Molecular dynamics simulation of 7, 8-dihydro-8-oxoguanine DNA

To elucidate the effect of guanine lesion produced by the oxidative damage on DNA, 1 nanosecond molecular dynamics simulations of native and oxidized DNA were performed. The target DNA molecules are dodecamer duplex d(CGCGAATTCGCG)(2) and its derivative duplex d(C(1)G(2)C(3)(8-oxoG)(4)A(5)A(6)T(7)T(8)C(9)G(10)C(11)G(12).d(C(13)G(14)C(15)G(16)A(17)A(18)T(19)T(20)C(21)G(22)C(23)G(24), which has one oxidized guanine, 7, 8-dihydro-8-oxoguanine (8-oxoG), at the fourth position. The local structural change due to the lesion of 8-oxoG and the global dynamic structure of the 8-oxoG DNA were studied. It was found that the 8-oxoG DNA remained structurally stable during the simulation due to newly produced hydrogen bonds around the (8-oxoG)(4) residue. However, there were distinguishable differences in structural parameters and dynamic property in the 8-oxoG DNA. The conformation around the (8-oxoG)(4) residue departed from the usual conformation of native DNA and took an unique conformation of epsilon-zeta in B(II) conformation and chi in high anti orientation at the (8-oxoG)(4) residue, and adopted a very low helical twist angle at the C(3):G(22)-(8-oxoG)(4):C21) step. Further analysis by principal component analysis indicated that the formation of the hydrogen bonds around the (8-oxoG)(4) residue plays a role as a trigger for the conformational transition of the 8-oxoG DNA in the conformational space.     

Conformations of DNA Duplexes Containing 8-Oxoguanine

Abstract

As a step towards elucidating the mechanisms of mutagenesis induced by irradiation and oxidation, we study the incorporation of 8-oxoguanine (OG) into duplex DNA. Molecular modelling is used to reveal changes in DNA conformational parameters due to mispairs within the sequences d(A₅XA₅) · d(T₅YT₅) and d(G₅XG₅) · d(C₅YC₅) where one of the bases of the bases of the central X:Y pair is OG and the other A T, G or C. The G:C to OG:C replacements in DNA duplexes produce only minor conformational changes, similar to normal base sequence effects. The calculations suggest that both OG(syn): G and OG(syn): A mispairs can also be introduced without drastic distortion of sugar-phosphate backbone. The distortions produced by OG-containing mispairs are also found to be sequence dependent Overall these calculations suggest that the G→OG conversion could be an important factor in the irradiative or oxidative damage of DNA.     

Crystal structure of d(GCGAAAGCT) containing a parallel-stranded duplex with homo base pairs and an anti-parallel duplex with Watson-Crick base pairs

A DNA fragment d(GCGAAAGCT), known to adopt a stable mini-hairpin structure in solution, has been crystallized in the space group I4₁22 with the unit-cell dimensions a = b = 53.4 Å and c = 54.0 Å, and the crystal structure has been determined at 2.5 Å resolution. The four nucleotide residues CGAA of the first half of the oligomer form a parallel duplex with another half through the homo base pairs, C₂:C₂⁺ (singly-protonated between the Watson– Crick sites), G₃:G₃ (between the minor groove sites), A₄:A₄ (between the major groove sites) and A₅:A₅ (between the Watson–Crick sites). The two strands remaining in the half of the parallel duplex are split away in different directions, and they pair in an anti-parallel B-form duplex with the second half extending from a neighboring parallel duplex, so that an infinite column is formed in a head-to-tail fashion along the c-axis. It seems that a hexa-ammine cobalt cation supports such a branched and bent conformation of the oligomer. One end of the parallel duplex is stacked on the corresponding end of the adjacent parallel duplex; between them, the guanine base of the first residue is stacked on the fourth ribose of another duplex.     

Base-pair exchange kinetics of the imino and amino protons of the 3′-phenazinium tethered DNA-RNA duplex,r(5′GAUUGAA3′):d(5′TCAATC3′-Pzn), and their comparison with those of B-DNA duplex

The dynamics of the opening-closing of the constituent base-pairs as well as of the exchange kinetics of the base-paired imino and amino protons with water in a DNA-RNA hybrid, [^5′r(G¹A²U³U⁴G⁵A⁶A⁷)^3′]:^5′p[d(T⁸C⁹A¹⁰A¹¹T¹²C¹³)]^3′-Pzn] duplex (I), are reported here in details for the first time. The exchange kinetics of amino and imino protons in the DNA-RNA hybrid (duplex I) have been compared with identical studies on the following B-DNA duplexes: d(C¹G²T³A⁴C⁵G⁶)₂ (II), d[p(^5′T¹G²T³T⁴T⁵G⁶ G⁷C⁸)^3′]:d[p(^5′C⁹C¹⁰A¹¹A¹²A¹³C¹⁴A¹⁵)^3′] (III), d(C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶)₂ (IV) and d(C¹G²C³G⁴C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶C¹⁷G¹⁸C¹⁹G²⁰)₂ (V). This comparative study shows that the life-times τ_o of various base-pairs in the DNA-RNA hybrid (I) varies in the range of ∼ 1 ms, and they are quite comparable to those of the shorter B-DNA duplexes (II) and (III), but very different from the τ_o of the larger duplexes (IV) and (V): the τ_o for the base pair of T¹¹ and T¹² residues in the 20-mer (duplex V) are 2.9 ± 2.3 ms and 23.2 ± 8.9 ms, respectively, while the corresponding τ_o in the 12-mer (duplex IV) are 2.8 ± 2.2 ms and 17.4 ± 5.4 ms. It has also been shown that the total energy of activation (E_a) assessed from the exchange rates of both imino and amino protons, representing energetic contributions from both base-pair and helix opening-closing as well as from the exchange process of the imino protons from the open state with the bound water, is close to the E_a of the short B-DNA duplex (E_a ≈ 28–47 kcal/mol).     

Light-induced oxidation of the telomeric G4 DNA in complex with Zn(II) tetracarboxymethyl porphyrin

Structure-specific ligands are convenient tools for the recognition, targeting or probing of non-canonical DNA structures. Porphyrin derivatives exhibit a preference for interaction with G-quadruplex (G4) structures over canonical duplex DNA and are able to cause photoinducible damage to nucleic acids. Here, we show that Zn(II) 5,10,15,20-tetrakis(N-carboxymethyl-4-pyridinium)porphyrin (ZnP1) interacts with different conformations of the telomeric sequence d(TAGGG(TTAGGG)₃) at submicromolar concentrations without any detectible disturbance of the particular fold. Among different folds, potassium (3+1) hybrid G4-structure. reveal the highest affinity to ZnP1. The pattern of guanine oxidation is specific for each telomeric DNA conformation and may serve as an additional tool for probing the G4 topology. The potassium (3+1) and parallel G4 conformations are more susceptible to light-induced oxidation than the sodium G4 conformation or double helix of the telomeric DNA. The major products of the guanine modifications are spiroiminodihydantoin (Sp) and 8-oxoguanine (8-oxoG). ZnP1-induced oxidation of guanines results in the structural rearrangement of parallel and (3+1) G4 conformations yielding an antiparallel-like G4 conformation. The mechanism of the observed light-induced conformational changes is discussed.     

The C-terminal Lysine of Ogg2 DNA Glycosylases is a Major Molecular Determinant for Guanine/8-Oxoguanine Distinction

7,8-Dihydro-8-oxoguanine (8-oxoG) is a major oxidative lesion found in DNA. The 8-oxoguanine DNA glycosylases (Ogg) responsible for the removal of 8-oxoG are divided into three families Ogg1, Ogg2 and AGOG. The Ogg2 members are devoid of the recognition loop used by Ogg1 to discriminate between 8-oxoG and guanine and it was unclear until recently how Ogg2 enzymes recognize the oxidized base. We present here the first crystallographic structure of an Ogg2 member, Methanocaldococcus janischii Ogg, in complex with a DNA duplex containing the 8-oxoG lesion. This structure highlights the crucial role of the C-terminal lysine, strictly conserved in Ogg2, in the recognition of 8-oxoG. The structure also reveals that Ogg2 undergoes a conformational change upon DNA binding similar to that observed in Ogg1 glycosylases. Furthermore, this work provides a structural rationale for the lack of opposite base specificity in this family of enzymes.     

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.     

Evidence for long-range interactions in DNA. Analysis of melting curves of block polymers d(C15A15)·d(T15G15), d(C20A15)·d(T15G20), and d(C20A10)·d(T10G20)

The influence of one DNA region on the stability of an adjoining region (telestability) was examined. Melting curves of three block DNA's, d(C₁₅A₁₅)·d(T₁₅G₁₅), d(C₂₀A₁₅)·d(T₁₅G₂₀), and d(C₂₀A₁₀)·d(T₁₀G₂₀) were analyzed in terms of the nearest neighbor Ising model. Comparisons of predicted and experimental curves were made in 0.01 M and 0.1 M sodium ion solutions. The nearest neighbor formalism was also employed to analyze block DNA transition in the presence of actinomycin, a G·C specific molecule. The results show that nearest neighbor base-pair interaction cannot predict the melting curves of the block DNA's. Adjustments in theoretical parameters to account for phosphate repulsion assuming a B conformation throughout the DNA's do not alter this conclusion. Changes in the theoretical parameters, which provide good overall agreement, are consistent with a substantial stabilization of the A·T region nearest the G·C block. The melting temperature T A·T for the average A·T pari in d(C₂₀A₁₀)·d(T₁₀G₂₀), with 10 A·T pairs, appears to be 4°C greater than T_A·T for d(C₁₅A₁₅)·d(T₁₅G₁₅) and d(C₂₀A₁₅)·d(T₁₅G₂₀), both with 15 A·T pairs. Actinomycin bound to the G·C end effectively stabilizes the A·T end by 9°C. These results indicate a long-range contribution to the interactions governing DNA stability. A possible mechanism for these interactions will be discussed.     

The Residence Time of the Bound Water in the Hydrophobic Minor Groove of the Carbocyclic-Nucleoside Analogs of Dickerson-Drew Dodecamers

Summary

The residence time of the bound water molecules in the antisense oligodeoxyribonucleotides containing 7′-α-methyl (T_Me). carbocyclic thymidines in duplex (I), d⁵′(¹C²G³C⁴G⁵A⁶A⁷T_Mc ⁸T_Mc ⁹C¹⁰G¹¹C¹²G)₂ ³′, and 6′-a-hydroxy (T_OH) carbocyclic thymidines in duplex (II), d⁵′(¹C³G³C⁴G⁵A_OH ⁶ A_OH ⁷T_OH ⁸ T_OH ⁹C¹⁰G¹¹C¹²G)₂3, have been investigated using a combination of NOESY and ROESY experiments. Because of the presence of 7′-α-methyl groups of T_Me in the centre of the minor groove in duplex (I), the residence time of the bound water molecule is shorter than 0.3 ns. The dramatic reduction of the residence time of the water molecule in the minor groove in duplex (I) compared with the natural counterpart has been attributed to the replacement of second shell of hydration and disruption of hydrogen-bonding with 04′ in the minor groove by hydrophobic α-methyl groups, as originally observed in the X-ray study. This effect could not be attributed to the change of the width of the minor groove because a comparative NMR study of the duplex (I) and its natural counterpart showed that the widths of their minor grooves are more or less unchanged (r.m.s.d change in the core part is <0.63Å). For duplex (II) with polar 6′-α-hydroxyl groups pointed to the minor groove, the correlation time is much longer than 0.36ns as a result of the stabilising hydrogen-bonding interaction with N3 or 02 of the neighbouring nucleotides.     

Recognition of O6-benzyl-2′-deoxyguanosine by a perimidinone-derived synthetic nucleoside: a DNA interstrand stacking interaction

The 2′-deoxynucleoside containing the synthetic base 1-[(2R,4S,5R)-4-hydroxy-5-(hydroxymethyl)-tetrahydrofuran-2-yl)-1H-perimidin-2(3H)-one] (dPer) recognizes in DNA the O⁶-benzyl-2′-deoxyguanosine nucleoside (O⁶-Bn-dG), formed by exposure to N-benzylmethylnitrosamine. Herein, we show how dPer distinguishes between O⁶-Bn-dG and dG in DNA. The structure of the modified Dickerson–Drew dodecamer (DDD) in which guanine at position G⁴ has been replaced by O⁶-Bn-dG and cytosine C⁹ has been replaced with dPer to form the modified O⁶-Bn-dG:dPer (DDD-XY) duplex [5′-d(C¹G²C³X⁴A⁵A⁶T⁷T⁸Y⁹G¹⁰C¹¹G¹²)-3′]₂ (X = O⁶-Bn-dG, Y = dPer) reveals that dPer intercalates into the duplex and adopts the syn conformation about the glycosyl bond. This provides a binding pocket that allows the benzyl group of O⁶-Bn-dG to intercalate between Per and thymine of the 3′-neighbor A:T base pair. Nuclear magnetic resonance data suggest that a similar intercalative recognition mechanism applies in this sequence in solution. However, in solution, the benzyl ring of O⁶-Bn-dG undergoes rotation on the nuclear magnetic resonance time scale. In contrast, the structure of the modified DDD in which cytosine at position C⁹ is replaced with dPer to form the dG:dPer (DDD-GY) [5′-d(C¹G²C³G⁴A⁵A⁶T⁷T⁸Y⁹G¹⁰C¹¹G¹²)-3′]₂ duplex (Y = dPer) reveals that dPer adopts the anti conformation about the glycosyl bond and forms a less stable wobble pairing interaction with guanine.     

Shape readout of AT‐rich DNA by carbohydrates

Gene expression can be altered by small molecules that target DNA; sequence as well as shape selectivities are both extremely important for DNA recognition by intercalating and groove‐binding ligands. We have characterized a carbohydrate scaffold (1) exhibiting DNA “shape readout” properties. Thermodynamic studies with 1 and model duplex DNAs demonstrate the molecule's high affinity and selectivity towards B* form (continuous AT‐rich) DNA. Isothermal titration calorimetry (ITC), circular dichroism (CD) titration, ultraviolet (UV) thermal denaturation, and Differential Scanning Calorimetry were used to characterize the binding of 1 with a B* form AT‐rich DNA duplex d[5′‐G₂A₆T₆C₂‐3′]. The binding constant was determined using ITC at various temperatures, salt concentrations, and pH. ITC titrations were fit using a two‐binding site model. The first binding event was shown to have a 1:1 binding stoichiometry and was predominantly entropy‐driven with a binding constant of approximately 10⁸ M^?1. ITC‐derived binding enthalpies were used to obtain the binding‐induced change in heat capacity (ΔC_p) of ?225 ± 19 cal/mol·K. The ionic strength dependence of the binding constant indicated a significant electrolytic contribution in ligand:DNA binding, with approximately four to five ion pairs involved in binding. Ligand 1 displayed a significantly higher affinity towards AT‐tract DNA over sequences containing GC inserts, and binding experiments revealed the order of binding affinity for 1 with DNA duplexes: contiguous B* form AT‐rich DNA (d[5′‐G₂A₆T₆C₂‐3′]) >B form alternate AT‐rich DNA (d[5′‐G₂(AT)₆C_2‐3′]) > A form GC‐rich DNA (d[5′‐A₂G₆C₆T₂‐3′]), demonstrating the preference of ligand 1 for B* form DNA. © 2013 Wiley Periodicals, Inc. Biopolymers 101: 720–732, 2014.     

A study of the interactions that stabilize DNA frayed wires

Oligodeoxyribonucleotides (ODNs) with long, terminal runs of consecutive guanines, and either a dA or dT tract at the other end form higher-order structures called DNA frayed wires. These aggregates self-assemble into species consisting of 2, 3, 4, 5, … associated strands. Some of the remarkable features of these structures are their extreme thermostability and resistance to chemical denaturants and nucleases. However, the nature of the molecular interactions that stabilize these structures remains unclear. Based on dimethyl sulfate (DMS) methylation results, our group previously proposed DNA frayed wires to be a unique set of nucleic-acid assemblies in which the N7 of guanine does not participate in the guanine–guanine interactions. To probe the hydrogen bonding involved in the stabilization of d(A₁₅G₁₅) frayed wires, we used Raman spectroscopy in which the DNA sample is held in photonic crystal fibers. This technique significantly enhances the signals thus allowing the use of very low laser power. Based on our results for d(A₁₅G₁₅) and those of incorporating the isoelectronic guanine analog pyrazolo[3,4,-d]pyrimidine or PPG, into a frayed wire-forming sequence, we provide evidence that these structures are based on the G-quadruplex model. Furthermore, from the Raman spectrum, we observed markers that are consistent with the presence of deoxyguanosine residues in the syn conformation, this suggests the presence of anti-parallel G-quadruplexes. To identify the species that contain syn guanine residues, we used circular dichroism and gel electrophoresis to study an ODN in which all of the guanine residues were brominated, d(A₁₅^8-BrG₁₅). In the presence of potassium, d(A₁₅^8-BrG₁₅) forms what appears to be an anti-parallel dimeric G-quadruplex. To our knowledge, this is the first report of a DNA sequence having all its guanine residues replaced by 8-bromo-guanine and maintaining its ability to form a G-quadruplex structure.     

Solution structure of a DNA quadruplex containing ALS and FTD related GGGGCC repeat stabilized by 8-bromodeoxyguanosine substitution

A prolonged expansion of GGGGCC repeat within non-coding region of C9orf72 gene has been identified as the most common cause of familial amyotrophic lateral sclerosis (ALS) and frontotemporal dementia (FTD), which are devastating neurodegenerative disorders. Formation of unusual secondary structures within expanded GGGGCC repeat, including DNA and RNA G-quadruplexes and R-loops was proposed to drive ALS and FTD pathogenesis. Initial NMR investigation on DNA oligonucleotides with four repeat units as the shortest model with the ability to form an unimolecular G-quadruplex indicated their folding into multiple G-quadruplex structures in the presence of K⁺ ions. Single dG to 8Br-dG substitution at position 21 in oligonucleotide d[(G₄C₂)₃G₄] and careful optimization of folding conditions enabled formation of mostly a single G-quadruplex species, which enabled determination of a high-resolution structure with NMR. G-quadruplex structure adopted by d[(G₄C₂)₃GG^BrGG] is composed of four G-quartets, which are connected by three edgewise C-C loops. All four strands adopt antiparallel orientation to one another and have alternating syn-anti progression of glycosidic conformation of guanine residues. One of the cytosines in every loop is stacked upon the G-quartet contributing to a very compact and stable structure.     

Tetraplex Formation of d(GGGGGTTTTT): 1H NMR Study in Solution

Abstract

The oligonucleotide d(G₅T₅) can in principle form a fully matched duplex with G · T pairing and/or a tetraplex. Non-denaturing gel electrophoresis, circular dichroism and NMR experiments show that the tetraplex is exclusively formed by this oligomer in solution. In the presence of its complementary strand d(A₅C₅) at low temperature, d(G₅T₅) forms the tetraplex over the normally expected Watson-Crick duplex. However, when d(G₅T₅) and d(A₅C₅) are mixed together in equimolar amounts and heated for several minutes at 85°C, and then allowed to cool, the product was essentially the Watson-Crick duplex. The lack of resolution in the 500 MHz ¹H NMR spectra and the presence of extensive spin diffusion do not allow us to derive a quantitative structure for the tetraplex from the NMR data. However, we find good qualitative agreement between the NOESY and MINSY data and a theoretically derived stereochemically sound structure in which the G's and T's are part of a parallel tetraplex.     

A Single Carbocyclic Nucleotide Substitution in a 12mer DNA Gives a Hoogsteen Basepaired Duplex (Till 38°C) and a Hairpin (Till 65°C). A 600 MHz NMR Spectroscopic Study

Abstract

The impact of intramolecular stereoelectronic effects has been examined by comparison of the solution structures of natural oligo-DNA duplex, 5′(¹C²G³C⁴G⁵A⁶A⁷T⁸T⁹C¹⁰G¹¹C¹²G)₂ ³′, and its carbocyclic-nucleotide analogues in which the pentose sugar in 2′-dA residue is replaced with its carbocyclic counterpart (i.e. 2′-deoxyaristeromycin). Based on the NMR evidences, it has been shown, that 2′-deoxyaristeromycin analog exists in a dynamic equilibrium between the two forms of duplexes, one with W-C bp and the second with Hoogsteen bp in ca 1:1 ratio at lower temperature (below 35°C) and as hairpin at higher temperature (from ～40° – 60°C).     

Effect ofmutY andmutM/fpg-1 mutations on starvation-associated mutation inEscherichia coli: implications for the role of 7,8-dihydro-8-oxoguanine

MutY specifies a DNA glycosylase that removes adenines unnaturally paired with various bases including oxidized derivatives of guanine, such as 7,8-dihydro-8-oxoguanine (8-oxoG). The rate of mutation in starvedEscherichia coli cells is markedly raised inmutY mutants defective in this glycosylase. As predicted, the mutations produced include G to T transversions. Bacteria carryingmutM orfpg-1 mutations (defective in Fapy glycosylase, which removes oxidized guanine residues such as 8-oxoG) show little or no enhancement of mutation under starvation conditions. When present together withmutY, however,mutM clearly further enhances the rate of mutation in starved cells. Plasmids resulting in overproduction of MutY or Fapy glycosylases reduce the rate of mutation in starved cells. We conclude that, in non-growing bacteria, oxidized guanine residues, including 8-oxoG, constitute an important component of spontaneous mutation. Addition of catalase to the plates did not reduce the mutant yield, indicating that extracellular hydrogen peroxide is not involved in the production of the premutational damage. Singlet oxygen, known to give rise to 8-oxoG, may be the ultimate oxidative species.     

CD studies of double-stranded polydeoxynucleotides composed of repeating units of contiguous homopurine residues

Double-stranded synthetic polydeoxynucleotides of the general form poly[d(G_nC_n)] · poly[d(G_nC_n)], poly[d(G_nC)] · poly[d(GC_n)], and poly[d(A_nT_n)] · poly[d(A_nT_n)] have been synthesized. When n = 4 or larger, the CD spectra of polymers of the form poly[d(G_nC_n)] · poly[d(G_nC_n)] or poly[d(G_nC)] · poly[d(GC_n)] closely resemble the spectrum of poly[dG] · poly[dC], suggesting that a string of four continguous guanosine residues is sufficient to induce a conformation resembling that of the polypurine · polypyrimidine. With polymers of the form poly[d(A_nT_n)] · poly[d(A_nT_n)], however, the CD spectrum only gradually approaches that of poly[dA] · poly[dT].     

Structural basis for the lack of opposite base specificity of Clostridium acetobutylicum 8-oxoguanine DNA glycosylase

7,8-Dihydro-8-oxoguanine (8-oxoG) is the major oxidative product of guanine and the most prevalent base lesion observed in DNA molecules. Because 8-oxoG has the capability to form a Hoogsteen pair with adenine (8-oxoG:A) in addition to a normal Watson–Crick pair with cytosine (8-oxoG:C), this lesion can lead to a G:C → T:A transversion after replication. However, 8-oxoG is recognized and excised by the 8-oxoguanine DNA glycosylase (Ogg) of the base excision repair pathway. Members of the Ogg1 family usually display a strong preference for a C opposite the lesion. In contrast, the atypical Ogg1 from Clostridium actetobutylicum (CacOgg) can excise 8-oxoG when paired with either one of the four bases, albeit with a preference for C and A. Here we describe the first high-resolution crystal structures of CacOgg in complex with duplex DNA containing the 8-oxoG lesion paired to cytosine and to adenine. A structural comparison with human OGG1 provides a rationale for the lack of opposite base specificity displayed by the bacterial Ogg.     

Effect ofmutY andmutM/fpg-1 mutations on starvation-associated mutation inEscherichia coli: implications for the role of 7,8-dihydro-8-oxoguanine

MutY specifies a DNA glycosylase that removes adenines unnaturally paired with various bases including oxidized derivatives of guanine, such as 7,8-dihydro-8-oxoguanine (8-oxoG). The rate of mutation in starvedEscherichia coli cells is markedly raised inmutY mutants defective in this glycosylase. As predicted, the mutations produced include G to T transversions. Bacteria carryingmutM orfpg-1 mutations (defective in Fapy glycosylase, which removes oxidized guanine residues such as 8-oxoG) show little or no enhancement of mutation under starvation conditions. When present together withmutY, however,mutM clearly further enhances the rate of mutation in starved cells. Plasmids resulting in overproduction of MutY or Fapy glycosylases reduce the rate of mutation in starved cells. We conclude that, in non-growing bacteria, oxidized guanine residues, including 8-oxoG, constitute an important component of spontaneous mutation. Addition of catalase to the plates did not reduce the mutant yield, indicating that extracellular hydrogen peroxide is not involved in the production of the premutational damage. Singlet oxygen, known to give rise to 8-oxoG, may be the ultimate oxidative species.     

Structure-specific binding of [Co(phen)2(HPIP)] to a DNA duplex containing sheared G:A mismatch base pairs

The binding of a Co(III) complex to the decanucleotide d(CCGAATGAGG)₂ containing two pairs of G:A mismatches was studied by 2D-NMR, UV absorption, and molecular modeling. NMR investigations indicate that racemic [Co(phen)₂(HPIP)]Cl₃ [HPIP = 2-(2-hydroxyphenyl) imidazo [4,5-f][1,10] phenanthroline] binds the decanucleotide by intercalation: the HPIP ligand selectively inserts between the stacked bases from the minor groove at the terminal regions and from the major groove at the sheared region. Further, molecular modeling revealed that the recognition shows strong enantioselectivity: the Λ-isomer preferentially intercalates into the T₆G₇:A₅A₄ region from the DNA major groove, while Δ-isomer favors the terminal C₁C₂:G₁₀G₉ region and intercalates from the minor groove. Detailed energy analysis suggests that the steric interaction, especially the electrostatic effect, is the primary determinants of the recognition event. Melting experiments indicate that binding stabilizes the DNA duplex and increases the melting temperature by 9.5 °C. The intrinsic binding constant of the complex to the mismatched duplex was determined to be 3.5 × 105 M⁻¹.