Circular dichroism spectroscopy reveals invariant conformation of guanine runs in DNA

We demonstrate that the characteristic circular dichroism (CD) features of the parallel-stranded DNA tetraplex of d(G4), especially the strong band at 260 nm, are characteristic for the B and A forms of the antiparallel duplex of d(C4G4). Hence, this band evidently originates from intrastrand guanine-guanine stacking, which is therefore very similar in the duplex and tetraplex DNA. In addition, the same type of the CD spectrum is provided by the ordered single strand of d(GA)10. This observation suggests that the ordered single strand of d(GA)10 is stabilized by a core of guanines stacked like in the parallel tetraplex. This view is used to start the modeling of the molecular structure of the ordered d(GA)10 single strand. Our studies suggest that guanine itself is strong enough to stabilize various secondary structures of DNA, which is a property relevant to thinking about the origin and evolution of molecular replicators.     

A-like guanine-guanine stacking in the aqueous DNA duplex of d(GGGGCCCC)

We have used CD spectroscopy, NMR spectroscopy and unrestrained molecular dynamics to study conformational properties of a DNA duplex formed by the self-complementary octamer d(GGGGCCCC). Its unusual CD spectrum contains features indicating A-like stacking of half of the bases, whereas the other half stack in a B-like fashion. Unrestrained molecular dynamics simulations converged to a stable B-like double-helix of d(GGGGCCCC). However, the double-helix contained a central hole whose size was half of that occurring in structure A. In the canonical structure B, the hole does not exist at all because the base-pairs cross the double-helix centre. The cytosine bases were stacked in the duplex of d(GGGGCCCC) as in structure B, while stacking of the guanine bases displayed features characteristic for structure A. NMR spectroscopy revealed that the A-like guanine-guanine stacking was accompanied by an increased tendency of the deoxyribose rings attached to the guanine bases to be puckered in an A-like fashion. Otherwise, the duplex of d(GGGGCCCC) showed no clash, no bend and no other significant deviation from structure B. The present analysis demonstrates a remarkable propensity of the guanine runs to stack in an A-like fashion even within the B-DNA framework. This property explains why the oligo(dG). oligo(dC) tracts switch into structure A so easily. Secondly, this property may influence replication, because structure A is replicated more faithfully than structure B. Thirdly, the oligo(dG) runs might have played an important role in early evolution, when DNA took on functions that originally evolved on RNA. Fourthly, the present study extends the vocabulary of DNA secondary structures by the heteronomous duplex of d(GGGGCCCC) in which the B-like strand of oligo(dC) is bound to the A-like strand of oligo(dG).     

Guanine tetraplex formation by short DNA fragments containing runs of guanine and cytosine.

Using CD spectroscopy, guanine tetraplex formation was studied with short DNA fragments in which cytosine residues were systematically added to runs of guanine either at the 5' or 3' ends. Potassium cations induced the G-tetraplex more easily with fragments having the guanine run at the 5' end, which is just an opposite tendency to what was reported for (G+T) oligonucleotides. However, the present (G+C) fragments simultaneously adopted other conformers that complicated the analysis. We demonstrate that repeated freezing/thawing, performed at low ionic strength, is a suitable method to exclusively stabilize the tetraplex in the (G+C) DNA fragments. In contrast to KCl, the repeated freeze/thaw cycles better stabilized the tetraplex with fragments having the guanine run on the 3' end. The tendency of guanine blocks to generate the tetraplex destabilized the d(G5).d(C5) duplex whose strands dissociated, giving rise to a stable tetraplex of (dG5) and single-stranded (dC5). In contrast to d(G3C3) and d(G5C5), repeated freezing/thawing induced the tetraplex even with the self-complementary d(C3G3) or d(C5G5); hence the latter oligonucleotides preferred the tetraplex to the apparently very stable duplex. The tetraplexes only included guanine blocks while the 5' end cytosines interfered neither with the tetraplex formation nor the tetraplex structure.     

Raman spectra of single crystals of r(GCG)d(CGC) and d(CCCCGGGG) as models for A DNA, their structure transitions in aqueous solution, and comparison with double-helical poly(dG).poly(dC)

The self-complementary oligonucleotides [r(CGC)d(CGC)]2 and [d(CCCCGGGG)]2 in single-crystal and solution forms have been investigated by Raman spectroscopy. Comparison of the Raman spectra with results of single-crystal X-ray diffraction and with data from polynucleotides permits the identification of a number of Raman frequencies diagnostic of the A-helix structure for GC sequences. The guanine ring frequency characteristic of C3'-endo pucker and anti base orientation is assigned at 668 +/- 2 cm-1 for both dG and rG residues of the DNA/RNA hybrid [r(GCG)d(CGC)]2. The A-helix backbone of crystalline [r(GCG)d(CGC)]2 is altered slightly in the aqueous structure, consistent with the conversion of at least two residues to the C2'-endo/anti conformation. For crystalline [d(CCCCGGGG)]2, the Raman and X-ray data indicate nucleosides of alternating 2'-endo-3'-endo pucker sandwiched between terminal and penultimate pairs of C3'-endo pucker. The A-A-B-A-B-A-A-A backbone of the crystalline octamer is converted completely to a B-DNA fragment in aqueous solution with Raman markers characteristic of C2'-endo/anti-G (682 +/- 2) and the B backbone (826 +/- 2 cm-1). In the case of poly(dG).poly(dC), considerable structural variability is detected. A 4% solution of the duplex is largely A DNA, but a 2% solution is predominantly B DNA. On the other hand, an oriented fiber drawn at 75% relative humidity reveals Raman markers characteristic of both A DNA and a modified B DNA, not unlike the [d-(CCCCGGGG)]2 crystal. A comparison of Raman and CD spectra of the aqueous [d(CCCCGGGG)]2 and poly(dG).poly(dC) structures suggests the need for caution in the interpretation of CD data from G clusters in DNA.     

Induction of B-A transitions of deoxyoligonucleotides by multivalent cations in dilute aqueous solution.

Circular dichroism (CD) spectra of d(CCCCGGGG) in the presence of Co(NH3)6(3+) are very similar to spectra of r(CCCCGGGG). In contrast, B-form characteristics are observed for d(CCCCGGGG) in the presence of Na+ and Mg2+, even at high salt concentrations. Spermidine induces modest changes of the CD of d(CCCCGGGG). The NMR chemical shifts of the nonexchangeable protons of d(CCCCGGGG) in the absence and presence of Co(NH3)6(3+) were assigned by proton two-dimensional (2D) NOESY and COSY measurements. The chemical shifts of the GH8 protons of d(CCCCGGGG) move upfield upon titration with Co(NH3)6Cl3. The sums of the sugar H1' coupling constants decrease with added Co(NH3)6Cl3. Cross peak intensities in the 2D proton NOESY spectra show a transformation from B-DNA to A-DNA characteristics upon the addition of Co(NH3)6Cl3. The temperature-dependent 59Co transverse and longitudinal relaxation rates demonstrate that Co(NH3)6(3+) is site-bound to the oligomer. Such localization is not a general feature of Co(NH3)6(3+) binding to oligonucleotides. 59Co NMR relaxation and CD measurements demonstrate chiral discrimination by d(CCCCGGGG) for the two stereoisomers of Co(en)3(3+). Both stereoisomers bind tightly as judged by 59Co NMR, and both cause large (but nonequivalent) changes in the CD of this oligomer.     

Binding of meso-tetrakis(N-methylpyridinium-4-yl)porphyrin to AT oligomers: effect of chain length and the location of the porphyrin stacking

Circular dichroism (CD) spectra of meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (TMPyP) that are associated with various duplex and triplex AT oligomers were investigated in this study. A strong positive CD was apparent for both the TMPyP complexed with duplex d[(A-T)(12)](2), d(A)(12).d(T)(12) and triplex d(A)(12).d[(T)(12)](2) at a low mixing ratio. As the mixing ratio increased, bisignate excitonic CD was produced for TMPyP complexed with duplexes, whereas the positive CD signal remained the same for the TMPyP-d(A)(12).d[(T)(12)](2) complex. This difference in the CD spectrum in the presence of duplex and triplex oligomers indicates that the moderate stacking of TMPyP occurs at the major groove of the duplex and the monomeric binding occurs in (or near) the minor groove. When TMPyP forms a complex with duplex d[(A-T)(6)](2) only excitonic CD was observed, even at a very low mixing ratio. Therefore, at least seven or more basepairs are required for TMPyP to exhibit a monomeric CD spectrum. After close analysis of the CD spectrum, the TMPyP-poly[d(A-T)(2)] complex could be explained by a combination of the CD spectrum of the monomeric, moderately stacked, and extensively stacked TMPyP.     

Fold-back tetraplex DNA species in DNase I-resistant DNA isolated from HeLa cells

A DNase I-resistant DNA species has been isolated and purified from HeLa cells by gel electrophoresis. Our studies indicate that the DNase I-resistant DNA species was about 40-60 bp fragment sizes responding to double-strand DNA marker and has higher guanine content. The image of AFM showed that this species has been assumed to be tetraplex structure according to its apparent width and height. Its CD, UV spectrum also exhibited characteristics similar to some tetraplex structure, which was different from the standard duplex DNA. 32P-labeled probes (TTAGGG)4 and 5'-TGGGGAGGGTGGGGAGGGTGGGGAAGG-3' could be hybridized to purified DNase I-resistant species. All results suggest that the DNase I-resistant DNA species have at least two components, which adopt an intrastrand fold-back DNA tetraplex. Their sequences were similar to human telomere and human c-myc locus (NHE), respectively.     

Tetrahelical forms of the fragile X syndrome expanded sequence d(CGG)(n) are destabilized by two heterogeneous nuclear ribonucleoprotein-related telomeric DNA-binding proteins

Formations of hairpin and tetrahelical structures by the trinucleotide repeat sequence d(CGG)(n) might contribute to its expansion in fragile X syndrome. Here we show that tetraplex structures of d(CGG)(n) are destabilized by two mammalian heterogeneous nuclear ribonucleoprotein-related tetraplex telomeric DNA-binding and -stabilizing proteins, quadruplex telomeric DNA-binding protein 42 (qTBP42) (Sarig, G., Weisman-Shomer, P., Erlitzki, R., and Fry, M. (1997) J. Biol. Chem. 272, 4474-4482) and unimolecular quadruplex telomeric DNA-binding protein 25 (uqTBP25) (Erlitzki, R., and Fry, M. (1997) J. Biol. Chem. 272, 15881-15890). Blunt-ended and 3'-tailed or 3'- and 5'-tailed bimolecular tetraplex structures of d(CGG)(n) and guanine-sparse 20-/46-mer partial DNA duplex were progressively destabilized by increasing amounts of qTBP42 or uqTBP25 in time-dependent and ATP- or Mg(2+)-independent reactions. By contrast, tetraplex structures of telomeric and IgG sequences or guanine-rich double-stranded DNA resisted destabilization by qTBP42 or uqTBP25. Increased stability of tetraplex d(CGG)(n) in the presence of K(+) or Na(+) ions or at lowered reaction temperature diminished the destabilizing activity of uqTBP25. The contrasting stabilization of tetraplex telomeric DNA and destabilization of tetraplex d(CGG)(n) by qTBP42 and uqTBP25 suggested that sequence or structural differences between these tetraplexes might serve as cues for the differential stabilizing/destabilizing activities.     

Circular dichroism spectroscopy of conformers of (guanine + adenine) repeat strands of DNA

(Guanine+adenine) strands of DNA are known to associate into guanine tetraplexes, homodimerize into parallel or antiparallel duplexes, and fold into a cooperatively melting single strand resembling the protein alpha helix. Using CD spectroscopy and other methods, we studied how this conformational polymorphism depended on the primary structure of DNA. The study showed that d(GGGA)(5) and d(GGA)(7) associated into homoduplexes at low salt or in the presence of LiCl but were prone to guanine tetraplex formation, especially in the presence of KCl. In addition, they yielded essentially the same CD spectrum in the presence of ethanol as observed with the ordered single strand of d(GA)(10). Strands of d(GA)(10), d(GGAA)(5), d(GAA)(7), and d(GAAA)(5) associated into homoduplexes in both LiCl and KCl solutions, but not into guanine tetraplexes. d(GAAA)(5) and d(GAA)(7) further failed to form the single-stranded conformer in aqueous ethanol. Adenine protonation, however, stabilized the single-stranded conformer even in these adenine-rich fragments. The ordered single strands, homoduplexes as well as the guanine tetraplexes, all provided strikingly similar CD spectra, indicating that all of the conformers shared similar base stacking geometries. The increasing adenine content only decreased the conformer thermostability.     

Tetraplex formation of d(GGGGGTTTTT): 1H NMR study in solution.

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 degrees 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.     

N-acetoxy-2-acetylaminofluorene modification of a deoxyoligonucleotide duplex.

The carcinogen N-acetoxy-2-acetylaminofluorene was reacted with d (CCACGCACC) to form a covalent adduct with attachment at the single guanine. The sample was purified, mixed 1:1 with d (GGTGCGTGG) and studied by thermal denaturation experiments. The Tm for the mixture was 35 +/- 3 degrees C, consistent with duplex formation. The method of continuous variation shows that the modified oligomer, d (CCACGAAFCACC), forms a 1:1 duplex with d (GGTGCGTGG). Circular dichroism spectra also indicate the formation of a duplex and suggest that the modified duplex has a left-handed conformation. Addition of the intercalating drug ethidium alters the CD spectrum of the modified duplex, resulting in a CD spectrum similar to that of ethidium bound to right-handed DNA.     

Dinucleotides as simple models of the base stacking-unstacking component of DNA ‘breathing’ mechanisms

Regulatory protein access to the DNA duplex ‘interior’ depends on local DNA ‘breathing’ fluctuations, and the most fundamental of these are thermally-driven base stacking-unstacking interactions. The smallest DNA unit that can undergo such transitions is the dinucleotide, whose structural and dynamic properties are dominated by stacking, while the ion condensation, cooperative stacking and inter-base hydrogen-bonding present in duplex DNA are not involved. We use dApdA to study stacking-unstacking at the dinucleotide level because the fluctuations observed are likely to resemble those of larger DNA molecules, but in the absence of constraints introduced by cooperativity are likely to be more pronounced, and thus more accessible to measurement. We study these fluctuations with a combination of Molecular Dynamics simulations on the microsecond timescale and Markov State Model analyses, and validate our results by calculations of circular dichroism (CD) spectra, with results that agree well with the experimental spectra. Our analyses show that the CD spectrum of dApdA is defined by two distinct chiral conformations that correspond, respectively, to a Watson–Crick form and a hybrid form with one base in a Hoogsteen configuration. We find also that ionic structure and water orientation around dApdA play important roles in controlling its breathing fluctuations.     

A fractal model of chromosomes and chromosomal DNA replication

With the aim of clarifying topological problems involved in the process of chromosomal DNA replication, a fractal model of chromosomes was built based on the assumption that a part of a chromosome, e.g. a radial loop, is similar in shape to a whole chromosome and each radial loop represents structures in the lower-order organization (an assumption of self-similarity). Several other assumptions used include (i) one continuous DNA fiber makes a whole chromosome (a unineme hypothesis), (ii) in situ DNA exists in the form of a double duplex or a tetraplex which is made of two duplex DNAs, although a duplex DNA may appear transiently in S-phase (multi-strandedness hypothesis) and (iii) torsional stress on a DNA fiber causes the fiber to supercoil and thus stabilizes chromosome structure (torque-based stabilization). This model allowed to calculate of a fractal dimension of a representative metaphase chromosome (e.g. d = 2.34), to predict the mode of replication of double duplex and to furnish a topological basis for the decondensation unit hypothesis. It must also be admitted that all the arguments in this report except for the possible existence of split telomeres hold true without assuming a tetraplex organization of chromosomes. Implications of this model was discussed and the importance of the fractal dimension as a measure of chromatin condensation stressed.     

Tetraplex structure of fission yeast telomeric DNA and unfolding of the tetraplex on the interaction with telomeric DNA binding protein Pot1

To understand the regulation mechanism of fission yeast telomeric DNA, we analysed the structural properties of Gn: d(GnTTAC) (n=2-6) and 4Gn: d(GnTTAC)4 (n=3 and 4), and their interaction with the single-stranded telomeric DNA binding domain of telomere-binding protein Pot1 (Pot1DBD). G4, G5 and G6 formed a parallel tetraplex in contrast with no tetraplex formation by G2 and G3. Also, 4G4 adopted only an antiparallel tetraplex in spite of a mixture of parallel and antiparallel tetraplexes of 4G3. The variety of tetraplex structures was governed by the number of consecutive guanines in a single copy and the number of repeats. The antiparallel tetraplex of 4G4 became unfolded upon the interaction with Pot1DBD. The interaction with mutant Pot1DBD proteins revealed that the ability to unfold the antiparallel tetraplex was strongly correlated with the specific binding affinity for the single-stranded telomeric DNA. The result suggests that the decrease in the free single strand upon the complex formation with Pot1DBD may shift the equilibrium from the tetraplex to the single strand, which may cause the tetraplex unfolding. Considering that the antiparallel tetraplex inhibits telomerase-mediated telomere elongation, we conclude that the ability of Pot1 to unfold the antiparallel tetraplex is required for telomerase-mediated telomere regulation.     

The vacuum UV CD spectra of G.G.C triplexes.

Vacuum UV circular dichroism (CD) spectra were measured down to 175 nm for d(C)10, d(G)10, the d(G)10.d(C)10 duplex, and the d(G)10.d(G)10.d(C)10 triplex. A CD difference spectrum was calculated for d(G)10.d(C)10 giving the change in CD induced by forming the duplex from d(G)10 and d(C)10. The d(G)10.d(G)10.d(C)10 CD difference spectrum gave the CD induced by triplex formation from binding of d(G)10 to the d(G)10.d(C)10 duplex. In the near-UV, the d(G)10.d(C)10 and d(G)10.d(G)10.d(C)10 difference spectra resembled the difference spectrum for poly[r(G).r(C)] (Biopolymers 29, 325-333). This similarity may be an indication of similar purine base stacking. The d(G)10.d(G)10.d(C)10 vacuum UV difference spectrum had a negative band at 195 nm and a positive band at 180 nm, making it similar to difference spectra for homopolymer triplexes containing T.A.T and U.A.U triplets (Nucl. Acids Res. 19, 2275-2280). The appearance of these bands in difference spectra should be good indicators of triplex formation. The complementary oligonucleotides c-mycI d(CCCCACCCTCCC) and c-mycII d(GGGAGGGTGGGG) are part of the regulatory sequences of the human c-myc gene. G.G.C rich triplexes formed by binding c-mycII or c-mycIII d(GGGGTGGGTGGG) to the c-mycI.c-mycII duplex had CD difference spectra similar to that of d(G)10.d(G)10.d(C)10 in both the vacuum UV and near UV regions, indicating similar triplet structures.     

The crystal structure of d(CCCCGGGG): a new A-form variant with an extended backbone conformation

The crystal structure of d(CCCCGGGG) has been determined at a resolution of 2.25 A. The oligomers crystallize as A-DNA duplexes occupying crystallographic two-fold axes. The backbone conformation is, in general, similar to that observed in previously reported crystal structures of A-DNA fragments, except for the central linkage, where it adopts an extended structure resulting from all trans conformation at the P-O5'-C5'-C4' bonds. This type of conformation facilitates interstrand stacking between the guanines at the C-G site. The local helix twist at this step is very small (25 degrees) compared to an overall average of 33.5 degrees. The unique structure of the C-G base-pair step, namely the extended backbone and the distinct stacking geometry, may be an important feature in the recognition mechanism between double-stranded DNA molecules and restriction endonucleases such as Msp I, which cuts the sequence CCGG very specifically with a rate unaffected by neighboring base pairs.     

Duplex-tetraplex equilibrium between a hairpin and two interacting hairpins of d(A-G)10 at neutral pH.

d(A-G)10 forms two helical structures at neutrality, at low ionic strength a single-hairpin duplex, and at higher ionic strength a double-hairpin tetraplex. An ionic strength-dependent equilibrium between these forms is indicated by native PAGE, which also reveals additional single-stranded species below 0.3 M Na+, probably corresponding to partially denatured states. The equilibrium also depends upon oligomer concentration: at very low concentrations, d(A-G)10 migrates faster than the random coil d(C-T)10, probably because it is a more compact single hairpin; at high concentrations, it co-migrates with the linear duplex d(A-G)10 x d(C-T)10, probably because it is a two-hairpin tetraplex. Molecular weights measured by equilibrium sedimentation in 0.1 M Na+, pH 7, reveal a mixture of monomer and dimer species at 1 degree C, but only a monomer at 40 degrees C; in 0.6 M Na+, pH 7, only a dimer species is observed at 4 degrees C. That the single- and double-stranded species are hairpin helices, is indicated by preferential S1 nuclease cleavage at the center of the oligomer(s), i.e., the loop of the hairpin(s). The UV melting transition below 0.3 M Na+ or K+, exhibits a dTm/dlog[Na+/K+] of 33 or 36 degrees C, respectively, consistent with conversion of a two-hairpin tetraplex to a single-hairpin duplex with extrahelical residues. When [Na+/K+] > or = 0.3 M, dTm/dlog [Na+/K+] is 19 or 17 degrees C, respectively, consistent with conversion of a two-hairpin tetraplex directly to single strands. A two-hairpin structure stabilized by G-tetrads is indicated by differential scanning calorimetry in 0.15 M Na+/5 mM Mg2+, with deltaH of formation per mole of the two-hairpin tetraplex of -116.9 kcal or -29.2 kcal/mol of G-tetrad.     

Fission yeast telomeric DNA binding protein Pot1 has the ability to unfold tetraplex structure of telomeric DNA

To understand the regulation mechanism of fission yeast telomeric DNA, we analyzed the structural properties of 4Gn: d(G(n)TTAC)(4) (n = 3, 4) and their interaction with the single-stranded telomeric DNA binding domain of telomere-binding protein Pot1 (Pot1DBD). 4G4 adopted only an antiparallel tetraplex in spite of a mixture of parallel and antiparallel tetraplexes of 4G3. The antiparallel tetraplex of 4G4 became unfolded upon the interaction with Pot1DBD. Considering that the antiparallel tetraplex inhibits telomerase-mediated telomere elongation, we conclude that the ability of Pot1 to unfold the antiparallel tetraplex is required for telomerase-mediated telomere regulation.     

The Crystal Structure of d(CCCCGGGG): A New A-Form Variant with an Extended Backbone Conformation

Abstract

The crystal structure of d(CCCCGGGG) has been determined at a resolution of 2.25Å. The oligomers crystallize as A-DNA duplexes occupying crystallographic two-fold axes. The backbone conformation is, in general, similar to that observed in previously reported crystal structures of A-DNA fragments, except for the central linkage, where it adopts an extended structure resulting from all trans conformation at the P-05′-C5′-C4′ bonds. This type of conformation facilitates interstrand stacking between the guanines at the C-G site. The local helix twist at this step is very small (25°) compared to an overall average of 33.5°. The unique structure of the C-G base-pair step, namely the extended backbone and the distinct stacking geometry, may be an important feature in the recognition mechanism between double- stranded DNA molecules and restriction endonucleases such as Msp I, which cuts the sequence CCGG very specifically with a rate unaffected by neighboring base pairs.