Base tilt of B-form poly[d(G)]-poly[d(C)] and the B- and Z-conformations of poly[d(GC)]-poly[d(GC)] in solution

DNA stretching and compression: large-scale simulations of double helical structures

Computer-simulated elongation and compression of A - and B -DNA structures beyond the range of thermal fluctuations provide new insights into high energy "activated" forms of DNA implicated in biochemical processes, such as recombination and transcription. All-atom potential energy studies of regular poly(dG).poly(dC) and poly(dA).poly(dT) double helices, stretched from compressed states of 2.0 A per base-pair step to highly extended forms of 7.0 A per residue, uncover four different hyperfamilies of right-handed structures that differ in mutual base-pair orientation and sugar-phosphate backbone conformation. The optimized structures embrace all currently known right-handed forms of double-helical DNA identified in single crystals as well as non-canonical forms, such as the original "Watson-Crick" duplex with trans conformations about the P-O5' and C5'-C4' backbone bonds. The lowest energy minima correspond to canonical A and B -form duplexes. The calculations further reveal a number of unusual helical conformations that are energetically disfavored under equilibrium conditions but become favored when DNA is highly stretched or compressed. The variation of potential energy versus stretching provides a detailed picture of dramatic conformational changes that accompany the transitions between various families of double-helical forms. In particular, the interchanges between extended canonical and non-canonical states are reminiscent of the cooperative transitions identified by direct stretching experiments. The large-scale, concerted changes in base-pair inclination, brought about by changes in backbone and glycosyl torsion angles, could easily give rise to the observed sharp increase in force required to stretch single DNA molecules more than 1.6-1.65 times their canonical extension. Our extended duplexes also help to tie together a number of previously known structural features of the RecA-DNA complex and offer a self-consistent stereochemical model for the single-stranded/duplex DNA recognition brought in register by recombination proteins. The compression of model duplexes, by contrast, yields non-canonical structures resembling the deformed steps in crystal complexes of DNA with the TATA-box binding protein (TBP). The crystalline TBP-bound DNA steps follow the calculated compression-elongation pattern of an unusual "vertical" duplex with base planes highly inclined with respect to the helical axis, exposed into the minor groove, and accordingly accessible for recognition.Significantly, the double helix can be stretched by a factor of two and compressed roughly in half before its computed internal energy rises sharply. The energy profiles show that DNA extension-compression is related not only to the variation of base-pair Rise but also to concerted changes of Twist, Roll, and Slide. We suggest that the high energy "activated" forms calculated here are critical for DNA processing, e.g. nucleo-protein recognition, DNA/RNA synthesis, and strand exchange.

Structural equilibrium of DNA represented with different force fields

We have recently indicated preliminary evidence of different equilibrium average structures with the CHARMM and AMBER force fields in explicit solvent molecular dynamics simulations on the DNA duplex d(C5T5) . d(A5G5) (Feig, M. and B.M. Pettitt, 1997, Experiment vs. Force Fields: DNA conformation from molecular dynamics simulations. J. Phys. Chem. B. (101:7361-7363). This paper presents a detailed comparison of DNA structure and dynamics for both force fields from extended simulation times of 10 ns each. Average structures display an A-DNA base geometry with the CHARMM force field and a base geometry that is intermediate between A- and B-DNA with the AMBER force field. The backbone assumes B form on both strands with the AMBER force field, while the CHARMM force field produces heterogeneous structures with the purine strand in A form and the pyrimidine strand in dynamical equilibrium between A and B conformations. The results compare well with experimental data for the cytosine/guanine part but fail to fully reproduce an overall B conformation in the thymine/adenine tract expected from crystallographic data, particularly with the CHARMM force field. Fluctuations between A and B conformations are observed on the nanosecond time scale in both simulations, particularly with the AMBER force field. Different dynamical behavior during the first 4 ns indicates that convergence times of several nanoseconds are necessary to fully establish a dynamical equilibrium in all structural quantities on the time scale of the simulations presented here.

Comparison of base inclination of ribo-AU and deoxyribo-AT polymers

The inclination angle between the base normal and the helix axis is measured for ribo-AU polymers by using flow linear dichroism (LD), and compared to measurements for deoxyribo-AT polymers under dehydrating conditions. The CD of the DNA polymers under the dehydrating conditions is not the same as the corresponding RNA polymers, which are presumed to be in the A form. However, the LD indicates that poly(dAdT)-poly(dAdT) can assume the A form in 80% 2,2,2-trifluoroethanol, although poly(dA)-poly(dT) retains B form structure in this dehydrating solvent. The inclination angles are similar for B form poly(dAdT)-poly(dAdT) and poly(dA)-poly(dT), and these parameters are also similar for A form poly(rArU)-poly(rArU) and poly(rA)-poly(rU). All inclination axes are similar.

Comparison of base inclination of ribo-GC and deoxyribo-GC polymers, and synthesis of poly(rGrC)-poly(rGrC)

The inclination angle between the base normal and the helix axis, and the axes around which the bases incline, are measured for ribo-GC polymers in buffer by using flow linear dichroism (LD), and compared to measurements for deoxyribo-GC polymers in buffer and under dehydrating conditions. A new method is designed to synthesize poly(rGrC)-poly(rGrC), which is not available commercially, in large quantities. The LD of this RNA reveals inclination angles that are similar to the B-form DNA in buffer, although the axes are different. The CD of poly(dGdC)-poly(dGdC) under the dehydrating conditions is similar to poly(rGrC)-poly(rGrC), indicating it is in the A form, and the LD gives larger inclination angles than either the B form or the corresponding RNA. Poly(dG)-poly(dC) is in the A form in buffer. Comparison among poly(rG)-poly(rC) in buffer, and poly(dG)-poly(dC) in buffer under dehydrating conditions, reveals similar inclination angles and axes, although the LD shows that the DNA has the largest inclination angles. Except for poly(rGrC)-poly(rGrC), which has a unique reduced dichroism, all the axes for G are similar, as are the axes for C.

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.

Linear-dichroism spectroscopy for the study of structural properties of proteins

This review gives an experiment directed survey of the application of linear-dichroism (LD) spectroscopy to the study of proteins. LD spectroscopy is a relatively simple technique that provides information on the orientation of chromophores in molecules, on molecular characteristics such as shape, size and electronic properties, and on binding parameters in molecular complexes. Since LD is only observed when the molecules are non-randomly oriented in the sample, particular attention is paid to various orientation techniques, viz. in electric and flow fields, in polymer films and gels, and by light induction (photoselection). Examples are given on bacteriorhodopsin and retinals, chlorosomes, lens crystallins, aspartate aminotransferase, and the interaction of gene32- and recA-protein with DNA.

Linear dichroism demonstrates that the bases in poly[d(AC)].poly[d (GT)] and poly[d(AG)].poly[d(CT)] are inclined from perpendicular to the helix axis

Flow linear dichroism is used to measure specific inclinations for each of the four bases in poly[d(AC)].poly[d(GT)] and poly[d(AG)].poly[d(CT)] in both the B and A forms. For the B form in solution the bases are found to have a sizable inclination. Inclination is increased in the A form, as expected. In all cases the pyrimidines are more inclined than the purines.

Linear dichroism spectroscopy of nucleic acids

This review will consider solution studies of structure and interactions of DNA and DNA complexes using linear dichroism spectroscopy, with emphasis on the technique of orientation by flow. The theoretical and experimental background to be given may serve, in addition, as a general introduction into the state of the art of linear dichroism spectroscopy, particularly as it is applied to biophysical problems.

Circular dichroism studies of the structure of DNA complex with berberine

The binding of the benzodioxolo-benzoquinolizine alkaloid, berberine chloride to natural and synthetic DNAs has been studied by intrinsic and extrinsic circular dichroic measurements. Binding of berberine causes changes in the circular dichroism spectrum of DNA as shown by the increase of molar ellipticity of the 270nm band, but with very little change of the 240nm band. The molar ellipticity at the saturation depends strongly on the base composition of DNA and also on salt concentration, but always larger for the AT rich DNA than the GC rich DNA. The features in the circular dichroic spectral changes of berberine-synthetic DNA complexes were similar to that of native DNA, but depends on the sequence of base pairs. On binding to DNA and polynucleotides, the alkaloid becomes optically active. The extrinsic circular dichroism developed in the visible absorption region (300-500nm) for the berberine-DNA complexes shows two broad spectral bands in the regions 425-440nm and 340-360nm with the maximum varying depending on base composition and sequence of DNA. While the 425nm band shows less variation on the binding ratio, the 360nm band is remarkably dependent on the DNA/alkaloid ratio. The generation of the alkaloid associated extrinsic circular dichroic bands is not dependent on the base composition or sequence of base pairs, but the nature and magnitude of the bands are very much dependent on these two factors and also on the salt concentration. The interpretation of the results with respect to the modes of the alkaloid binding to DNA are presented.

Microscopic behaviour of DNA during electrophoresis: electrophoretic orientation

The study of the behaviour of DNA when subjected to electric fields poses several intriguing problems of fundamental physico-chemical importance. Electric field (Kerr effect) orientation of DNA in free solution as well as migration of DNA in gel electrophoresis are two well-established, but so far rather separate, research fields. Whereas the first one has been generally concerned with basic structural and dynamical properties of DNA (Charney, 1988), the second is closely related to techniques of molecular biology (for a review on DNA electrophoresis, see stellwagen 1987).

Polarized electronic spectra of Z-DNA single crystals

Polarized electronic absorption spectra of the (100) face of single crystals of the Z-form double helical duplex of d(m5CGUAm5CG) have been obtained from Kramers-Kronig analysis of reflection data. The c crystallographic axis is parallel to the helix axis and shows but weak absorption. The b axis is perpendicular to the helix axis and shows a structureless absorption band centered at 270 nm with an oscillator strength of 0.26. Calculations of the crystal spectra utilizing available transition moment data for the individual chromophores are carried through using the oriented gas model (no interbase interactions) and, again, employing all base-base interactions (point dipole) in the duplex. The calculated hypochromism of the 270 nm band is much less than the experimental value obtained from the crystal data. The crystal spectra appear to be representative of Z-form double helices of essentially infinite length and not of a collection of twelve base duplexes. No evidence for n pi* transitions polarized parallel to the helix axis is found.

The B-DNA to Z-DNA transition in alkali and tetraalkylammonium salts correlated with cation effects on solvent structure

The B-to-Z transition in DNA with alternating purine and pyrimidine sequences is driven by high concentrations of monovalent cations. In addition to screening of phosphate repulsion, an important factor may be the influence of ions on DNA hydration. The relative efficiencies of tetraalkylammonium and alkali metal salts in promoting the formation of Z-DNA, monitored by CD, in poly[d(G-C)] and poly[d(G-m5C)] was correlated with the degree to which the cations tie up water molecules in ordered arrangements and therefore decrease the availability of the solvent to hydrate DNA.