Molecular recognition in purine-rich internal loops: thermodynamic,structural, and dynamic consequences of purine for adenine substitutions in 5'(rGGCAAGCCU)2

The contribution of amino groups to the thermodynamics, structure, and dynamics of tandem A.A mismatches is investigated by substitution of purine (P) for adenine (A) within the RNA duplex, 5'(rGGCAAGCCU)(2), to give 5'(rGGCPAGCCU)(2), 5'(rGGCAPGCCU)(2), and 5'(rGGCPPGCCU)(2). The 5'(rGGCAAGCCU)(2) duplex has sheared A(anti).A(anti) (A.A trans Hoogsteen/Sugar-edge) pairs in which the A5 amino group is involved in hydrogen bonds but the A4 amino group is not [Znosko, B. M., Burkard, M. E., Schroeder, S. J., Krugh, T. R., and Turner, D. H. (2002) Biochemistry 41, 14969-14977]. In comparison to 5'(rGGCAAGCCU)(2), replacing the amino group of A4 with a hydrogen stabilizes the duplex by 1.3 kcal/mol, replacement of the A5 amino group destabilizes the duplex by 0.6 kcal/mol, and replacement of both A4 and A5 amino groups destabilizes the duplex by 0.8 kcal/mol. In NMR structures, the P.A noncanonical pairs of the 5'(rGGCPAGCCU)(2) duplex have a sheared anti-anti structure (P.A trans Hoogsteen/Sugar-edge) with P4.A5 interstrand hydrogen bonding and A5 bases that interstrand stack, similar to the structure of 5'(rGGCAAGCCU)(2). In contrast, the A.P pairs of the 5'(rGGCAPGCCU)(2) duplex have a face-to-face conformation (A.P trans Watson-Crick/Watson-Crick) with intrastrand stacking resembling typical A-form geometry. Although the P5 bases in 5'(rGGCPPGCCU)(2) are involved in an interstrand stack, the loop region is largely undefined. The results illustrate that both hydrogen-bonded and non-hydrogen-bonded amino groups play important roles in determining the thermodynamic, structural, and dynamic characteristics of purine rich internal loops.     

The NMR structure of an internal loop from 23S ribosomal RNA differs from its structure in crystals of 50s ribosomal subunits

Internal loops play an important role in structure and folding of RNA and in recognition of RNA by other molecules such as proteins and ligands. An understanding of internal loops with propensities to form a particular structure will help predict RNA structure, recognition, and function. The structures of internal loops 5' 1009CUAAG1013 3'/3' 1168GAAGC1164 5' and 5' 998CUAAG1002 3'/3' 1157GAAGC1153 5' from helix 40 of the large subunit rRNA in Deinococcus radiodurans and Escherichia coli, respectively, are phylogenetically conserved, suggesting functional relevance. The energetics and NMR solution structure of the loop were determined in the duplex 5' 1GGCUAAGAC9 3'/3' 18CCGAAGCUG10 5'. The internal loop forms a different structure in solution and in the crystal structures of the ribosomal subunits. In particular, the crystal structures have a bulged out adenine at the equivalent of position A15 and a reverse Hoogsteen UA pair (trans Watson-Crick/Hoogsteen UA) at the equivalent of U4 and A14, whereas the solution structure has a single hydrogen bond UA pair (cis Watson-Crick/sugar edge A15U4) between U4 and A15 and a sheared AA pair (trans Hoogsteen/sugar edge A14A5) between A5 and A14. There is cross-strand stacking between A6 and A14 (A6/A14/A15 stacking pattern) in the NMR structure. All three structures have a sheared GA pair (trans Hoogsteen/sugar edge A6G13) at the equivalent of A6 and G13. The internal loop has contacts with ribosomal protein L20 and other parts of the RNA in the crystal structures. These contacts presumably provide the free energy to rearrange the base pairing in the loop. Evidently, molecular recognition of this internal loop involves induced fit binding, which could confer several advantages. The predicted thermodynamic stability of the loop agrees with the experimental value, even though the thermodynamic model assumes a Watson-Crick UA pair.     

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.     

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.     

Structural features and thermodynamics of the J4/5 loop from the Candida albicans and Candida dubliniensis group I introns

The J4/5 loop of group I introns has tertiary interactions with the P1 helix that position the P1 substrate for the self-splicing reaction. The J4/5 loop of Candida albicans and Candida dubliniensis, 5'GAAGG3'/3'UAAUU5', potentially contains two A.A pairs flanked by one G.U pair on one side and two G.U pairs on the other side. Results from optical melting, nuclear magnetic resonance spectroscopy, and functional group substitution experiments with a mimic of the C. albicans and C. dubliniensis J4/5 loop are consistent with the adenosines forming tandem sheared A.A pairs with a cross-strand stack and only the G.U pair not adjacent to an A.A pair forming a static wobble G.U pair. The two G.U pairs adjacent to the tandem A.A pairs are likely in a dynamic equilibrium between multiple conformations. Although Co(NH(3))(6)(3+) stabilizes the loop by several kilocalories per mole at 37 degrees C, addition of Mg(2+) or Co(NH(3))(6)(3+) has no effect on the structure of the loop. The tandem G.U pairs provide a pocket of negative charge for Co(NH(3))(6)(3+) to bind. The results contribute to understanding the structure and dynamics of purine-rich internal loops and potential G.U pairs adjacent to internal loops.     

The First Example of a Hoogsteen Basepaired DNA Duplex in Dynamic Equilibrium with a Watson-Crick Basepaired Duplex—A Structural (NMR), Kinetic and Thermodynamic Study

Abstract

A single-point substitution of the O4′ oxygen by a CH₂ group at the sugar residue of A ⁶ (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 A ⁶:T⁷ Hoogsteen basepaired (1B) B-type DNA duplex, resulting in a dynamic equilibrium of (1A)→←(1B): K_eq = 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; δH°? = 164±14 kJ/mol;-TδS°? (298K) = ?92 kJ/mol giving a δG₂₉₈°? 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, δH°? = 153±13 kJ/mol;-TδS°? (298K) = ?82 kJ/mol giving a δG₂₉₈°? of 71 kJ/mol. Ea (k-1) = 155±13 kJ/mol]. A comparison of δG₂₉₈°? 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 A ⁶: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 A ⁶:T⁷ basepairs in (1B) has enforced a syn conformation on the glycosyl torsion of the 2′- deoxyaristeromycin moiety, A ⁶, as a result of substitution of the endocyclic 4′-oxygen in the natural sugar with a methylene group in A ⁶. A comparison of the Watson-Crick basepaired duplex (1A) to the Hoogsteen basepaired duplex (1B) shows that only a few changes, mainly in α, σ and γ torsions, in the sugar-phosphate backbone seem to be necessary to accommodate the Hoogsteen basepair.     

Nuclear magnetic resonance spectroscopy and molecular modeling reveal that different hydrogen bonding patterns are possible for G.U pairs: one hydrogen bond for each G.U pair in r(GGCGUGCC)(2) and two for each G.U pair in r(GAGUGCUC)(2)

G.U pairs occur frequently and have many important biological functions. The stability of symmetric tandem G.U motifs depends both on the adjacent Watson-Crick base pairs, e.g., 5'G > 5'C, and the sequence of the G.U pairs, i.e., 5'-UG-3' > 5'-GU-3', where an underline represents a nucleotide in a G.U pair [Wu, M., McDowell, J. A., and Turner, D. H. (1995) Biochemistry 34, 3204-3211]. In particular, at 37 degrees C, the motif 5'-CGUG-3' is less stable by approximately 3 kcal/mol compared with other symmetric tandem G.U motifs with G-C as adjacent pairs: 5'-GGUC-3', 5'-GUGC-3', and 5'-CUGG-3'. The solution structures of r(GAGUGCUC)(2) and r(GGCGUGCC)(2) duplexes have been determined by NMR and restrained simulated annealing. The global geometry of both duplexes is close to A-form, with some distortions localized in the tandem G.U pair region. The striking discovery is that in r(GGCGUGCC)(2) each G.U pair apparently has only one hydrogen bond instead of the two expected for a canonical wobble pair. In the one-hydrogen-bond model, the distance between GO6 and UH3 is too far to form a hydrogen bond. In addition, the temperature dependence of the imino proton resonances is also consistent with the different number of hydrogen bonds in the G.U pair. To test the NMR models, U or G in various G.U pairs were individually replaced by N3-methyluridine or isoguanosine, respectively, thus eliminating the possibility of hydrogen bonding between GO6 and UH3. The results of thermal melting studies on duplexes with these substitutions support the NMR models.     

Hybrid characteristics of oligonucleotides consisting of isonucleoside 2',5'-anhydro-3'-deoxy-3'-(thymin-1-yl)-D-mannitol with different linkage modes

Oligonucleotides consisting of the isonucleoside repeating unit 2',5'-anhydro-3'-deoxy-3'-(thymin-1-yl)-D-mannitol (4) were synthesized with the monomeric unit 4 incorporated into oligonucleotides as 1'-->4' linkage 4a (oligomer I) or 6'-->4' linkage 4b (oligomer II). The hybrid properties of the two oligonucleotides I and II with their complementary strands were investigated by thermal denaturation and CD spectra. Oligonucleotide I (4a) formed a stable duplex with d(A)(14) with a slightly reduced T(m) value of 36.6 degrees C, relative to 38.2 degrees C for the control duplex d(T)(14)/d(A)(14), but oligomer II (4b) failed to hybridize with a DNA complementary single strand. The spectrum of the duplex oligomer I/d(A)(14) showed a positive CD band at 217 nm and a negative CD band at 248 nm attributable to a B-like conformation. Molecular modeling showed that in the case of oligomer I: the C6' hydroxy group of each unit could be located in the groove area when hybridized to the DNA single strand, which might contribute additional hydrogen bonding to the stability of duplex formation.     

An alternating sheared AA pair and elements of stability for a single sheared purine-purine pair flanked by sheared GA pairs in RNA

A previous NMR structure of the duplex 5'GGU GGA GGCU/PCCG AAG CCG5' revealed an unusually stable RNA internal loop with three consecutive sheared GA pairs. Here, we report NMR studies of two duplexes, 5'GGU GGA GGCU/PCCA AAG CCG5' (replacing the UG pair with a UA closing pair) and 5'GGU GAA GGCU/PCCG AAG CCG5' (replacing the middle GA pair with an AA pair). An unusually stable loop with three consecutive sheared GA pairs forms in the duplex 5'GGU GGA GGCU/PCCA AAG CCG5'. The structure contrasts with that reported for this loop in the crystal structure of the large ribosomal subunit of Deinococcus radiodurans [Harms, J., Schluenzen, F., Zarivach, R., Bashan, A., Gat, S., Agmon, I., Bartels, H., Franceschi, F., and Yonath, A. (2001) Cell 107, 679-688]. The middle AA pair in the duplex 5'GGU GAA GGCU/PCCG AAG CCG5' rapidly exchanges orientations, resulting in alternative base stacking and pseudosymmetry with exclusively sheared pairs. The U GAA G/G AAG C internal loop is 2.1 kcal/mol less stable than the U GGA G/G AAG C internal loop at 37 degrees C. Structural, energetic, and dynamic consequences upon functional group substitutions within related 3 x 3 and 3 x 6 internal loops are also reported.     

Crystal structure of an RNA duplex r(G GCGC CC)2 with non-adjacent G*U base pairs

The crystal structure of a self-complementary RNA duplex r(GGGCGCUCC)2with non-adjacent G*U and U*G wobble pairs separated by four Watson-Crick base pairs has been determined to 2.5 A resolution. Crystals belong to the space group R3; a = 33.09 A,alpha = 87.30 degrees with a pseudodyad related duplex in the asymmetric unit. The structure was refined to a final Rworkof 17.5% and Rfreeof 24.0%. The duplexes stack head-to-tail forming infinite columns with virtually no twist at the junction steps. The 3'-terminal cytosine nucleosides are disordered and there are no electron densities, but the 3' penultimate phosphates are observed. As expected, the wobble pairs are displaced with guanine towards the minor groove and uracil towards the major groove. The largest twist angles (37.70 and 40.57 degrees ) are at steps G1*C17/G2*U16 and U7*G11/C8*G10, while the smallest twist angles (28.24 and 27.27 degrees ) are at G2*U16/G3*C15 and C6*G12/U7*G11 and conform to the pseudo-dyad symmetry of the duplex. The molecule has two unequal kinks (17 and 11 degrees ) at the wobble sites and a third kink at the central G5 site which may be attributed to trans alpha (O5'-P), trans gamma (C4'-C5') backbone conformations. The 2'-hydroxyl groups in the minor groove form inter-column hydrogen bonding, either directly or through water molecules.     

2D NMR investigation of the binding of the anticancer drug actinomycin D to duplexed dATGCGCAT: conformational features of the unique 2:1 adduct

One- and two-dimensional NMR studies on the oligomer dA1T2G3C4G5C6A7T8, with and without actinomycin D (ActD), were conducted. Analysis of the NMR data, particularly 2D NOE intensities, revealed that the free oligonucleotide is a duplex in a standard right-handed B form. At the ratio of 1 ActD/duplex (R = 1), 1D NMR studies indicate that two 1:1 unsymmetric complexes form in unequal proportions with the phenoxazone ring intercalated at a GpC site, in agreement with previous studies [Scott, E.V., Jones, R.L., Banville, D.L., Zon, G., Marzilli, L.G., & Wilson, W.D. (1988) Biochemistry 27, 915-923]. The 2D COSY data also confirm this interpretation since eight cytosine H6 to H5 and two ActD H8 to H7 cross-peaks are observed. At R = 2, both COSY and NOESY spectra confirm the formation of a unique 2:1 species with C2 symmetry. The oligomer remains in a right-handed duplex but undergoes extreme conformational changes both at and adjacent to the binding site. The deoxyribose conformation of T2, C4, and C6 shifts from primarily C2'-endo in the free duplex to an increased amount of C3'-endo in the 2:1 complex as revealed by the greater intensity of the base H6 to 3' NOE cross-peak relative to the intensity of the H6 to H2' NOE cross-peak. This conformational change widens the minor groove and should help alleviate the steric crowding of the ActD peptides. The orientation of the ActD molecules at R = 2 has the quinoid portion of the phenoxazone ring at the G3pC4 site and the benzenoid portion of the phenoxazone ring at the G5pC6 site on the basis of NOE cross-peaks from ActD H7 and H8 to G5H8 and C6H6. All base pairs retain Watson-Crick type H-bonding, unlike echinomycin complexes [e.g., Gao, X., & Patel, D.J. (1988) Biochemistry 27, 1744-1751] where Hoogsteen base pairs have been observed. In contrast to previous studies on ActD, we were able to distinguish the two peptide chains.(ABSTRACT TRUNCATED AT 400 WORDS)     

Solution structure of a DNA double helix incorporating four consecutive non-Watson-Crick base-pairs

A series of DNA 21-mers containing a variety of the 4 x 4 internal loop sequence 5'-CAAG-3'/3'-ACGT-5' were studied using nuclear magnetic resonance (NMR) methodology and distance geometry (DG)/molecular dynamics (MD) approaches. Such oligomers exhibit excellent resolution in the NMR spectra and reveal many unusual NOEs (nuclear Overhauser effect) that allow for the detailed characterization of a DNA hairpin incorporating a track of four different non-Watson-Crick base-pairs in the stem. These include a wobble C.A base-pair, a sheared A.C base-pair, a sheared A.G base-pair, and a wobble G.T base-pair. Significantly different twisting angles were observed between the base-pairs in internal loop that results with excellent intra-strand and inter-strand base stacking within the four consecutive mismatches and the surrounding canonical base-pairs. This explains why it melts at 52 degrees C even though five out of ten base-pairs in the stem adopt non-Watson-Crick pairs. However, the 4 x 4 internal loop still fits into a B-DNA double helix very well without significant change in the backbone torsion angles; only zeta torsion angles between the tandem sheared base-pairs are changed to a great extent from the gauche(-) domain to the trans domain to accommodate the cross-strand base stacking in the internal loop. The observation that several consecutive non-canonical base-pairs can stably co-exist with Watson-Crick base-pairs greatly increases the limited repertoire of irregular DNA folds and reveals the possibility for unusual structural formation in the functionally important genomic regions that have potential to become single-stranded.     

Phosphorothioate analogues of (2'-5')(A)4: agonist and antagonist activities in intact cells

Metabolically stable phosphorothioate tetramer analogues of (2'-5')(A)n with Rp and/or Sp chirality in the 2'-5'-phosphodiester linkages constitute a new class of antiviral agents since they mimic the effects of interferons. Three of the diastereomeric 5'-monophosphates (i.e., pRpRpRp, pSpRpRp, and pRpSpSp) bind to and activate RNase L from extracts of HeLa cells. However, the pSpSpSp (2'-5')-(A)4-phosphorothioate is unique in that it binds to, but cannot activate, RNase L to cleave rRNA. When microinjected into the cytoplasm of HeLa cells followed by virus infection, the pRpRpRp, pSpRpRp, and pRpSpSp (2'-5')(A)4-phosphorothioates demonstrate antiviral activity, as does (2'-5')(A)4ox-red, an active (2'-5')(A)n analogue. When microinjected simultaneously with (2'-5')(A)nox-red, an active the pSpSpSp (2'-5')(A)4-phosphorothioate inhibits activation of RNase L in HeLa cells, thereby blocking direct protection of vesicular stomatitis virus. The agonist and antagonist properties of pRpRpRp and pSpSpSp, respectively, are transient probably as a consequence of the hydrolysis of the 5'-monophosphate and formation of the less active (2'-5')(A)4-phosphorothioate cores. The possible use of these (2'-5')(A)4-phosphorothioates as tools for dissecting the biological significance of the (2'-5')(A)n system or in antiviral chemotherapy is discussed.     

Mechanistic information on the reaction of cis- and trans-[RuCl2(DMSO)4] with d(T2GGT2) derived from MALDI-TOF and HPLC studies

Reactions of trans and cis isomers of the Ru(II) complex [RuCl(2)(DMSO)(4)] with single-stranded hexanucleotide d(T(2)GGT(2)) were studied in aqueous solutions in the absence and presence of excess chloride by high performance liquid chromatography (HPLC) and matrix-assisted laser desorption/ionisation time of flight mass spectrometry (MALDI-TOF MS). Despite the different reactive species formed from the two isomers in aqueous solution, similar reaction products are obtained in their interaction with d(T(2)GGT(2)). Both [RuCl(2)(DMSO)(4)] isomers bind to the oligonucleotide in the bidentate mode to form thermodynamically stable bis-guanosine adducts, Ru(G-N7)(2). Significant differences were observed in the reaction rates, however the reaction with trans- [RuCl(2)(DMSO)(4)] is ca. 5-10 times faster in comparison to that observed for the cis analogue. This difference is interpreted in terms of different rate-limiting steps for the trans and cis complexes, respectively. It is suggested that the rate of the reaction with the trans isomer is controlled by dissociation of a Cl(-) ligand from the initially formed trans,cis,cis-[RuCl(2)(DMSO)(2)(H(2)O)(2)]. In the contrast, release of a dimethyl sulfoxide molecule from the reactive species cis,fac-[RuCl(2)(DMSO)(3)(H(2)O)] is likely to be rate limiting for the cis analogue. Significant influence of electrostatic interactions on the reaction rate was observed for the trans isomer. Mechanistic interpretation of the observed reactivity trends based on data obtained from UV-Vis spectroscopy, HPLC and MALDI-TOF MS studies is presented and discussed within the paper.     

High-resolution NMR study of a synthetic DNA-RNA hybrid dodecamer containing the consensus pribnow promoter sequence: d(CGTTATAATGCG).r(CGCAUUAUAACG)

The nonsymmetrical double-helical hybrid dodecamer d(CGTTATAATGCG).r(CGCAUUAUAACG) was synthesized with solid-phase phosphoramidite methods and studied by high-resolution 2D NMR. The imino protons were assigned by one-dimensional nuclear Overhauser methods. All the base protons and H1', H2', H2", H3', and H4' sugar protons of the DNA strand and the base protons, H1', H2', and most of the H3'-H4' protons of the RNA strand were assigned by 2D NMR techniques. The well-resolved spectra allowed a qualitative analysis of relative proton-proton distances in both strands of the dodecamer. The chemical shifts of the hybrid duplex were compared to those of the pure DNA double helix with the same sequence (Wemmer et al., 1984). The intrastrand and cross-strand NOEs from adenine H2 to H1' resonances of neighboring base pairs exhibited characteristic patterns that were very useful for checking the spectral assignments, and their highly nonsymmetric nature reveals that the conformations of the two strands are quite different. Detailed analysis of the NOESY and COSY spectra, as well as the chemical shift data, indicate that the RNA strand assumes a normal A-type conformation (C3'-endo) whereas the DNA strand is in the general S domain but not exactly in the normal C2'-endo conformation. The overall structure of this RNA-DNA duplex is different from that reported for hybrid duplexes in solution by other groups (Reid et al., 1983a; Gupta et al., 1985) and is closer to the C3'-endo-C2'-endo hybrid found in poly(dA).poly(dT) and poly(rU).poly(dA) in the fiber state (Arnott et al., 1983, 1986).     

NMR characterization of clustered bistrand abasic site lesions: effect of orientation on their solution structure

A unique characteristic of ionizing radiation and radiomimetic anticancer drugs is the induction of clustered damage: two or more DNA lesions (oxidized bases, abasic sites, or strand breaks) occurring in the same or different strands of the DNA molecule within a single turn of the helix. In spite of arising at a lower frequency than single lesions, clustered DNA damage represents an exotic challenge to the repair systems present in the cells and, in some cases, these lesions may escape detection and/or processing. To understand the structural properties of clustered DNA lesions we have prepared two oligodeoxynucleotide duplexes containing adjacent tetrahydrofuran residues (abasic site analogues), positioned one in each strand of the duplex in a 5' or 3' orientation, and determined their solution structure by NMR spectroscopy and molecular dynamics simulations. The NMR data indicate that both duplex structures are right-handed helices of high similarity outside the clustered damage site. The thermal stability of the duplexes is severely reduced by the presence of the abasic residues, especially in a 5' orientation where the melting temperature is 5 degrees C lower. The structures show remarkable differences at the lesion site where the extrahelical location of the tetrahydrofuran residues in the (AP)(2)-5'-staggered duplex contrasts with their smooth alignment along the sugar-phosphate backbone in the (AP)(2)-3'-staggered duplex.     

The crystal structure of an RNA oligomer incorporating tandem adenosine-inosine mismatches.

The X-ray crystallographic structure of the RNA duplex [r(CGCAIGCG)]2 has been refined to 2.5 A. It shows a symmetric internal loop of two non-Watson-Crick base pairs which form in the middle of the duplex. The tandem A-I/I-A pairs are related by a crystallographic two-fold axis. Both A(anti)-I(anti) mismatches are in a head-to-head conformation forming hydrogen bonds using the Watson-Crick positions. The octamer duplexes stack above one another in the cell forming a pseudo-infinite helix throughout the crystal. A hydrated calcium ion bridges between the 3'-terminal of one molecule and the backbone of another. The tandem A-I mismatches are incorporated with only minor distortion to the backbone. This is in contrast to the large helical perturbations often produced by sheared G-A pairs in RNA oligonucleotides.     

Intercalation of the (-)-(1R,2S,3R, 4S)-N6-[1-benz[a]anthracenyl]-2'-deoxyadenosyl adduct in an oligodeoxynucleotide containing the human N-ras codon 61 sequence

The solution structure of the (-)-(1R,2S,3R,4S)-N6-[1-(1,2,3, 4-tetrahydroxy-benz[a]anthracenyl)]-2'-deoxyadenosyl adduct at X6 of 5'-d(CGGACXAGAAG)-3'.5'-d(CTTCTTGTCCG)-3', incorporating codons 60, 61(italic), and 62 of the human N-ras protooncogene, was determined. This adduct results from the trans opening of 1S,2R,3R,4S-1, 2-epoxy-1,2,3,4-tetrahydro-benz[a]anthracenyl-3,4-diol by the exocyclic N6 of adenine. Molecular dynamics simulations were restrained by 509 NOEs from 1H NMR. The precision of the refined structures was monitored by pairwise root-mean-square deviations which were <1.2 A; accuracy was measured by complete relaxation matrix calculations, which yielded a sixth root R factor of 9.1 x 10(-)2 at 250 ms. The refined structure was a right-handed duplex, in which the benz[a]anthracene moiety intercalated from the major groove between C5.G18 and R,S,R,SA6.T17. In this orientation, the saturated ring of BA was oriented in the major groove of the duplex, with the aromatic rings inserted into the duplex such that the terminal ring of BA threaded the duplex and faced toward the minor groove direction. The duplex suffered localized distortion at and immediately adjacent to the adduct site, evidenced by the increased rise of 8.8 A as compared to the value of 3.5 A normally observed for B-DNA between base pairs C5.G18 and R,S,R,SA6.T17. These two base pairs also buckled in opposite directions away from the intercalated BA moiety. The refined structure was similar to the (-)-(7S,8R,9S,10R)-N6-[10-(7,8,9, 10)-tetrahydrobenzo[a]pyrenyl)]-2'-deoxyadenosyl adduct of corresponding stereochemistry at X6 of the same oligodeoxynucleotide [Zegar, I. S., Kim, S. J., Johansen, T. N., Horton, P. J., Harris, C. M., Harris, T. M., and Stone, M. P. (1996) Biochemistry 35, 6212-6224]. Both adducts intercalated toward the 5'-direction from the site of adduction. The similarities in solution structures were reflected in similar biological responses, when repair-deficient AB2480 Escherichia coli were transformed with M13mp7L2 DNA site-specifically modified with these two adducts.     

Solution structure of [d(ATGAGCGAATA)]2. Adjacent G:A mismatches stabilized by cross-strand base-stacking and BII phosphate groups.

The solution structure of a rather unusual B-form duplex [d(ATGAGCGAATA)]2 has been determined using two-dimensional nuclear magnetic resonance (2D-NMR) and distance geometry methods. This sequence forms a stable ten base-pair B-form duplex with 3' overhangs and two pairs of adjacent G:A mismatches paired via a sheared hydrogen-bonding scheme. All non-exchangeable protons, including the stereo-specific H-5'S/H-5'R of the 3G and 7G residues, were assigned by 2D-NMR. The phosphorus spectrum was assigned using heteronuclear correlation with H-3' and H-4' reasonances. The complete assignments reveal several unusual nuclear Overhauser enhancements (NOEs) and unusual chemical shifts for the neighboring G:A mismatch pairs and their adjacent nucleotides. Inter-proton distances were derived from time-dependent NOEs and used to generate initial structures, which were further refined by iterative back-calculation of the two-dimensional nuclear Overhauser enhancement spectra; 22 final structures were calculated from the refined distance bounds. All these final structures exhibit fully wound helical structures with small penalty values against the refined distance bounds and small pair-wise root-mean-square deviation values (typically 0.5 A to 0.9 A). The two helical strands exchange base stacking at both of the two G:A mismatch sites, resulting in base stacking down each side rather than down each strand of the twisted duplex. Very large twist angles (77 degrees) were found at the G:A mismatch steps. All the final structures were found to have BII phosphate conformations at the adjacent G:A mismatch sites, consistent with observed downfield 31P chemical shifts and Monte-Carlo conformational search results. Our results support the hypothesis that 31P chemical shifts are related to backbone torsion angles. These BII phosphate conformations in the adjacent G:A mismatch step suggest that hydrogen bonding of the G:A pair G-NH2 to a nearby phosphate oxygen atom is unlikely. The unusual structure of the duplex may be stabilized by strong interstrand base stacking as well as intrastrand stacking, as indicated by excellent base overlap within the mismatch stacks.