CD of the Li-salt of DNA in ethanol/water mixtures: evidence for the B- to C-form transition in solution

Effect of Soybean Protein Concentrate Preparation on Copy Numbers and Structural Characteristics of DNA from Genetically Modified Soybean

To regulate the degradation of transgenic DNA and lay theoretical foundations for the rational utilization of genetically modified (GM) products, variations in copy numbers and structural characteristics of DNA from GM soybean event GTS 40-3-2 during soybean protein concentrate (SPC) preparation were evaluated. Results showed that defatting and the first ethanol extraction were key procedures inducing DNA degradation. After these two procedures, copy numbers of the lectin and cp4 epsps targets decreased by more than 4 × 10⁸, occupying 36.88-49.30% of the total copy numbers from raw soybean. Atomic force microscopy images visually revealed the degradation of DNA that thinned and shortened during SPC preparation. Circular dichroism spectra suggested a lower helicity of DNA from defatted soybean kernel flour and a conformation transition of DNA from B-type to A-type after ethanol extraction. The fluorescence intensity of DNA decreased during SPC preparation, verifying the DNA damage along this preparation chain.

Melting transition of oriented Li-DNA fibers submerged in ethanol solutions

The melting transition of Li-DNA fibers immersed in ethanol-water solutions has been studied using calorimetry and neutron diffraction techniques. The data have been analyzed using the Peyrard-Bishop-Dauxois model to determine the strengths of the intra- and inter-base pair potentials. The data and analysis show that the potentials are weaker than those for DNA in water. They become weaker still and the DNA less stable as the ethanol concentration increases but, conversely, the fibers become more compact and the distances between base pairs become more regular. The results show that the melting transition is relatively insensitive to local confinement and depends more on the interaction between the DNA and its aqueous environment.

Nucleic acid binding mechanism of flavone derivative, riviciclib: Structural analysis to unveil anticancer potential

Despite burgeoned knowledge about the origin, growth, tissue interactions, and spread of cancer in recent years, the functional complexity and unique survival ability of cancer cells still make it difficult to target them. Riviciclib is a semi-synthetic derivative of rohitukine and possesses anticancer potential. Inhibition of nucleic acid activity in an uncontrolled dividing cell can form the basis for the development of new-age cancer therapeutics. The present study reports the molecular interaction between riviciclib and nucleic acid (DNA/tRNA) using spectroscopic and molecular docking studies in an attempt to comprehend its cellular toxicity as well as the nature and mode of binding between them. Vibrational spectroscopic results suggest that riviciclib intercalates DNA duplex and primarily binds with guanine, adenine, and thymine nucleobases. While in the case of riviciclib-tRNA complexation, riviciclib interacts mostly with uracil residues of the tRNA molecule. Besides nucleobases, riviciclib interacts with the sugar-phosphate backbone of both biomacromolecules. Conformationally, DNA alters from B-form to C-form, whereas tRNA shows no change in its native A-form. The order (10⁴ M^-1) of binding constant for riviciclib-nucleic acid complexation infer moderate to strong affinity of riviciclib with DNA and tRNA, respectively. Molecular docking explorations are further in corroboration with our spectroscopic outcomes.

The chromatin nuclear protein NUPR1L is intrinsically disordered and binds to the same proteins as its paralogue

NUPR1 is a protumoral multifunctional intrinsically disordered protein (IDP), which is activated during the acute phases of pancreatitis. It interacts with other IDPs such as prothymosin α, as well as with folded proteins such as the C-terminal region of RING1-B (C-RING1B) of the Polycomb complex; in all those interactions, residues around Ala33 and Thr68 (the ‘hot-spot’ region) of NUPR1 intervene. Its paralogue, NUPR1L, is also expressed in response to DNA damage, it is p53-regulated, and its expression down-regulates that of the NUPR1 gene. In this work, we characterized the conformational preferences of isolated NUPR1L and its possible interactions with the same molecular partners of NUPR1. Our results show that NUPR1L was an oligomeric IDP from pH 2.0 to 12.0, as judged by steady-state fluorescence, circular dichroism (CD), dynamic light scattering, 1D 1H-NMR (nuclear magnetic resonance), and as indicated by structural modelling. However, in contrast with NUPR1, there was evidence of local helical- or turn-like structures; these structures were not rigid, as judged by the lack of sigmoidal behaviour in the chemical and thermal denaturation curves obtained by CD and fluorescence. Interestingly enough, NUPR1L interacted with prothymosin α and C-RING1B, and with a similar affinity to that of NUPR1 (in the low micromolar range). Moreover, NUPR1L hetero-associated with NUPR1 with an affinity of 0.4 µM and interacted with the ‘hot-spot’ region of NUPR1. Thus, we suggest that the regulation of NUPR1 gene by NUPR1L does not only happen at the DNA level, but it could also involve direct interactions with NUPR1 natural partners.

The Cyanobacterial Ribosomal-Associated Protein LrtA from Synechocystis sp. PCC 6803 Is an Oligomeric Protein in Solution with Chameleonic Sequence Properties

The LrtA protein of Synechocystis sp. PCC 6803 intervenes in cyanobacterial post-stress survival and in stabilizing 70S ribosomal particles. It belongs to the hibernating promoting factor (HPF) family of proteins, involved in protein synthesis. In this work, we studied the conformational preferences and stability of isolated LrtA in solution. At physiological conditions, as shown by hydrodynamic techniques, LrtA was involved in a self-association equilibrium. As indicated by Nuclear Magnetic Resonance (NMR), circular dichroism (CD) and fluorescence, the protein acquired a folded, native-like conformation between pH 6.0 and 9.0. However, that conformation was not very stable, as suggested by thermal and chemical denaturations followed by CD and fluorescence. Theoretical studies of its highly-charged sequence suggest that LrtA had a Janus sequence, with a context-dependent fold. Our modelling and molecular dynamics (MD) simulations indicate that the protein adopted the same fold observed in other members of the HPF family (β-α-β-β-β-α) at its N-terminal region (residues 1–100), whereas the C terminus (residues 100–197) appeared disordered and collapsed, supporting the overall percentage of overall secondary structure obtained by CD deconvolution. Then, LrtA has a chameleonic sequence and it is the first member of the HPF family involved in a self-association equilibrium, when isolated in solution.

Boundary conditions for free A-DNA in solution and the relation of local to global DNA structures at reduced water activity

Because of repeated claims that A-DNA cannot exist without aggregation or condensation, the state of DNA restriction fragments with 84–859 bp has been analyzed in aqueous solutions upon reduction of the water activity. Rotational diffusion times τ^d measured by electric dichroism at different water activities with a wide variation of viscosities are normalized to values τ^c at the viscosity of water, which indicate DNA structures at a high sensitivity. For short helices (chain lengths \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\ell} $$\end{document}ℓ ≤ persistence length p), cooperative formation of A-DNA is reflected by the expected reduction of the hydrodynamic length; the transition to the A-form is without aggregation or condensation upon addition of ethanol at monovalent salt ≤1 mM. The aggregation boundary, indicated by a strong increase of τ^c, is shifted to higher monovalent salt (≥4 mM) when ethanol is replaced by trifluoroethanol. The BA transition is not indicated anymore by a cooperative change of τ^c for \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\ell} $$\end{document}ℓ » p; τ^c values for these long chains decrease upon reduction of the water activity continuously over the full range, including the BA transition interval. This suggests a non-cooperative BC transition, which induces DNA curvature. The resulting wide distribution of global structures hides changes of local length during the BA transition. Free A-DNA without aggregation/condensation is found at low-salt concentrations where aggregation is inhibited and/or very slow. In an intermediate range of solvent conditions, where the A-form starts to aggregate, a time window remains that can be used for analysis of free A-DNA in a quasi-equilibrium state.

Sequence-selective DNA binding with cell-permeable oligoguanidinium–peptide conjugates

Conjugation of a short peptide fragment from a bZIP protein to an oligoguanidinium tail results in a DNA-binding miniprotein that selectively interacts with composite sequences containing the peptide-binding site next to an A/T-rich tract.

Unequal effect of ethanol-water on the stability of ct-DNA, poly[(dA-dT)]₂ and poly(rA)·poly(rU). Thermophysical properties

Ethanol affects unequally the thermal stability of DNA and RNA. It stabilizes RNA, while destabilizing DNA. The variation of the relative viscosity (η/η0) of [poly(dA-dT)]2 with temperature unveils transitions close to the respective denaturation temperature, calculated spectrophotometrically and calorimetrically. From the raw data densities and speeds of sound, the volumetric observables were calculated. In all cases studied, a change in sign from low to high ethanol content occurred for both partial molar volume (ϕV) and partial molar adiabatic compressibility (ϕK(S)). The minima, close to 10%, should correspond to the highest solvation and the maxima, close to 30%, to the lowest solvation. For 40-50% ethanol, the solvation increases again. The complex structure of ethanol-water, for which changes are observed in regions close to such critical concentrations, justifies the observed behaviour. The variation of ϕV and ϕK(S) was sharper for RNA compared with respect to DNA, indicating that the solvation sequence is poly(rA)·poly(rU) < ct-DNA < [poly(dA-dT)]2.

A structural insight into major groove directed binding of nitrosourea derivative nimustine with DNA: a spectroscopic study

Nitrosourea therapeutics occupies a definite place in cancer therapy but its exact mechanism of action has yet to be established. Nimustine, a chloroethyl nitrosourea derivative, is used to treat various types of malignancy including gliomas. The present work focuses on the understanding of nimustine interaction with DNA to delineate its mechanism at molecular level. Attenuated total reflection-Fourier transform infrared (ATR-FTIR) has been used to determine the binding sites of nimustine on DNA. Circular dichroism (CD) spectroscopy has been used to confirm conformational variations in DNA molecule upon nimustine-DNA interaction. Thermodynamic parameters of nimustine-DNA reaction have been calculated by isothermal titration calorimetry. Results of the present study demonstrate that nimustine is not a simple alkylating agent rather it causes major grove-directed-alkylation. Spectroscopic data suggest binding of nimustine with nitrogenous bases guanine (C6 = O6) and thymine (C4 = O4) in DNA major groove. CD spectra of nimustine-DNA complexes point toward the perturbation of native B-conformation of DNA and its partial transition into C-form. Thermodynamically, nimustine-DNA interaction is an entropy driven endothermic reaction, which suggests hydrophobic interaction of nimustine in DNA-major groove pocket. Spectral results suggest base binding and local conformational changes in DNA upon nimustine interaction. Investigation of drug-DNA interaction is an essential part of rational drug designing that also provides information about the drug's action at molecular level. Results, demonstrated here, may contribute in the development of new nitrosourea therapeutics with better efficacy and fewer side effects.

Linear dichroism of chlorosomes from chloroflexus aurantiacus in compressed gels and electric fields

The linear dichroism of chlorosomes from Chloroflexus aurantiacus was measured between 250 and 800 nm. To orient the chlorosomes we used a new way of compressing polyacrylamide gels, where the dimension of the gel along the measuring light-beam is kept constant. The press required for such a way of compressing is relatively easy to construct. A theoretical description is given to interpret the measured linear dichroism in terms of the orientation of the transition moments. The results obtained with the polyacrylamide gels are compared with the linear dichroism measurements for chlorosomes oriented in electric fields. Both the spectral features as well as the absolute size of the linear dichroism signals are in reasonable agreement. We find that the transition moment corresponding to the 741 nm bacteriochlorophyll c (Bchl c) absorption band makes an angle of 20 degrees with the long axis of the chlorosome. For the 461 nm Bchl c band an angle of 30 degrees is found. Both angles are significantly lower than the values reported so far in literature and they imply that Bchl c is highly organized in the chlorosomes.

On structural transitions, thermodynamic equilibrium, and the phase diagram of DNA and RNA duplexes under torque and tension

A precise understanding of the flexibility of double stranded nucleic acids and the nature of their deformed conformations induced by external forces is important for a wide range of biological processes including transcriptional regulation, supercoil and catenane removal, and site-specific recombination. We present, at atomic resolution, a simulation of the dynamics involved in the transitions from B-DNA and A-RNA to Pauling (P) forms and to denatured states driven by application of external torque and tension. We then calculate the free energy profile along a B- to P-transition coordinate and from it, compute a reversible pathway, i.e., an isotherm of tension and torque pairs required to maintain P-DNA in equilibrium. The reversible isotherm maps correctly onto a phase diagram derived from single molecule experiments, and yields values of elongation, twist, and twist-stretch coupling in agreement with measured values. We also show that configurational entropy compensates significantly for the large electrostatic energy increase due to closer-packed P backbones. A similar set of simulations applied to RNA are used to predict a novel structure, P-RNA, with its associated free energy, equilibrium tension, torque and structural parameters, and to assign the location, on the phase-diagram, of a putative force-torque-dependent RNA "triple point."

Cationic lipids and cationic ligands induce DNA helix denaturation: detection of single stranded regions by KMnO4probing

Cationic lipids and cationic polymers are widely used in gene delivery. Using 1,2-dioleoyl-3-trimethylammonium-propane (DOTAP) as a cationic lipid, we have investigated the stability of the DNA in DOTAP:DNA complexes by probing with potassium permanganate (KMnO4). Interestingly, thymidines followed by a purine showed higher susceptibility to cationic ligand-mediated melting. Similar studies performed with other water-soluble cationic ligands such as polylysine, protamine sulfate and polyethyleneimine also demonstrated melting of the DNA but with variations. Small cations such as spermine and spermidine and a cationic detergent, cetyl trimethylammonium bromide, also rendered the DNA susceptible to modification by KMnO4. The data presented here provide direct proof for melting of DNA upon interaction with cationic lipids. Structural changes subsequent to binding of cationic lipids/ligands to DNA may lead to instability and formation of DNA bubbles in double-stranded DNA.

The structure of DNA within cationic lipid/DNA complexes

The structure of DNA within CLDCs used for gene delivery is controversial. Previous studies using CD have been interpreted to indicate that the DNA is converted from normal B to C form in complexes. This investigation reexamines this interpretation using CD of model complexes, FTIR as well as Raman spectroscopy and molecular dynamics simulations to address this issue. CD spectra of supercoiled plasmid DNA undergo a significant loss of rotational strength in the signal near 275 nm upon interaction with either the cationic lipid dimethyldioctadecylammonium bromide or 1,2-dioleoyltrimethylammonium propane. This loss of rotational strength is shown, however, by both FTIR and Raman spectroscopy to occur within the parameters of the B-type conformation. Contributions of absorption flattening and differential scattering to the CD spectra of complexes are unable to account for the observed spectra. Model studies of the CD of complexes prepared from synthetic oligonucleotides of varying length suggest that significant reductions in rotational strength can occur within short stretches of DNA. Furthermore, some alteration in the hydrogen bonding of bases within CLDCs is indicated in the FTIR and Raman spectroscopy results. In addition, alterations in base stacking interactions as well as hydrogen bonding are suggested by molecular dynamics simulations. A global interpretation of all of the data suggests the DNA component of CLDCs remains in a variant B form in which base/base interactions are perturbed.

Structural changes in DNA mediated by cationic lipids alter in vitro transcriptional activity at low charge ratios

Lipid/DNA complexes or Lipoplexes have been characterized by various biochemical and biophysical methods to understand the physical basis of transfection. Here we have addressed the effect of cationic liposomes, 1,2-dioleoyl-3-trimethylammonium-propane (DOTAP), on transcription of DNA templates in vitro. Transcriptional activity of DNA-dependent RNA polymerase at DNA templates complexed with the cationic lipid varied as a function of charge ratio of lipid/DNA. At low charge ratios of 0.3:1 lipid/DNA and up to 1:1, we observed stimulation in transcription, while at higher charge ratios of lipid/DNA 3:1, complete inhibition in the activity occurred. Cetyl tri-methyl ammonium bromide (CTAB), a cationic detergent, and polyethylenimine (PEI), a cationic polymer, also bring about similar changes although to a lesser extent. The stimulation in transcription motivated us to probe into the molecular nature of the lipid/DNA interactions by absorbance spectroscopy and circular dichroism (CD). Upon interaction with lipids, hyperchromicity and susceptibility to micrococcal nuclease has increased, which suggests that the DNA was partially denatured. On complexation with the cationic lipid (DOTAP), the magnitude of the positive band in CD spectra decreased, accompanied with a red shift, as a function of charge ratio. Results from spectroscopic and enzyme assays suggest that at low charge ratios DNA may be partially unwound.

Molecular dynamics simulation of nucleic acids

We review molecular dynamics simulations of nucleic acids, including those completed from 1995 to 2000, with a focus on the applications and results rather than the methods. After the introduction, which discusses recent advances in the simulation of nucleic acids in solution, we describe force fields for nucleic acids and then provide a detailed summary of the published literature. We emphasize simulations of small nucleic acids ( approximately 6 to 24 mer) in explicit solvent with counterions, using reliable force fields and modern simulation protocols that properly represent the long-range electrostatic interactions. We also provide some limited discussion of simulation in the absence of explicit solvent. Absent from this discussion are results from simulations of protein-nucleic acid complexes and modified DNA analogs. Highlights from the molecular dynamics simulation are the spontaneous observation of A B transitions in duplex DNA in response to the environment, specific ion binding and hydration, and reliable representation of protein-nucleic acid interactions. We close by examining major issues and the future promise for these methods.

Effect of polyethylene glycol on the supercoiling free energy of DNA

The supercoiling free energy of pUC19 DNA [2686 base pairs (bp)] was measured in various concentrations of PEG 8000 (polyethylene glycol; molecular weight 8000) by the topoisomer distribution method. The effective twist energy parameter (E(T)) that governs the supercoiling free energy declined linearly by 1.9-fold with increasing w/v % PEG from 0 to 7.5%, which lies below the threshold for intermolecular condensation. In principle, PEG could affect E(T) either via an osmotic exclusion mechanism or by altering the torsion elastic constant, bending rigidity, or self-repulsions of the DNA. Possible alterations of the DNA secondary structure and torsion elastic constant were assessed by CD spectroscopy and time-resolved fluorescence polarization anisotropy of intercalated ethidium. Up to 7.5% PEG, the secondary structure of the DNA remained largely unaltered, as evidenced by (1) the absence of any significant change in the CD spectrum, (2) an extremely small relative decrease (-0.0013) in intrinsic twist, and (3) a negligibly small change in the torsion elastic constant. The observed reduction in E(T) cannot be ascribed primarily to a decrease in torsion elastic constant, and most likely does not stem from a decrease in bending rigidity either. The decrease in medium dielectric constant due to PEG should increase the self-repulsions, and thereby increase E(T), which is opposite to the observed trend. Instead, the observed decline in E(T) is attributed to an osmotic exclusion mechanism. The change in molar volume excluded to the PEG (Delta V(ex)), when the linking difference converts from Delta l = 0 to Delta l = +/-1, was determined from the observed E(T) value and PEG osmotic pressure at each concentration. The experimental Delta V(ex) values agree well with theoretical estimates reckoned for a simple osmotic exclusion model, in which PEG is excluded by hard-core interactions from a concentric cylindrical volume around every duplex segment. The difference in volume excluded to PEG between the Delta l = 0 and the Delta l = +/-1 topoisomers is attributed entirely to the approximately 0.7 additional writhe "crossing" of two duplex strands at roughly 90 degrees, which is known to occur in the latter species. When the separation between the duplex centers at the "crossing" was adjusted so that the theoretical estimate of Delta V(ex) matched the experimental value at each PEG concentration, a value near 5.7 nm was obtained in each case. The invariance and plausible magnitude of this mean separation at the crossing provide strong support for this simple osmotic exclusion model. An alternative model, in which the PEG is excluded from the entire coil envelope of the DNA out to its radius of gyration, perhaps because it decreases the local dielectric constant, was also considered. The estimated difference in excluded volume in that case exceeds the experimental value by a factor of nearly 10(4), and could be ruled out on that basis.

BII nucleotides in the B and C forms of natural-sequence polymeric DNA: A new model for the C form of DNA

A combination of solid-state (31)P and (13)C NMR, X-ray diffraction, and model building is used to show that the B and C forms of fibrous macromolecular DNA consist of two distinct nucleotide conformations, which correspond closely to the BI and BII nucleotide conformations known from oligonucleotide crystals. The proportion of the BII conformation is higher in the C form than in the B form. We show structural models for a 10(1) double helix involving BI nucleotides and a 9(1) double helix involving BII nucleotides. The 10(1) BI model is similar to a previous model of B-form DNA, while the 9(1) BII model is novel. The BII model has a very deep and narrow minor groove, a shallow and wide major groove, and highly inclined bases. This work shows that the B to C transition in fibers corresponds to BI to BII conformational changes of the individual nucleotides.

Conformational transition of DNA in electroreduction studied by in situ UV and CD thin layer spectroelectrochemistry

Electrochemically induced three conformational transitions of calf thymus DNA from B10.4 to Z10.2-DNA and from B10.2 to B10.4 and to C-DNA in 10 mM phosphate buffer solution (pH 7.21) at glassy carbon electrode are found and studied by in situ circular dichroism (CD) thin layer spectroelectrochemistry with singular value decomposition least square (SVDLS) analysis. It indicates that the so-called B10.2 form and the C-form of DNA may be composed of B10.4 and left-A DNA and of B10.4 and right-A DNA, respectively. The irreversible electrochemical reduction of adenine and cytosine groups in the DNA molecule is studied by UV-Vis spectroelectrochemistry. Some electrochemical parameters alpha n = 0.17, E0' = -0.70 V (vs. Ag/AgCl), and the standard heterogeneous electron transfer rate constant, k0 = 1.8 x 10(-5) cm s(-1), are obtained by double logarithmic analysis and non-linear regression.

The question of long-range allosteric transitions in DNA

The question of long-range allosteric transitions of DNA secondary structure and their possible involvement in transcriptional activation is discussed in the light of new results. A variety of recent evidence strongly supports a fluctuating long-range description of DNA secondary structure. Balanced equilibria between two or more different secondary structures, and the occurrence of very large domain sizes, have been documented in several instances. Long-range allosteric effects stemming from changes in sequence or secondary structure over a small region of the DNA have been observed to extend over distances up to hundreds of base pairs in some cases. The discovery that coherent bending strain beyond a threshold level in small (N < or = 250 base pairs (bp)] circular DNAs significantly alters the DNA secondary structure has important implications, especially for transcriptional activators that either bend the DNA directly or are involved in the formation of DNA loops of sufficiently small size (N < or = 250 bp). Whether the RNA polymerase is activated primarily via protein: protein contacts, as is widely believed, or instead via a bend-induced allosteric transition of the DNA in such a small loop, is now an open question. Binding of the transcriptional activator Sp1 to linear DNA induces a remarkably long-range change in its secondary structure, and catabolite activator protein binding to a supercoiled DNA behaves similarly, though possibly for different reasons. Compelling evidence for a bend-induced long-range structural transmission effect of the transcriptional activator integration host factor on RNA polymerase activity was recently reported. These results may augur a new paradigm in which allosteric transitions of duplex DNA, as well as of the proteins, are involved in the regulation of transcription.

Effect of temperature on DNA secondary structure in the absence and presence of 0.5 M tetramethylammonium chloride

Changes in the average secondary structures of three different linear DNAs over the premelting region from 5 to 60 degrees C were investigated by measuring their CD spectra and also their torsion elastic constants (<alpha>) by time-resolved fluorescence polarization anisotropy. For one of these DNAs, the Haell fragment of pBR322, the apparent diffusion coefficients [Dapp(k)] at small and large scattering vectors (k) were also measured by dynamic light scattering. With increasing temperature, all three DNAs exhibited typical premelting changes in their CD spectra, and these were accompanied by 1.4- to 1.7-fold decreases in <alpha>. Also for the 1876 base pair fragment, Dapp(k) at large scattering vectors, which is sensitive to the dynamic bending rigidity, decreased by 17%, even though there was no change at small scattering vectors, where Dapp(k) = D0 is the translational diffusion coefficient of the center-of-mass. These observations demonstrate conclusively that the premelting CD changes of these DNAs are associated with a significant change in average secondary structure and mechanical properties, though not in persistence length. In the presence of 0.5 M tetramethylammonium chloride (TMA-Cl) the premelting change in CD is largely suppressed, and the corresponding changes in <alpha> and Dapp(k) at large scattering vectors are substantially diminished. These observations suggest that TMA-Cl, which binds preferentially to A.T-rich regions and stabilizes those regions (relative to G.C-rich regions) against melting, effectively stabilizes the prevailing low-temperature secondary structure sufficiently that the DNA is effectively trapped in that state over the temperature range observed.

Analysis of plasmid DNA from a pharmaceutical perspective

The advent of gene therapy and polynucleotide-based vaccines has resulted in the use of plasmid DNA as a drug substance. Although biologically (cell or animal) based assays must currently be employed to establish the identity and potency of such drugs, we argue that in the future, a combination of microchip-based mutation detection devices combined with an array of chromatographic, electrophoretic, hydrodynamic, and spectroscopic methods can be employed to rigorously establish these properties. We review a variety of such methods in this context and also consider the issue of the chemical stability of plasmids. Extensive comparison is made to protein-based pharmaceuticals with the unique importance of polynucleotide sequence emphasized in comparison to protein tertiary structure.

A molecular level picture of the stabilization of A-DNA in mixed ethanol-water solutions

Advances in computer power, methodology, and empirical force fields now allow routine "stable" nanosecond-length molecular dynamics simulations of DNA in water. The accurate representation of environmental influences on structure remains a major, unresolved issue. In contrast to simulations of A-DNA in water (where an A-DNA to B-DNA transition is observed) and in pure ethanol (where disruption of the structure is observed), A-DNA in approximately 85% ethanol solution remains in a canonical A-DNA geometry as expected. The stabilization of A-DNA by ethanol is likely due to disruption of the spine of hydration in the minor groove and the presence of ion-mediated interhelical bonds and extensive hydration across the major groove.

Aggregated DNA in ethanol solution

A recently developed mechanochemical method has provided a new, efficient tool for studies on the thermal stability and structure of aggregated DNA in ethanol-water solutions. At low ethanol concentrations DNA is fully soluble and is in the B form. However, with increasing ethanol concentration the melting temperature of DNA, Tm, decreases. At a critical ethanol concentration, dependent on the nature and concentration of the counterion, aggregation of the DNA molecules sets in. This is reflected in a marked increase in Tm indicating that the aggregated DNA molecules are thermally more stable than the dissolved ones. However, they are still in the B form. In general, Tm of aggregated DNA also decreases with further increasing ethanol concentration and is dependent on the nature of the counterion, but Tm is not affected by the concentration of the counterion (excess salt) in the ethanol-water solution. When the ethanol concentration reaches the range of 70-80% (v/v), the B-to-A conformational transition occurs in the case of Na-, K- and CsDNA. Above this transition point the A form is more stable than the B form due to the reduced water activity and to increased interhelical interactions. At very high ethanol concentrations, above 85% and dependent on the nature of the counterion, a drastic change in the thermal behaviour is observed. Apparently such a strong interhelical interaction is induced in the aggregated DNA that the DNA is stabilized and cannot adopt a random coil state even at very high temperatures. This stability of DNA in the P form is fully reversed if the ethanol concentration is lowered and the activity of water, thereby, is restored.

Ultraviolet absorbance and circular dichroism of Pf1 virus: nucleotide/subunit ratio of unity, hyperchromic tyrosines and DNA bases, and high helicity in the subunits

Data have been obtained for the Pf1 virion that establish its stoichiometry and conformational features of its DNA and its protein. The absorbance spectrum of the dissociated virus under alkaline denaturing conditions is fit exactly by spectra for DNA and protein at a mole ratio of one nucleotide per protein subunit. This result, together with three previous values by independent methods, establishes that the nucleotide/subunit ratio (n/s) of Pf1 is unity. The absorbance spectrum of DNA in the intact native virus is assigned as the spectrum for heat denatured Pf1 DNA, with epsilon (P) = 8400 M-1 cm-1 at 259 nm. The absorbance spectrum assigned to protein (two tyrosines) in the intact virus has <epsilon (Y)> = 2500 M-1 cm-1 per tyrosine at lambda max of 281.5 nm; this is the most red-shifted and hyperchromic tyrosine spectrum known. The CD spectrum of the intact virus from 250 to 320 nm has no apparent DNA contribution, but has a strong contribution from the red-shifted tyrosine(s). The CD spectrum from 185 to 250 nm has the shape of alpha-helical CD reference spectra, but is perceptibly blue-shifted, with a crossover from negative to positive ellipticity at 199.7 nm, and it has very high amplitudes (e.g. [theta 207.5nm] = -44,000 deg cm2 dmol-1). This spectrum indicates completely helical protein in the virus, with a predominance of alpha-helix and perhaps some 3(10)-helix. The unit n/s ratio, the high absorbance and negligible near-UV CD for the DNA bases, and the high amplitudes for the helical protein are critical input data for the determination of Pf1 virus structure.

Dynamics and structures of DNA: long-range effects of a 16 base-pair (CG)8 sequence on secondary structure

The effects of inserting 16 base pair (bp) of alternating CG [(CG)8] near the middle of a much longer restriction fragment (1097 bp) are investigated by measuring various properties that are sensitive to secondary and tertiary structure. Results for this fragment are compared with those for a control fragment (1089 bp) with the identical sequence except at the insert. Another fragment (1382 bp), which contains a 296-bp extension at the 5'-end of the 1089-bp control fragment, is also used as a secondary control in some experiments. When the 1097-bp (CG)8 insert fragment is compared with the control fragments in 0.1 M NaCl buffer, the (CG)8 insert is found to induce disproportionately large relative changes in the molar ellipticity at 273 nm ([theta]273), the torsion constant (alpha) measured by fluorescence polarization anisotropy, the optical melting profile, and the susceptibility to S1 nuclease. Estimates of the minimum distance over which the (CG)8 insert alters the secondary structure range from 330 to 550 bp. With increasing NaCl concentration, the 1097-bp insert fragment undergoes a structural transition between 2.0 and 2.5 M that is manifested in the apparent diffusion coefficient (Dplat) from dynamic light scattering at large scattering vector. This transition, which is not exhibited by the control DNAs, is presumed to involve formation of Z-helix at the insert. However, the observed decrease in (Dplat) is attributed to an increase in bending rigidity, which perforce must be globally distributed far beyond the (CG)8 insert per se. In 4.25 M NaCl (but not in 0.1 M NaCl), the addition of 1 ethidium dye per 300 bp induces an extensive structural transition in the 1097 bp (CG)8 insert fragment. This transition, which also is not exhibited by the control DNAs, significantly decreases the bending rigidity, doubles [theta]273, and takes place on a time scale of a few days. Removal of ethidium and salt by dialysis vs 0.1 M NaCl buffer restores the original properties of the 1097-bp (CG)8 insert fragment. The present results are consistent with a (fluctuating, long-range) description of the secondary structure in which a given short sequence transiently fluctuates among two or more distinct secondary structures that extend over much larger domains of variable position and size, and whose relative stabilities depend on distant as well as close-lying base pairs.

Further characterization of structural and electric properties of non-spherical alpha-crystallin

Recently we have shown that the population of native alpha-crystallin, isolated using size-exclusion chromatography from eye lenses of calves, is multimodal. Most of the protein probably possesses an almost spherical appearance, but at least one of the other modes represents more extended, ellipsoidally and/or cylindrically shaped molecules [Van Haeringen, B., Eden, D., Van den Bogaerde, M.R., Van Grondelle, R. & Bloemendal, M. (1992) Eur. J. Biochem. 210, 211-216]. In the present study, we characterize various subpools of a single alpha-crystallin size-exclusion chromatography elution peak by means of transient-electric-birefringence measurements, ultraviolet linear-dichroism spectroscopy and analytical fast protein liquid chromatography. It is concluded that the fractions have a well-defined stable mass and are not in reversible equilibrium with each other. All pools appear to be composed of at least two types of differently shaped molecules. The hydrodynamic dimensions and electric properties of the different alpha-crystallin species are characterized. The non-spherical alpha-crystallin is found to be optically and electrically more anisotropic, and to contain a larger permanent electric dipole moment than the spherical form. A model for the composition of the alpha-crystallin pool is presented.

New insights into sequence recognition process of esperamicin A1 and calicheamicin gamma 1I.: origin of their selectivities and "induced fit" mechanism

This study addresses the DNA sequence recognition event of the enediyne antibiotics esperamicin A1 and calicheamicin gamma 1I by the use of synthetic DNA oligomers, salt effects, and circular dichroism studies. The results reported here provide several important insights: (1) esperamicin A1 requires a purine/pyrimidine trimer in host DNA for favorable interaction, (2) the sequence selectivity of esperamicin C is an origin of esperamicin A1 and calicheamicin gamma 1I selectivities, (3) in the target recognition by esperamicin C, its total structure and hydrophobicity are important, and (4) the binding of hydrophobic esperamicin to DNA duplex induces dehydration and conformational change of the host DNA. The specific sequence recognition process of esperamicin/calicheamicin has been discussed.

Alpha-crystallin exists in a non-spherical form. A study on the rotational properties of native and reconstituted alpha-crystallin

Native alpha-crystallin, obtained from the cortex of calf lenses with FPLC (Pharmacia) was characterized by means of transient-electric-birefringence measurements and ultraviolet linear-dichroism spectroscopy. These techniques were also performed on 6-M-urea-dissociated and reconstituted alpha-crystallin. Transient-electric-birefringence measurements offer the possibility to characterize the often observed, but usually neglected, non-spherical occurrences of alpha-crystallin in more detail. Although not distinguishable with size-exclusion chromatography, we could identify at least two different classes of both native and reconstituted alpha-crystallin, from which at least one consists of non-spherical molecules. The results are compared with those obtained with electron microscopy using different staining methods. From the three independent techniques used we find evidence that a fraction of the alpha-crystallin exists in a more extended quaternary structure. The results are difficult to explain with a concentric three-layer model for alpha-crystallin as proposed by Tardieu et al. [Tardieu, A., Laporte, D., Licinio, P., Krop, B. & Delaye, M. (1986) J. Mol. Biol. 192, 711-724].

Structural alterations of double-stranded DNA in complex with the adenovirus DNA-binding protein. Implications for its function in DNA replication

The Adenovirus DNA-binding protein (DBP) binds to single-stranded (ss) DNA as well as to double-stranded (ds) DNA and forms multimeric protein-DNA complexes with both. Gel retardation assays indicate rapid complex formation for both DNAs. DBP rapidly dissociates from dsDNA, indicating a dynamic equilibrium, whereas the ssDNA-DBP complex is much more stable. We investigated the complex between DBP and dsDNA in more detail. Electron microscopical analysis shows thick filament-like and beaded structures in which the length of the DNA is not significantly altered. Cryo-electron micrographs suggest the presence of interwound protein fibres around the DNA. Ligase-mediated cyclization, but not linear multimerization, of DBP-saturated DNA fragments exceeding the persistence length was severely inhibited. This suggests that DNA may be organized by DBP into a rigid structure. Under those conditions, DBP induces distinct changes in the circular dichroism spectrum of the DNA, indicative of structural DNA changes. No bending or twisting of the complex was observed. Hydroxyl radical footprinting showed that the breakdown pattern of DNA at saturating DBP concentrations is much more regular than the protein-free DNA. This suggests the removal of tertiary structures, which may be related to the effects of DBP on enhanced NFI binding and chain elongation during Adenovirus DNA replication. Using purified proteins in an in vitro replication system, we correlate the structural changes with the effects of DBP on enhancement of NFI-binding as well as on DNA replication.

Changes in the c.d. spectra of calf thymus DNA induced by sequential polypeptides in aqueous solutions. Part I

Interactions of calf thymus DNA with sequential polypeptides were studied using c.d. spectroscopy in aqueous solutions. It was found that DNA structural alterations induced by sequential polypeptides (L-Arg-X-Gly)n (where X = L-Val, Leu, Ile, Nva, Nle) are modulated by the nature of the X residue. Thus, the polypeptide (L-Arg-L-Nva-Gly)n induced the 10.2B-DNA form, whereas the polypeptides (L-Arg-L-Ile-Gly)n having one methyl group less on the X residue side chain, did not provide any significant modification to the structure of DNA. The effect of ionic strength from 0.14 M NaCl (physiological value) to zero was also analysed on the basis of the observed c.d. changes and the degree of complexation in the DNA-polypeptides was estimated.

Non-random conformation of a mouse IgG2a monoclonal antibody at low pH

The pH dependence of the conformation of a mouse IgG2a, kappa monoclonal antibody (MN12) was investigated by several physical techniques, including fluorescence spectroscopy, near-ultraviolet and far-ultraviolet CD, and electric-field-induced transient birefringence measurements. The intensity of the intrinsic tryptophan fluorescence remained constant in the pH range from 3.5 to 10.0. A conformational alteration in the MN12 molecule was observed in the pH region between pH 3.5 and 2.5, as reflected by a substantial enhancement of the fluorescence quantum yield. This effect was more pronounced at high ionic strengths. The fluorescence emission was unaltered, indicating that the acid-induced conformational state is different from a completely unfolded state. This was confirmed by CD and fluorescence polarisation measurements. Iodide and acrylamide fluorescence quenching studies indicated a gradually increasing accessibility of MN12 tryptophan residues with decreasing pH. At low pH precipitation was observed in the presence of iodide. One rotational relaxation time (0.16-0.18 microseconds) was observed for MN12 by electric-field-induced transient birefringence measurements at low ionic strength. After exposure of MN12 to low pH for 1 h, the relaxation time was increased to 0.23 microseconds; a further increase to 0.30 microseconds was observed after 24 h. The combined results suggest an acid-induced expansion and enhanced flexibility of MN12, which eventually leads to irreversible aggregation.

A circular dichroism study on the conformation of d(CGT) modified with N-acetyl-2-aminofluorene or 2-aminofluorene

The trinucleotide d(CGT) was modified by covalent binding of the carcinogen N-acetyl-2-aminofluorene (AAF) or 2-aminofluorene (AF) at the C8 position of the guanine base. The conformations of d(CGT)-AAF and -AF were studied by comparing the absorption and circular dichroism properties with those of dCMP + dGMP-AAF or -AF + dTMP in a molar ratio of 1:1:1 and AAF- and AF-containing dGMP. For both AAF- and AF-d(CGT) complexes the results show significant stacking interactions between the fluorene residue and the base(s) and are discussed in terms of the conformation of d(CGT)-AAF and -AF. In d(CGT)-AF we observe a clear interaction between AF and thymine, whereas the C-G stack is still intact. In the case of d(CGT)-AAF the C-G stack is weakened and the glycosidic rotation angle of dGuo-C8-AAF is most probably syn. The specific fluorene-base interactions persist at elevated temperatures. The carcinogen-base interactions are stronger in the AAF-carrying d(CGT) than in the case of the deacetylated complex. This is consistent with the higher mobility of the AF-adduct and its conformationally heterogeneous appearance in DNA.

Average orientation of aromatic residues in proteins determined from linear dichroism spectroscopy. A comparison of results on bovine gamma-crystallins with X-ray data

The structures of the two very closely related proteins, bovine gamma II- and gamma IVa-crystallin have been studied by means of near-ultra-violet linear dichroism spectroscopy on squeezed polyacrylamide gel systems. The crystallin spectra are discussed in terms of the spectra of the aromatic chromophores present in these proteins and provide detailed information on the average orientation of these residues in the proteins. A comparison of our results with information based on crystallographic X-ray experiments shows excellent agreement, reflecting even some of the minor differences between the two proteins studied. Since linear dichroism measurements as performed here take a few days only, and can be done on most aqueous protein solutions, linear dichroism spectroscopy may give a valuable contribution to structural studies on proteins.

Study of the binding of single-stranded DNA-binding protein to DNA and poly(rA) using electric field induced birefringence and circular dichroism spectroscopy

Binding of the single-stranded DNA-binding protein (SSB) of Escherichia coli to single-stranded (ss) polynucleotides produces characteristic changes in the absorbance (OD) and circular dichroism (CD) spectra of the polynucleotides. By use of these techniques, complexes of SSB protein and poly(rA) were shown to display two of the binding modes reported by Lohman and Overman [Lohman, T.M., & Overman, L. (1985) J. Biol. Chem. 260, 3594-3603]. The circular dichroism spectra of the "low salt" (10 mM NaCl) and "high salt" (greater than 50 mM NaCl) binding mode are similar in shape, but not in intensity. SSB binding to poly(rA) yields a complexed CD spectrum that shares several characteristics with the spectra obtained for the binding of AdDBP, GP32, and gene V protein to poly(rA). We therefore propose that the local structure of the SSB-poly(rA) complex is comparable to the structures proposed for the complexes of these three-stranded DNA-binding proteins with DNA (and RNA) and independent of the SSB-binding mode. Electric field induced birefringence experiments were used to show that the projected base-base distance of the complex is about 0.23 nm, in agreement with electron microscopy results. Nevertheless, the local distance between the successive bases in the complex will be quite large, due to the coiling of the DNA around the SSB tetramer, thus partly explaining the observed CD changes induced upon complexation with single-stranded DNA and RNA.

Structural principles of B-DNA grooves hydration in fibers as revealed by Monte Carlo simulations and X-ray diffraction

Being interested in possible effects of sequence-dependent hydration of B-DNA with mixed sequence in fibers, we performed a series of Monte Carlo calculations of hydration of polydeoxyribonucleotides in B form, considering all sequences with dinucleotide repeat. The computational results allow the ten base-stacking types to be classified in accordance with their primary hydration in the minor groove. As a rule, the minor groove is occupied by two water molecules per base pair in the depth of the groove, which are located nearly midway between the planes of successive base pairs and symmetrically according to the dyad there. The primary hydration of the major groove depends on the type of the given base pair. The coordinates of 3 water molecules per base pair in the depth of the major groove are determined by the type of this pair together with its position and orientation in the helix, and are practically independent on the adjacent base pairs. A/T-homopolymer tracts do not fit into this hydration pattern; the base pair edges are hydrated autonomously in both grooves. Analysis of the Li-B-DNA x-ray diffraction intensities reveals those two water positions in the minor groove. In the major groove, no electronic density peaks in sufficient distance from the base edges were found, thus confirming the absence of any helical invariance of primary hydration in this region. With the help of the rules proposed in this paper it is possible to position the water molecules of the first hydration shell in the grooves of canonical B-DNA for any given sequence.

A structural study of bovine lens alpha-crystallin and its subunits by absorption and linear dichroism spectroscopy

The structure of the bovine alpha-crystallin aggregate and its reaggregated isolated subunits has been studied by measurement of their absorption and linear dichroism spectra over the range 250-350 nm. Also, changes in structure with respect to time have been monitored in this way. From the absorption spectra it appears that the aromatic residues in subunit aggregates are in the same chemical environment as those in native protein. The light scattering due to the size of the protein molecules increases when the proteins are kept in solution, this effect being much stronger for the subunits. The linear dichroism spectra point to strong structural ordering in alpha-crystallin, the absorption transition dipoles of the aromatic residues being preferentially aligned along the long axis of the molecules. Moreover, a considerable deviation from a spherical or tetrahedrally symmetric structure of alpha-crystallin is inferred. The subunit aggregates show less ordering and might be more spherical. When kept in solution, their structural order seems to be decreased. The linear dichroism spectra show absorption at 325 nm, which is not detectable in the normal absorption spectra.

Linear dichroism of the complex between the gene 32 protein of bacteriophage T4 and poly(1,N6-ethenoadenylic acid)

We performed linear dichroism measurements in compressed polyacrylamide gels on the complex between the helix-destabilizing protein of bacteriophage T4, GP32 and poly(1,N6-ethenoadenylic acid), which is used as a model system for single-stranded DNA. A strong hyperchromism for poly(1,N6-ethenoadenylic acid) in the complex indicates a strongly altered conformation. The positive linear dichroism in the wavelength region where the bases absorb must be explained by a strong tilting of the bases in the complex. This finding is in accordance with results from earlier studies, using electric birefringence and circular dichroism measurements. Our measurements show that the angle between the bases and the local helix axis is 42(+/- 6)degrees. In addition, a pronounced contribution from the tryptophan residues of GP32 can be recognized, indicating that several of these residues have a specific orientation in the complex. The sign of the dichroism due to the tryptophan residues is the same as that due to the DNA bases. However, it is not sufficient to assume that all the observed dichroism is due to one or more intercalated tryptophan residues and there must be one or more additional tryptophan residues that make an angle of less than 40 degrees with the local helix axis. Some possible structures of the DNA-protein complex are discussed.