids (CeNA) are characterised by the carbon–carbon double bond replacing the O4′‐oxygen atom of the natural D ‐2′‐deoxyribose sugar ring in DNA. CeNAs exhibit a high conformational flexibility, are stable against nuclease activity and their hybridisation is RNA selective. Additionally, CeNA has been shown to induce an enhanced biological activity when incorporated in siRNA. This makes CeNA a good candidate for siRNA and synthetic aptamer applications. The crystal structure of the synthetic CeNA:RNA hybrid ce(GCGTAGCG):r(CGCUACGC) has been solved with a resolution of 2.50 Å. The CeNA:RNA duplex adopts an anti‐parallel, right‐handed double helix with standard Watson–Crick base pairing. Analyses of the helical parameters revealed the octamer to form an A‐like double helix. The cyclohexenyl rings mainly adopt the ³H₂ conformation, which resembles the C3′‐endo conformation of RNA ribose ring. This C3′‐endo ring puckering was found in most of the RNA residues and is typical for A‐family helices. The crystal structure is stabilised by the presence of hexahydrated magnesium ions. The fact that the CeNA:RNA hybrid adopts an A‐type double helical conformation confirms the high potential of CeNAs for the construction of efficient siRNAs which can be used for therapeutical applications.     

A novel RNA motif based on the structure of unusually stable 2',5'-linked r(UUCG) loops

We have recently shown that hairpins containing 2',5'-linked RNA loops exhibit superior thermodynamic stability compared to native hairpins comprised of 3',5'-RNA loops [Hannoush, R. N.; Damha, M. J. J. Am. Chem. Soc. 2001, 123, 12368-12374]. A remarkable feature of the 2',5'-r(UUCG) tetraloop is that, unlike the corresponding 3',5'-linked tetraloop, its stability is virtually independent of the hairpin stem composition. Here, we determine the solution structure of unusually stable hairpins of the sequence 5'-G(1)G(2)A(3)C(4)-(U(5)U(6)C(7)G(8))-G(9)(U/T(10))C(11)C(12)-3' containing a 2',5'-linked RNA (UUCG) loop and either an RNA or a DNA stem. The 2',5'-linked RNA loop adopts a new fold that is completely different from that previously observed for the native 3',5'-linked RNA loop. The 2',5'-RNA loop is stabilized by (a). U5.G8 wobble base pairing, with both nucleotide residues in the anti-conformation, (b). extensive base stacking, and (c). sugar-base and sugar-sugar contacts, all of which contribute to the extra stability of this hairpin structure. The U5:G8 base pair stacks on top of the C4:G9 loop-closing base pair and thus appears as a continuation of the stem. The loop uracil U6 base stacks above U5 base, while the cytosine C7 base protrudes out into the solvent and does not participate in any of the stabilizing interactions. The different sugar pucker and intrinsic bonding interactions within the 2',5'-linked ribonucleotides help explain the unusual stability and conformational properties displayed by 2',5'-RNA tetraloops. These findings are relevant for the design of more effective RNA-based aptamers, ribozymes, and antisense agents and identify the 2',5'-RNA loop as a novel structural motif.     

Structural studies of LNA:RNA duplexes by NMR: conformations and implications for RNase H activity

We have used NMR and CD spectroscopy to study the conformations of modified oligonucleotides (locked nucleic acid, LNA) containing a conformationally restricted nucleotide (T(L)) with a 2'-O,4'-C-methylene bridge. We have investigated two LNA:RNA duplexes, d(CTGAT(L)ATGC):r(GCAUAUCAG) and d(CT(L)GAT(L)AT(L)GC):r(GCAUAUCAG), along with the unmodified DNA:RNA reference duplex. Increases in the melting temperatures of +9.6 degrees C and +8.1 degrees C per modification relative to the unmodified duplex were observed for these two LNA:RNA sequences. The three duplexes all adopt right-handed helix conformations and form normal Watson-Crick base pairs with all the bases in the anti conformation. Sugar conformations were determined from measurements of scalar coupling constants in the sugar rings and distance information derived from 1H-1H NOE measurements; all the sugars in the RNA strands of the three duplexes adopt an N-type conformation (A-type structure), whereas the sugars in the DNA strands change from an equilibrium between S- and N-type conformations in the unmodified duplex towards more of the N-type conformation when modified nucleotides are introduced. The presence of three modified T(L) nucleotides induces drastic conformational shifts of the remaining unmodified nucleotides of the DNA strand, changing all the sugar conformations except those of the terminal sugars to the N type. The CD spectra of the three duplexes confirm the structural changes described above. On the basis of the results reported herein, we suggest that the observed conformational changes can be used to tune LNA:RNA duplexes into substrates for RNase H: Partly modified LNA:RNA duplexes may adopt a duplex structure between the standard A and B types, thereby making the RNA strand amenable to RNase H-mediated degradation.