Interaction between the Z-type DNA duplex and 1,3-propanediamine: crystal structure of d(CACGTG)2 at 1.2 A resolution

The crystal structure of a hexamer duplex d(CACGTG)(2) has been determined and refined to an R-factor of 18.3% using X-ray data up to 1.2 A resolution. The sequence crystallizes as a left-handed Z-form double helix with Watson-Crick base pairing. There is one hexamer duplex, a spermine molecule, 71 water molecules, and an unexpected diamine (Z-5, 1,3-propanediamine, C(3)H(10)N(2)) in the asymmetric unit. This is the high-resolution non-disordered structure of a Z-DNA hexamer containing two AT base pairs in the interior of a duplex with no modifications such as bromination or methylation on cytosine bases. This structure does not possess multivalent cations such as cobalt hexaammine that are known to stabilize Z-DNA. The overall duplex structure and its crystal interactions are similar to those of the pure-spermine form of the d(CGCGCG)(2) structure. The spine of hydration in the minor groove is intact except in the vicinity of the T5A8 base pair. The binding of the Z-5 molecule in the minor grove of the d(CACGTG)(2) duplex appears to have a profound effect in conferring stability to a Z-DNA conformation via electrostatic complementarity and hydrogen bonding interactions. The successive base stacking geometry in d(CACGTG)(2) is similar to the corresponding steps in d(CG)(3). These results suggest that specific polyamines such as Z-5 could serve as powerful inducers of Z-type conformation in unmodified DNA sequences with AT base pairs. This structure provides a molecular basis for stabilizing AT base pairs incorporated into an alternating d(CG) sequence.     

Spectroscopic studies of (m5dC-dG)3: thermal stability of B- and Z-forms.

The hexanucleoside pentaphosphate d(m5CpGpm5CpGpm5CpG) has been studied in solution by ultra-violet absorption, circular dichroism and 31P nuclear magnetic resonance under various experimental conditions. In 0.2 M NaClO4 at low temperature, an hexamer duplex is formed which has a B or B-like conformation. As the salt concentration is increased, a transition from a B-form to the Z-form occurs and is complete in 3 M NaClO4. In 3 M NaClO4, the behavior of the Z double helix is complex as a function of temperature. The variation of the circular dichroism at 295 nm is biphasic. A first transition occurs over a large range of temperature and corresponds to a conformational change due to a non-cooperative intramolecular process. Ultra-violet absorption and 31P nuclear magnetic resonance show that the new conformation arising from a distortion of the backbone is not similar to that observed in low salt conditions (B-form). At high hexanucleotide concentration, aggregates are formed. The second transition is cooperative and corresponds to the melting of a double stranded helix into single strands.     

Theoretical optical properties of poly-L-proline

A non-perturbational technique is used to calculate the circular dichroism and absorption spectra of polypeptide chains having conformations similar to that of poly-L -proline II. The method employs a Bogoliubov exciton formalism, from which the various optical terms associated with parallel and perpendicular components of the exciton band are obtained. A simple model for the peptide unit, consisting of three Gaussian absorption bands, leads to reasonable results for the polymer spectra, provided the lowest energy peptide π → π* transition is taken at 207 mμ and the value of the Ramachandran angle Ψ is taken to be 390°. The calculations suggest that the polymer circular dichroism spectrum is the resultant of strong interference among the two Gaussian exciton terms and the non-Gaussian helix term. Consequently, the CD spectrum is very sensitive to the value of Ψ. It is found that the small positive CD band in the vicinity of 230 mμ arises partly from the effect of the static (crystal) field interactions on the n → π* CD band.     

The hydrogen-bonding structure in parallel-stranded duplex DNA is reverse Watson-Crick

Raman spectra of the parallel-stranded duplex formed from the deoxyoligonucleotides 5'-d-[(A)10TAATTTTAAATATTT]-3' (D1) and 5'-d[(T)10ATTAAAATTTATAAA]-3' (D2) in H2O and D2O have been acquired. The spectra of the parallel-stranded DNA are then compared to the spectra of the antiparallel double helix formed from the deoxyoligonucleotides D1 and 5'-d(AAATATTTAAAATTA-(T)10]-3' (D3). The Raman spectra of the antiparallel-stranded (aps) duplex are reminiscent of the spectra of poly[d(A)].poly[d(T)] and a B-form structure similar to that adopted by the homopolymer duplex is assigned to the antiparallel double helix. The spectra of the parallel-stranded (ps) and antiparallel-stranded duplexes differ significantly due to changes in helical organization, i.e., base pairing, base stacking, and backbone conformation. Large changes observed in the carbonyl stretching region (1600-1700 cm-1) implicate the involvement of the C(2) carbonyl of thymine in base pairing. The interaction of adenine with the C(2) carbonyl of thymine is consistent wtih formation of reverse Watson-Crick base pairing in parallel-stranded DNA. Phosphate-furanose vibrations similar to those observed for B-form DNA of heterogenous sequence and high A,T content are observed at 843 and 1092 cm-1 in the spectra of the parallel-stranded duplex. The 843-cm-1 band is due to the presence of a sizable population of furanose rings in the C2'-endo conformation. Significant changes observed in the regions from 1150 to 1250 cm-1 and from 1340 to 1400 cm-1 in the spectra of the parallel-stranded duplex are attributed to variations in backbone torsional and glycosidic angles and base stacking.     

Spectroscopic studies on ethidium bromide binding to intramolecular parallel and antiparallel triple helices containing T*A:T and G*G:C triplets

The interaction of ethidium bromide (EB), a DNA intercalator, with two intramolecular triplexes 5'd(G4A4G4-[T4]-C4T4C4-[T4]-G4T4G4), 5'd(G4T4G4-[T4]-G4A4G4-[T4]-C4T4C4) ([T4] represents a stretch of 4 thymine residues) and their precursor duplexes has been investigated by circular dichroism, fluorescence and UV absorption spectroscopy. Binding of EB induces a circular dichroism band in the region around 310 nm which is positive for the duplex forms but negative for the triplex forms. We observed that the binding of EB to the duplex form does not induce the formation of the triplex structures. Thermal denaturation experiments demonstrate that EB stabilizes more the parallel triple helix than the antiparallel one. Analysis of the binding process from fluorescence measurements shows that binding constants to the triple helical forms and to the hairpin reference duplex [T4]-G4A4G4-[T4]-C4T4C4) are close. However the binding site size is larger for the triplexes (4-6 base triplets) than for the duplex (2 base pairs).     

Oligo-[alpha]-deoxynucleotides covalently linked to an intercalating agent. Double helices with parallel strands are formed with complementary oligo-[beta]-deoxynucleotides.

An oligo-[alpha]-deoxynucleotide of sequence (5')d(TCTAAACTC) (3') was synthesized using the alpha-anomers of deoxynucleosides and its 5'-phosphate was covalently linked to a 9-amino acridine derivative via a pentamethylene linker. Two oligo-[beta]-deoxynucleotides containing the complementary sequence in either the 5'----3' or the 3'----5' orientation were synthesized using natural [beta]-deoxynucleosides. Complex formation was investigated by absorption and fluorescence spectroscopies. No change in spectroscopic properties was detected with the anti-parallel [beta] sequence. Absorption changes were induced in the visible absorption band of the acridine derivative at 2 degrees C when the acridine-substituted oligo-[alpha]-deoxynucleotide was mixed in equimolecular amounts with the complementary [beta]-sequence in the parallel orientation. Hypochromism was observed in the UV range. The fluorescence of the acridine derivative was quenched by the guanine base present in the second position of the complementary sequence. Cooperative dissociation curves were observed and identical values of melting temperatures were obtained by absorption and fluorescence. An increase in salt concentration stabilized the complex with a delta Tm of 8 degrees C when NaCl concentration increased from 0.1 to 1 M. These results demonstrate that an oligo-[alpha]-deoxynucleotide covalently linked to an intercalating agent is able to form a double helix with an oligo-[beta]-deoxynucleotide. The two strands of this [alpha]-[beta] double helix adopt a parallel 5'----3' orientation. The acridine ring is able to intercalate between the first two base pairs on the 5'-side of the duplex structure.     

Three-dimensional structures of bulge-containing DNA fragments.

The three-dimensional structure of a DNA tridecamer d(CGCAGAATTCGCG)2 containing bulged adenine bases was determined by single crystal X-ray diffraction methods, at 120 K, to 2.6 A resolution. The structure is a B-DNA type double helix with a single duplex in the asymmetric unit. One of the bulged adenine bases loops out from the double helix, while the other stacks in to it. This is in contrast to our preliminary finding, which indicated that both adenine bases were looped out. This revised model was confirmed by the use of a covalently bound heavy-atom derivative. The conformation of the looped-out bulge hardly disrupts base stacking interactions of the bases flanking it. This is achieved by the backbone making a "loop-the-loop" curve with the extra adenine flipping over with respect to the other nucleotides in the strand. The looped-out base intercalates into the stacked-in bulge site of a symmetrically related duplex. The looped-out and stacked-in bases form an A.A reversed Hoogsteen base-pair that stacks between the surrounding base-pairs, thus stabilizing both bulges. The double helix is frayed at one end with the two "melted" bases participating in intermolecular interactions. A related structure, of the same tridecamer, after soaking the crystals with proflavin, was determined to 3.2 A resolution. The main features of this B-DNA duplex are basically similar to the native tridecamer but differ in detail especially in the conformation of the bulged-out base. Accommodation of a large perturbation such as that described here with minimal disruption of the double helix shows both the flexibility and resiliency of the DNA molecule.     

On the formation of the double helix between adenine single strands at acidic pH from synchrotron radiation circular dichroism experiments

Here, we present synchrotron radiation circular dichroism spectra for a series of DNA adenine strands, (dA)(n) , n = 2-10, 15, at acidic pH. Reference spectra of a protonated single strand, (dAH(+) )(n) , and a protonated double helix, (dAH(+) )(n) :(dAH(+) )(n) , are provided in the wavelength region from 175 to 330 nm. The largest spectral difference between single and double strands is in the vacuum ultraviolet, where a band changes sign. This new spectral feature that characterizes double helix formation may be useful for analytical purposes but also for shedding light on the underlying complexation mechanism. Furthermore, we find that a minimum of eight or nine bases in a strand is needed for two (dAH(+) )(n) strands to form a duplex. This is a relatively high number as compared with guanine quadruplex and cytosine i-motif formation, which is likely linked to the significant Coulomb repulsion between the all-protonated bases. Finally, spectra recorded as a function of time after sample preparation indicates that the equilibrium is slowly reached, in certain cases taking an hour or more.     

Circular dichroism of helical polynucleotides calculated by the linear response method

Linear response theory in the decorrelation or random-phase approximation is used to calculate the absorption and CD spectra of model helical polymers, including single-stranded polyadenylic acid. The method, which makes use of infinite polymer selection rules for the linear response tensor, has the advantages that (1) only a few three-dimensional matrices need be inverted; (2) spectral band shapes of the polymer arise naturally from those of the monomer, as well as from the geometry-dependent interactions in the helix; and (3) the spectral dependence on geometrical factors of the helix is made transparent. It is found that the structure of the polymer CD spectrum depends critically on monomer bandshape. An asymmetric CD spectrum, similar to some experimental spectra, arises from either a Gaussian or a composite monomer band. Single-stranded polyadenylic acid spectra are sensitive to helix geometry in the region 200–240 nm, in reasonable agreement with experimental spectra. This sensitivity arises from the 207-nm monomer transition, and the results suggest that this region of the spectrum should be more fully exploited as a tool for helix geometry studies.     

Crystal structure of a poly(rA) staggered zipper at acidic pH: evidence that adenine N1 protonation mediates parallel double helix formation

We have solved at 1.07 Å resolution the X-ray crystal structure of a polyriboadenylic acid (poly(rA)) parallel and continuous double helix. Fifty-nine years ago, double helices of poly(rA) were first proposed to form at acidic pH. Here, we show that 7-mer oligo(rA), i.e. rA₇, hybridizes and overlaps in all registers at pH 3.5 to form stacked double helices that span the crystal. Under these conditions, rA₇ forms well-ordered crystals, whereas rA₆ forms fragile crystalline-like structures, and rA₅, rA₈ and rA₁₁ fail to crystallize. Our findings support studies from ∼50 years ago: one showed using spectroscopic methods that duplex formation at pH 4.5 largely starts with rA₇ and begins to plateau with rA₈; another proposed a so-called ‘staggered zipper’ model in which oligo(rA) strands overlap in multiple registers to extend the helical duplex. While never shown, protonation of adenines at position N1 has been hypothesized to be critical for helix formation. Bond angles in our structure suggest that N1 is protonated on the adenines of every other rAMP−rAMP helix base pair. Our data offer new insights into poly(rA) duplex formation that may be useful in developing a pH sensor.     

Electron-spin-resonance studies of a chlorpromazine derivative bound to DNA fibres.

Solutions of DNA, spin-labelled with the radical cation of chlorpromazine, were used to produce oriented species of fibres pulled from a gel obtained by ultracentrifugation. The electron spin resonance spectra, recorded at X and Q band frequencies, are given for both gel and fibres; 14N hyperfine coupling parameters were obtained by computer fitting. The spectra are explained in terms of a strongly immobilized label having one principal hyperfine tensor axis parallel to the axis of the DNA helix, and the preferential orientation of the chlorpromazine ions with their planes perpendicular to the DNA helical axis.     

Circular dichroism and UV melting studies on formation of an intramolecular triplex containing parallel T*A:T and G*G:C triplets: netropsin complexation with the triplex.

We have used circular dichroism and UV absorption spectroscopy to characterize the formation and melting behaviour of an intramolecular DNA triple helix containing parallel T*A:T and G*G:C triplets. Our approach to induce and to stabilize a parallel triplex involves the oligonucleotide 5'-d(G4A4G4[T4]C4T4C4-[T4]G4T4G4) ([T4] represents a stretch of four thymine residues). In a 10 mM sodium cacodylate, 0.2 mM disodium EDTA (pH 7) buffer, we have shown the following significant results. (i) While in the absence of MgCl2 this oligonucleotide adopts an intramolecular hairpin duplex structure prolonged by the single strand extremity 5'-d([T4]G4T4G4), the presence of millimolar concentrations of MgCl2generates an intramolecular triplex (via double hairpin formation). (ii) In contrast to the antiparallel triplex formed by the oligonucleotide 5'-d(G4T4G4[T4]G4A4G4[T4]C4T4C4), the parallel triplex melts in a biphasic manner (a triplex to duplex transition followed by a duplex to coil transition) and is less stable than the antiparallel one. The enthalpy change associated with triplex formation (-37 kcal/mol) is approximately half that of duplex formation (-81 kcal/mol). (iii) The parallel triple helix is disrupted by increasing the concentration of KCl(>10 mM), whereas, under the same conditions, the antiparallel triplex remains stable. (iv) Netropsin, a natural DNA minor groove-binding ligand, binds to the central site A4/T4of the duplex or triplex in an equimolar stoichiometry. Its association constant K is smaller for the parallel triplex ( approximately 1 x 10(7) M-1) than for the antiparallel one ( approximately 1 x 10(8) M-1). In contrast to the antiparallel structure, netropsin binding has no apparent effect on thermal stability of the parallel triple helix.     

Total optical activity of agarose: relation to observable transitions in the vacuum ultraviolet

The changes in optical activity that accompany and characterize the coil-helix and helix-coil transitions of agarose in aqueous solutions and gels have been investigated by combined quantitative analysis of data from vacuum ultraviolet circular dichroism (VUCD) and optical rotary dispersion (ORD). VUCD of agarose in the high-temperature coil state shows a single accessible Gaussian band centered at ～183 nm. In the helix state this band is blue-shifted by ～9 nm, and the intensity is increased by a factor of ～2.6. Spectra at intermediate temperatures can be fitted to within experimental error by linear combination of coil and helix spectra, the relative proportions required providing an index of the extent of conformational ordering. ORD spectra throughout the conformational transition have a common form and differ only in absolute magnitude. The temperature course of conformational ordering derived from ORD intensity is in close agreement with the values obtained from VUCD. In both the coil and helix states the accessible VUCD band is positive, while the overall ORD is negative, indicating strong negative CD activity at lower wavelength. The ORD contribution corresponding to the positive VUCD band was calculated by Kronig–Kramers transform, and it was subtracted from the total ORD to give the residual ORD from all other optically active transitions of the molecule. In both the coil and helix states, this residual ORD could be fitted to within experimental error by a single Gaussian CD band at ～149 nm. A negative band at this wavelength has been reported previously for agarose films, but the observed intensity, relative to that of the lower energy positive band, is substantially smaller than the fitted value under hydrated conditions. In both the coil and helix states the total optical activity of agarose, characterized by observed ORD spectra, can be matched to within experimental error by Kronig-Kramers transform of the 149-nm negative band and the smaller positive band at higher wavelength, with no necessary involvement of deeper-lying transitions. The significance of this conclusion for fundamental understanding of carbohydrate optical activity is discussed.     

A Z-DNA binding protein isolated from D. radiodurans

A DNA binding protein isolated from D. radiodurans changes CD-spectrum of Z-form poly(dG-dC) X poly(dG-dC). We have found that a positive band at 268 nm is converted close to that of B-form in the presence of the protein. Concomitantly, a negative band at 295 nm shown by Z-form poly(dG-dC) X poly (dG-dC) was weakened by the protein but not by albumin. Such changes in the CD-spectra were not induced by the protein and by albumin when they were mixed with Z- or B-form poly(dG-me5dC) X poly(dG-me5dC) or with B-form poly(dG-dC) X poly(dG-dC). The protein formed a complex preferentially with Z-form poly(dG-dC) X poly(dG-dC).     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls a and b in nematic liquid crystals. II. Magnetic circular dichroism spectra

Absorption and magnetic circular dichroism (MCD) spectra are reported for chlorophyll (Chl) a and Chl b dissolved in nematic liquid crystal solvents. The spectra were measured with the dye molecules oriented uniaxially along the direction of. the magnetic field and measuring light beam. It is significant that under such conditions the MCD spectra recorded in the wavelength region of the Q and Soret bands of the chlorophyll are essentially unchanged with respect to rotation of the sample cell around this axis, even though there is almost complete orientation of the chlorophyll molecules by the liquid crystals. The MCD spectra of Chl a and b in the nematic liquid crystal solvents used in this study are surprisingly similar to the spectra obtained under isotropic conditions. These results illustrate an important technique with which to examine the optical spectra of dyes oriented in liquid crystal matrices in which the anisotropic effects can be reduced the negligible proportions by the application of a strong magnetic field parallel to the direction of the measuring light beam. The first deconvolution calculations are reported that describe the deconvolution of pairs of absorption and MCD spectra, in the Q and B band regions, for both Chl a and b. The spectral analysis to obtain quantitative estimates of transition energies was accomplished by carrying out detailed deconvolution calculations in which the both the absorption and MCD spectral envelopes were fitted with the same number of components; each pair of components had the same hand centres and bandwidth values. This procedure resulted in an assignment of each of the main transitions in the absorption spectra of both Chl a and b. Chl a is clearly monomeric, with Qy, Qx, By and Bx located at 671, 582, 439 and 431 nm, respectively. Analysis of the spectral data for Chl b located Qy, By and Bx, at 662, 476 and 464 nm, respectively.     

A parallel stranded linear DNA duplex incorporating dG.dC base pairs

DNA oligonucleotides with appropriately designed complementary sequences can form a duplex in which the two strands are paired in a parallel orientation and not in the conventional antiparallel double helix of B-DNA. All parallel stranded (ps) molecules reported to date have consisted exclusively of dA.dT base pairs. We have substituted four dA.dT base pairs of a 25-nt parallel stranded linear duplex (ps-D1.D2) with dG.dC base pairs. The two strands still adopt a duplex structure with the characteristic spectroscopic properties of the ps conformation but with a reduced thermodynamic stability. Thus, the melting temperature of the ps duplex with four dG.dC base pairs (ps-D5.D6) is 10-16 degrees C lower and the van't Hoff enthalpy difference delta HvH for the helix-coil transition is reduced by 20% (in NaCl) and 10% (in MgCl2) compared to that of ps-D1.D2. Based on energy minimizations of a ps-[d(T5GA5).d(A5CT5)] duplex using force field calculations we propose a model for the conformation of a trans dG.dC base pair in a ps helix.     

Ultraviolet circular dichroism of polyproline and oriented collagen

The ultraviolet absorption, linear dichroism, circular dichroism, and oriented circular dichroism of collagen are reported and the spectra are resolved into a self-consistent set of bands in accord with exciton theory. The parallel band at 200 nm has 40% of the π → π* intensity; the perpendicular band is placed at 189 nm yielding a splitting of 2700 cm^?1. The circular dichroism is resolved into two Gaussians at λ_∥ and λ_τ (rotational strengths +14 × 10^?40 and ?32 × 10^?40 esu². cm²) plus a large non-Gaussian (“helix”) band with ampplitude ?25,000° at 201 nm. These data appear to be in reasonably good accord with recent calculations. Measurements of the absorption, linear dichroism and circular dichroism of polyproline I and II are also reported and are resolved into their component bands. Polyproline I is in good accord with exciton theory, whereas polyproline II remains unsatisfactory.     

Binding geometries of benzo[a]pyrene diol epoxide isomers covalently bound to DNA. Orientational distribution

Flow linear dichroism (LD) of different benzo[a]pyrene diol epoxide (BPDE) isomers covalently bound to calf thymus DNA or poly(dG-dC) provides information about binding geometry and DNA perturbation. With anti-BPDE the apparent angle between the long axis (z) of the pyrene chromophore and the DNA helix axis is approximately 30 degrees as evidenced from the LD of z-polarized absorption bands in the pyrenyl chromophore at 252 and 346 nm. The corresponding angle for the in-plane short axis (y) is determined to be approximately 70 degrees from a y-polarized band at 275 nm. The binding of (+)-anti-BPDE to DNA is found to cause a considerable reduction of the DNA orientation. This is ascribed to a decreased persistence length of DNA, owing either to increased flexibility ("flexible joints") or to permanent kinks at the points of binding. The reduced linear dichroism (LDr), i.e., the ratio between LD and isotropic absorbance, of the long-wavelength absorption band system of BPDE bound to DNA exhibits a wavelength dependence that indicates a relatively wide orientational distribution of the z axis of pyrene. Fluorescence data support the conclusion of a heterogeneous distribution, and a very low polarization anisotropy indicates a mobility between the different orientational states, which is rapid compared to the fluorescence lifetime (nanosecond time scale). Attempts are made to simulate the observed LDr features of the (+)-anti-BPDE-poly(dG-dC) complex using different distribution models on the assumption that the angular dependence of the spectral perturbation is due to dispersive interactions with DNA bases.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structural model for an oligonucleotide containing a bulged guanosine by NMR and energy minimization

We present three-dimensional structural models for a DNA oligomer containing a bulged guanosine based on proton NMR data and energy minimization computations. The nonexchangeable proton resonances of the duplex 5'd(GATGGGCAG).d(CTGCGCCATC) are assigned by nuclear Overhauser effect spectroscopy (NOESY) and correlated spectroscopy connectivities, and the NMR spectrum is compared with that of a regular 8-mer of similar sequence, 5'd(GATGGCAG).d(CTGCCATC). Experimental proton-proton distances are obtained from NOESY spectra acquired with mixing times of 100, 150, and 200 ms. A refined three-dimensional structure for the bulge-containing duplex is calculated from regular B DNA starting coordinates by using the AMBER molecular mechanics program [Weiner, S. J., Kollman, P. A., Case, D. A., Singh, U. C., Ghio, C., Alagona, G., Profeta, S., & Weiner, P. (1984) J. Am. Chem. Soc. 106, 765-784]. We compare structures obtained by building the helix in three and four base pair increments with structures obtained by direct minimization of the entire nine base sequence, with and without experimental distance constraints. The general features of all the calculated structures are very similar. The helix is of the B family, with the extra guanine stacked into the helix, and the helix axis is bent by 18-23 degrees, in agreement with gel mobility data for bulge-containing sequences [Rice, J. A. (1987) Ph.D. Thesis, Yale University].