Z → B transition in poly[d(G-m5C)2] induced by interaction with 4′,6-diamidino-2-phenylindole

The Z form of poly[d(G-m⁵C)₂], in presence of Mg²⁺ ion, is found to be transformed into B form upon interaction with 4′,6-diamidino-2-phenylindole (DAPI). The Z → B transformation is complete at a mixing ratio of about 0.07 DAPI per DNA base pairs, i.e., each DAPI molecule may be related to the conversion of 6–7 base pairs. An interaction between DAPI and poly[d(G-m⁵C)₂] in its Z form at low drug: DNA ratios is suggested from optical dichroism and time-resolved luminescence anisotropy results. The spectroscopic behaviour of DAPI indicates that the Z conformation of DNA does not provide normal binding sites for DAPI, such as groove or intercalation sites, but that the initial association may be of external nature. © 1993 John Wiley & Sons, Inc.     

Studies on interaction between poly(L-lysine) and DNA of varied G + C contents

Interaction between polylysine and DNA's of varied G + C contents was studied using thermal denaturation and circular dichroism (CD). For each complex there is one melting band at a lower temperature t_m, corresponding to the helix–coil transition of free base pairs, and another band at a higher temperature t′_m, corresponding to the transition of polylysine-bound base pairs. For free base pairs, with natural DNA's and poly(dA-dT) a linear relation is observed between the t_m and the G + C content of the particular DNA used. This is not true with poly(dG)·poly(dC), which has a t_m about 20°C lower than the extrapolated value for DNA of 100% G + C. For polylysine-bound base pairs, a linear relation is also observed between the t′_m and the G + C content of natural DNA's but neither poly(dA-dT) nor poly(dG)·poly(dC) complexes follow this relationship. The dependence of melting temperature on composition, expressed as dt_m/dX_G·C, where X_G·C is the fraction of G·C pairs, is 60°C for free base pairs and only 21°C for polylysine-bound base pairs. This reduction in compositional dependence of T_m is similar to that observed for pure DNA in high ionic strength. Although the t′_m of polylysine-poly(dA-dT) is 9°C lower than the extrapolated value for 0% G + C in EDTA buffer, it is independent of ionic strength in the medium and is equal to the t_m⁰ extrapolated from the linear plot of t_m against log Na⁺. There is also a noticeable similarity in the CD spectra of polylysine· and polyarginine·DNA complexes, except for complexes with poly(dA-dT). The calculated CD spectrum of polylysine-bound poly(dA-dT) is substantially different from that of polyarginine-bound poly(dA-dT).     

Fine structure of DNA melting curves.

Theoretical calculations predict that the differential melting curves for random polynucleotide sequences having lengths up to several tens of thousands of base pairs have a clear-cut fine structure. This structure appears in the form of multiple narrow peaks 0.3–0.4°C wide on the bell shaped main curve. The differential melting curves have different shapes for different specific sequences. The theory also predicts the disappearance of the fine structure when the length of the sequence increases and when circular, covalently closed DNA is considered instead of the open structure. The predictions of the theory were confirmed by the measurements of differential melting curves for open and covalently closed circular forms of DNA for PM2 phage (N = 10⁴ base pairs) and also for other phage DNA's of different length: T7 (N = 3.8 × 10⁴); S_D (N = 9.2 × 10⁴); T2 (N = 17 × 10⁴). It was shown that the effect of fine structure results mainly from the cooperative melting out of DNA regions 300–500 base pairs long.     

Light scattering studies of supercoiled and nicked DNA

Static and dynamic light scattering measurements were made of solutions of pGem1a plasmids (3730 base pairs) in the relaxed circular (nicked) and supercoiled forms. The static structure factor and the spectrum of decay modes in the autocorrelation function were examined in order to determine the salient differences between the behaviors of nicked DNA and supercoiled DNA. The concentrations studied are within the dilute regime, which is to say that the structure and dynamics of an isolated DNA molecule were probed. Static light scattering measurements yielded estimates for the molecular weight M, second virial coefficient A₂, and radius of gyration R_G. For the nicked DNA, M = (2.8 ± 0.4) × 10⁶g/mol, A₂ = (0.9 ± 0.2) × 10⁻³ mol cm³/g², and R_G = 90 ± 3 nm were obtained. For the supercoiled DNA, M = (2.5 ± 0.4) × 10⁶ g/mol, A₂ = (1.2 ± 0.2) × 10⁻³ mol cm³/g², and R_G = 82 ± 2.5 nm were obtained. The static structure factors for the nicked and supercoiled DNA were found to superpose when they were scaled by the radius of gyration. The intrinsic stiffness of DNA was evident in the static light scattering data. Homodyne intensity autocorrelation functions were collected for both DNAs at several angles, or scattering vectors. At the smallest scattering vectors the probe size was comparable to the longest intramolecular distance, while at the largest scattering vectors the probe size was smaller than the persistence length of the DNA. Values of the self-diffusion coefficients D were obtained from the low-angle data. For the nicked DNA, D = (2.9 ± 0.3) × 10⁻⁸ cm²/s, and for the supercoiled DNA, D = (4.11 ± 0.21) × 10⁻⁸ cm²/s. The contribution to the correlation function from the internal dynamics of the DNA was seen to result in a strictly bimodal decay function. The rates of the faster mode Γ_int, reached plateau values at low angles. For the nicked DNA, Γ_int = 2500 ± 500 s⁻¹, and for the supercoiled DNA, Γ_int = 5000 ± 500 s⁻¹. These rates correspond to the slowest internal relaxation modes of the DNAs. The dependence of the relaxation rates on scattering vector was monitored with the aid of cumulants analysis and compared with theoretical predictions for the semiflexible ring molecule. The internal mode rates and the dependence of the cumulants moments reflected the difference between the nicked DNA and the supercoiled DNA dynamical behavior. The supercoiled DNA behavior seen here indicates that conformational dynamics might play a larger role in DNA behavior than is suggested by the notion of a branched interwound structure. © 1996 John Wiley & Sons, Inc.     

A novel form of intercalation involving four DNA duplexes in an acridine-4-carboxamide complex of d(CGTACG)(2)

The structures of the complexes formed between 9-amino-[N-(2-dimethyl-amino)butyl]acridine-4-carboxamide and d(CG^5BrUACG)₂ and d(CGTACG)₂ have been solved by X-ray crystallography using MAD phasing methodology and refined to a resolution of 1.6 Å. The complexes crystallised in space group C222. An asymmetric unit in the brominated complex comprises two strands of DNA, one disordered drug molecule, two cobalt (II) ions and 19 water molecules (31 in the native complex). Asymmetric units in the native complex also contain a sodium ion. The structures exhibit novel features not previously observed in crystals of DNA/drug complexes. The DNA helices stack in continuous columns with their central 4 bp adopting a B-like motif. However, despite being a palindromic sequence, the terminal GC base pairs engage in quite different interactions. At one end of the duplex there is a CpG dinucleotide overlap modified by ligand intercalation and terminal cytosine exchange between symmetry-related duplexes. A novel intercalation complex is formed involving four DNA duplexes, four ligand molecules and two pairs of base tetrads. The other end of the DNA is frayed with the terminal guanine lying in the minor groove of the next duplex in the column. The structure is stabilised by guanine N7/cobalt (II) coordination. We discuss our findings with respect to the effects of packing forces on DNA crystal structure, and the potential effects of intercalating agents on biochemical processes involving DNA quadruplexes and strand exchanges. NDB accession numbers: DD0032 (brominated) and DD0033 (native).     

A long polypyrimidine/polypurine tract induces an altered DNA conformation on the 3'' coding region of the adjacent myosin heavy chain gene.

A long (147 base pairs), natural A.T rich polypyrimidine/polypurine tract has been found 55 base pairs downstream of a chicken embryonic myosin heavy chain (MHC) gene. Analysis at the nucleotide level of nicks induced by S1 and Neurospora crassa nucleases indicate that this long interrupted polypyrimidine/polypurine tract exists in an alternate DNA structure in vitro at pH 4.5 and pH 7.5 in both supercoiled and linear plasmid DNA. The polypyrimidine/polypurine tract induces this alternate structure upon at least 200 base pairs of its 5' flanking DNA, and thus extends into the 3' coding and non-coding regions of the neighboring MHC gene. The different nicking patterns induced by the nucleases S1 and N. crassa on each strand of this alternate structure suggests that the polypyrimidine/polypurine tract may form heteronomous DNA. When this long polypyrimidine/polypurine tract is present in a supercoiled plasmid at low pH, a new and as yet undefined S1 hypersensitive DNA alteration was detected near the center of this tract.     

Crystal Structure of A Z-DNA Fragment Containing Thymine/2-Aminoadenine Base Pairs

Abstract

The Z-DNA structure has been shown to form in two crystals made from self-complementary DNA hexamers d(CGTDCG) and d(CDCGTG) which contain thymine/2-ammoadenine (TD) base pairs. The latter structure has been solved and refined to 1.3 Å resolution and it shows only small conformational changes due to the introduction of the TD base pairs in comparison with the structure of d(CG)3. Spectroscopic studies with these compounds demonstrate that DNA molecules containing 2-aminoadenine residues form Z-DNA slightly more easily than do those containing adenine nucleotides, but not as readily as the parent sequence containing only guanine-cytosine base pairs.     

Direct observation of positive supercoils introduced by reverse gyrase through atomic force microscopy

Reverse gyrase is a hyperthermophilic enzyme that can introduce positive supercoiling in substrate DNA. It is showed in our studies that positive DNA supercoils were induced in both pBR322 vector and an artificially synthesized mini-plasmid DNA by reverse gyrase. The left-handed structures adopted by positively supercoiled DNA molecules could be identified from their right-handed topoisomers through atomic force microscopic examination. Additional structural comparisons revealed that positively supercoiled DNA molecule AFM images exhibited increased contour lengths. Moreover, enzymatic assays showed that the positively supercoiled DNA could not be cleaved by T7 endonuclease. Together, this suggests that the overwound structure of positive supercoils could prevent genomic duplex DNA from randomly forming single-stranded DNA regions and intra-stranded secondary structures.     

Light induced DNA scission by a luminescent mixed-ligand uranyl complex

Efficient cleavage of supercoiled pBR322 DNA by X-ray crystallographically characterized complex, [UO₂(phen)(aba)(OC₂H₅)] (phen = 1,10-phenanthroline; aba = 4-dimethylamino benzoate) has been observed on irradiation with UV (350 nm) or visible light without any external additives through a mechanistic pathway involving singlet oxygen. This complex having 1,10-phenanthroline as an intercalator/binder to supercoiled DNA and N,N-(dimethylamino)benzoate as a chromophore.     

Crystal and molecular structure of a DNA fragment: d(CGTGAATTCACG)

The crystal structure of the dodecanucleotide d(CGTGAATTCACG) has been determined to a resolution of 2.7 A and refined to an R factor of 17.0% for 1532 reflections. The sequence crystallizes as a B-form double helix, with Watson-Crick base pairing. This sequence contains the EcoRI restriction endonuclease recognition site, GAATTC, and is flanked by CGT on the 5'-end and ACG on the 3'-end, in contrast to the CGC on the 5'-end and GCG on the 3'-end in the parent dodecamer d(CGCGAATTCGCG). A comparison with the isomorphous parent compound shows that any changes in the structure induced by the change in the sequence in the flanking region are highly localized. The global conformation of the duplex is conserved. The overall bend in the helix is 10 degrees. The average helical twist values for the present and the parent structures are 36.5 degrees and 36.4 degrees, respectively, corresponding to 10 base pairs per turn. The buckle at the substituted sites are significantly different from those seen at the corresponding positions in the parent dodecamer. Step 2 (GpT) is underwound with respect to the parent structure (27 degrees vs 36 degrees) and step 3 (TpG) is overwound (34 degrees vs 27 degrees). There is a spine of hydration in the narrow minor groove. The N3 atom of adenine on the substituted A10 and A22 bases are involved in the formation of hydrogen bonds with other duplexes or with water; the N3 atom of guanine on G10 and G22 bases in the parent structure does not form hydrogen bonds.     

Comparative Studies of the Thermodynamic Stabilities Between Sheared A:G and Watson-Crick A:U(T) Base Pairs in RNA and DNA

Abstract

Thermodynamic parameters for duplex formation were determined from CD melting curves for r(GGACGAGUCC)₂ and d(GGACGAGTCC)₂, both of which form two consecutive ‘sheared’ A:G base pairs at the center [Katahira et al. (1993) Nucleic Acids Res. 21, 5418–5424; Katahira et al., (1994) Nucleic Acids Res. 22, 2752–27591. The parameters were determined also for r(GGACUAGUCC)₂ and d(GGACTAGTCC)₂, where the A:G mismatches are replaced by Watson-Crick A:U(T) base pairs. Thermodynamic properties for duplex formation are compared between the sheared and the Watson-Crick base pairs, and between RNA and DNA. Difference in the thermodynamic stability is analyzed and discussed in terms of enthalpy and entropy changes. The characteristic features in CD spectra of RNA and DNA containing the sheared A:G base pairs are also reported.

     

Urea perturbation and the reversibility of nucleohistone conformation

Urea effect on conformation and thermal stabilities in nucleohistone and NaCl-treated partially dehistonized nucleohistones has been studied by circular dichroism (CD) and thermal denaturation. Urea imposes a CD change at 278mm of DNA base pairs in native and NaCl-treated nucleohistones which can be decomposed into two parts: a decrease in Δε₂₇₈ for histone-free base pairs and an increase for histone-bound base pairs. The reduction by urea of Δε₂₂₀ of bound histones is approximately proportional to the increase of Δε₂₇₈ of histone-bound base pairs. Urea also lowers the melting temperatures of base pairs both free and bound by histones. The presence of urea indeed destroys the secondary structure of bound histones, causing changes in the conformation and thermal stabilities of histone-bound base pairs in nucleohistone. Such a urea perturbation on nucleohistone conformation is reversible.     

Solution structure of RNA duplexes containing alternating CG base pairs: NMR study of r(CGCGCG)2 and 2'-O-Me(CGCGCG)2 under low salt conditions.

Structures of r(CGCGCG)2 and 2'-O-Me(CGCGCG)2 have been determined by NMR spectroscopy under low salt conditions. All protons and phosphorus nuclei resonances have been assigned. Signals of H5'/5" have been assigned stereospecifically. All 3JH,H and 3JP,H coupling constants have been measured. The structures were determined and refined using an iterative relaxation matrix procedure (IRMA) and the restrained MD simulation. Both duplexes form half-turn, right-handed helices with several conformational features which deviate significantly from a canonical A-RNA structure. Duplexes are characterised as having C3'-endo sugar pucker, very low base-pair rise and high helical twist and inclination angles. Helices are overwound with <10 bp per turn. There is limited inter-strand guanine stacking for CG steps. Within CG steps of both duplexes, the planes of the inter-strand cytosines are not parallel while guanines are almost parallel. For the GC steps this pattern is reversed. The 2'-O-methyl groups are spatially close to the 5'-hydrogens of neighbouring residues from the 3'-side and are directed towards the minor groove of 2'-O-Me(CGCGCG)2 forming a hydrophobic layer. Solution structures of both duplexes are similar; the effect of 2'-O-methylation on the parent RNA structure is small. This suggests that intrinsic properties imposed by alternating CG base pairs govern the overall conformation of both duplexes.     

Sequence and conformational effects on imino proton exchange in A.T- and A.U-containing DNA and RNA duplexes

¹H-nmr relaxation has been used to study the effect of sequence and conformation on imino proton exchange in adenine–thymine (A · T) and adenine–uracil (A · U) containing DNA and RNA duplexes. At low temperature, relaxation is caused by dipolar interactions between the imino and the adenine amino and AH2 protons, and at higher temperature, by exchange with the solvent protons. Although room temperature exchange rates vary between 3 and 12s^?1, the exchange activation energies (E_α) are insensitive to changes in the duplex sequence (alternating vs homopolymer duplexes), the conformation (B-form DNA vs A-form RNA), and the identity of the pyrimidine base (thymine vs uracil). The average value of the activation energy for the five duplexes studied, poly[d(A-T)], poly[d(A) · d(T)], poly[d(A-U)], Poly[d(A) · d(U)], and poly[r(A) · r(U)], was 16.8 ± 1.3 kcal/mol. In addition, we find that the average E_α for the A.T base pairs in a 43-base-pair restriction fragment is 16.4 ± 1.0 kcal/mol. This result is to be contrasted with the observation that the E_α of cytosine-containing duplexes depends on the sequence, conformation, and substituent groups on the purine and pyrimidine bases. Taken together, the data indicate that there is a common low-energy pathway for the escape of the thymine (uracil) imino protons from the double helix. The absolute values of the exchange rates in the simple sequence polymers are typically 3–10 times faster than in DNAs containing both A · T and G · C base pairs.     

AT base pairs are less stable than GC base pairs in Z-DNA: The crystal structure of d(m5CGTAm5CG)

Two hexanucleoside pentaphosphates, 5-methyl and 5-bromo cytosine derivatives of d(CpGpTp-ApCpG) have been synthesized, crystallized, and their three-dimensional structure solved. They both form left-handed Z-DNA and the methylated derivative has been refined to 1.2 Å resolution. These are the first crystal Z-DNA structures that contain AT base pairs. The overall form of the molecule is very similar to that of the unmethylated or the fully methylated (dC-dG)₃ hexamer although there are slight changes in base stacking. However, significant differences are found in the hydration of the helical groove. When GC base pairs are present, the helical groove is systematically filled with two water molecules per base pair hydrogen bonded to the bases. Both of these water molecules are not seen in the electron density map in the segments of the helix containing AT base pairs, probably because of solvent disorder. This could be one of the features that makes AT base pairs form Z-DNA less readily than GC base pairs.     

Molecular modeling of closed circular DNA thermodynamic ensembles

Many modeling studies of supercoiled DNA are based on equilibrium structures from theoretical calculations or energy minimization. Since closed circular DNAs are flexible, it is possible that errors are introduced by calculating properties from a single minimum energy structure, rather than from a complete thermodynamic ensemble. We have investigated this question using molecular dynamics simulations on a low resolution molecular mechanics model in which each base pair is represented by three points (a plane). This allows the inclusion of sequence-dependent variations of tip, inclination, and twist. Three kinds of sequences were tested: (1) homogeneous DNA, in which all base pairs have the helicoidal parameters of an ideal, average B-DNA; (2) random sequence DNA; and (3) curved DNA. We examined the rate of convergence of various structural parameters. Convergence for most of these is slowest for homogeneous sequences, more rapid for random sequences, and most rapid for curved sequences. The most slowly converging parameter is the antipodes profile. In a plasmid with N base pairs (bp), the antipodes distance is the distance d _ij from base pair i to base pair j halfway around the plasmid, j = i + N/2. The antipodes profile at time t is a plot of d _ij over the range i = 1, N/2. In a homogeneous plasmid, convergence requires that the antipodes profile averaged over time must be flat. Even in the small plasmids examined here, the average properties of the ensembles were found to differ from those of static equilibrium structures. These effects will be even more dramatic for larger plasmids. Further, average and dynamic properties are affected by both plasmid size and sequence. © 1996 John Wiley & Sons, Inc.     

Detection of triple-helix related structures adopted by poly(dG)-poly(dC) sequences in supercoiled plasmid DNA.

Negative superhelical strain induces the poly(dG)-poly(dC) sequence to adopt two totally different types of triple-helices, either a dG.dG.dC triplex in the presence of Mg(+)+ at both neutral and acidic pHs or a protonated dC+.dG.dC triplex in the absence of Mg(+)+ ions at acidic pH (1). To examine whether there are still other types of non-B DNA structures formed by the same sequence, we constructed supercoiled plasmid DNAs harboring varying lengths of the poly(dG) tract, and the structures adopted by each supercoiled plasmid DNA were studied with a chemical probe, chloroacetaldehyde. The potential of a poly(dG)-poly(dC) sequence to adopt non-B DNA structures depends critically on the length of the tract. Furthermore, in the presence of Mg(+)+ and at a mildly acidic pH, in addition to the expected dG.dG.dC triplex detected for the poly(dG) tracts of 14 to 30 base pairs (bp), new structures were also detected for the tracts longer than 35 bp. The structure formed by a poly(dG) tract of 45 bp revealed chemical reaction patterns consistent with a dG.dG.dC triplex and protonated dC+.dG.dC triple-helices fused together. This structure lacks single-stranded stretches typical of intramolecular triplexes.     

Existence of the C Structure in Poly(dA-dC) · Poly(dG-dT)

Abstract

We show that the lithium salt of calf-thymus DNA can assume the C structure in nonoriented, hydrated gels. The transitions between the B and C structures showed little hysteresis and none of the metastable structural states which occur in oriented gels. Therefore crystal-lattice forces are not needed to stabilize the C structure.

The occurrence of the alternative structures of the Li, Na and K salts of poly(dA-dC) · poly(dG-dT) was measured as a function of hydration for nonoriented gels. Poly(dA-dC) · poly(dG-dT) · Li exists in the B structure at high hydrations and in the C structure at moderate hydrations with no A or Z structure at any hydration tested. The Na salt of poly(dA-dC) · poly(dG-dT) exists in the B structure at high hydration, as mixtures of B and C at moderate hydrations and in the A structure at lower hydrations. The potassium salt behaves similarly except that mixtures of the C and A structures exist at lower hydrations.

ZnCl₂ and NaNO₃, which promote the Z structure in duplex poly(dG-dC), promote the C structure in poly(dA-dC) · poly(dG-dT). Information contained in the sequence of base pairs and not specific ionic interactions appear to determine the stability of the alternative structures of polynucleotides as hydration is changed.