Internal motions in B- and Z-form poly(dG-dC).poly(dG-dC): 1H NMR relaxation studies

Proton NMR relaxation measurements are used to compare the molecular dynamics of 60 base pair duplexes of B- and Z-form poly(dG-dC).poly(dG-dC). The relaxation rates of the exchangeable guanine imino protons (Gim) in H2O and in 90% D2O show that below 20 degrees C spin-lattice relaxation is exclusively from proton-proton magnetic dipolar interactions while proton-nitrogen interactions contribute about 30% to the spin-spin relaxation. The observation that the spin-lattice relaxation is nonexponential and that the initial spin-lattice relaxation rate of the Gim, G-H8 and C-H6 protons depends on the selectivity of the exciting pulse shows that spin-diffusion dominates the spin-lattice relaxation. The relaxation rates of the Gim, C-H5, and C-H6 in B- and Z-form poly(dG-dC).poly(dG-dC) cannot be explained by assuming the DNA behaves as a rigid rod. The data can be fit by assuming large-amplitude out of plane motions (+/- 30-40 degrees, tau = 1-100 ns) and fast, large-amplitude local torsional motions (+/- 25-90 degrees, tau = 0.1-1.5 ns) in addition to collective torsional motions. The results for the B and Z forms show that the rapid internal motions are similar and large in both conformations although backbone motions are slightly slower, or of lower amplitude, in Z DNA. At high temperatures (greater than 60 degrees C), imino proton exchange with solvent dominates the spin-lattice relaxation of B-form poly(dG-dC).poly(dG-dC), but in the Z form no exchange contribution (less than 2 s-1) is observed at temperatures as high as 85 degrees C. Conformational fluctuations that expose the imino protons to the solvent are strikingly different in the B and Z forms. The results obtained here are compared with those previously reported for poly(dA-dT).poly(dA-dT).     

DNA in phosphorus atom representation: the heteronomous double helices of poly(dA).poly(dT) and poly(dG).poly(dC) and simulation of the yeast genome and of a human chromosome DNA

We extracted phosphorus atom coordinates from the database of DNA crystal structures and calculated geometrical parameters needed to reproduce the crystal structures in the phosphorus atom representation. Using the geometrical parameters we wrote a piece of software assigning the phosphorus atom coordinates to the DNA of any nucleotide sequence. The software demonstrates non-negligible influence of the primary structure on DNA helicity, which may stand behind the heteromonous double helices of poly(dA).poly(dT) and poly(dG).poly(dC). In addition, the software is so simple that it makes possible to simulate the "crystal" structures of not only viral DNAs, but also the whole genome of Saccharomyces cerevisiae as well as the DNA human chromosome 22 having dozens of megabases in length.     

Lattice vibrational modes of poly(rU) and poly(rA)

A normal coordinate analysis has been performed for the polyribonucleotides poly(rU) and poly(rA). The polymers are assumed to be 11-fold infinite helical structures in the A conformation. The hydrogen atoms have been rigidly attached to the appropriate atoms in order to reduce the dimension of the problem. The potential energy is defined in terms of a valence force field initially and a model for the inclusion of nonbonded interactions has been presented. A method for factoring the secular equation for infinite helical polymers in Cartesian coordinates is presented. All of the general features of polyribonucleotide spectra have been reproduced and, in many cases, good quantitative agreement between observed and calculated frequencies is obtained. More specific assignments are offered for some of the observed lines.     

Vibrational analysis of peptides, polypeptides, and proteins. XXXII. alpha-Poly(L-glutamic acid)

The Raman and ir spectra of α-helical poly(L -glutamic acid) have been assigned on the basis of a normal mode calculation for this structure. The force field was based on our previously refined main-chain force constants for α-poly(L -alanine) and side-chain force constants for β-calcium–poly(L -glutamate). Despite the identical backbone α-helical structures, significantly different frequencies are calculated, and observed, in the amide III and backbone stretch regions of α-poly(L -glutamic acid), as compared with α-poly(L -alanine). This clearly demonstrates the influence of side-chain structure on mainchain vibrational modes.     

Poly(dA).poly(dT) exists in an unusual conformation under physiological conditions: propidium binding to poly(dA).poly(dT) and poly[d(A-T)].poly[d(A-T)]

The binding of propidium to poly(dA).poly(dT) [poly(dA.dT)] and to poly[d(A-T)].poly[d(A-T)] [poly[d(A-T)2]] has been compared under a variety of solution conditions by viscometric titrations, binding studies, and kinetic experiments. The binding of propidium to poly[d(A-T)2] is quite similar to its binding to calf thymus deoxyribonucleic acid (DNA). The interaction with poly(dA.dT), however, is quite unusual. The viscosity of a poly(dA.dT) solution first decreases and then increases in a titration with propidium at 18 degrees C. The viscosity of poly[d(A-T)2] shows no decrease in a similar titration. Scatchard plots for the interaction of propidium with poly(dA.dT) show the classical upward curvature for positive cooperativity. The curvature decreases as the temperature is increased in binding experiments. A van't Hoff plot of the observed binding constants yields an apparent positive enthalpy of approximately +6 kcal/mol for the propidium-poly(dA.dT) interaction. Propidium binding to poly[d(A-T)2] shows no evidence for positive cooperativity, and the enthalpy change for the reaction is approximately -9 kcal/mol. Both the magnitude of the dissociation constants and the effects of ionic strength are quite similar for the dissociation of propidium from poly(dA-T)2] and from poly[d(A-T)2], suggesting that the intercalated states are similar for the two complexes. The observed association reactions, under pseudo-first-order conditions, are quite different. Plots of the observed pseudo-first-order association rate constant vs. polymer concentration have much larger slopes for propidium binding to poly[d(A-T)2] than to poly(dA.dT).(ABSTRACT TRUNCATED AT 250 WORDS)     

Vibrational analysis of peptides,polypeptides, and proteins. II. β-Poly(L-alanine) and β-poly(L-alanylglycine)

The normal vibration frequencies of poly(L -alanine) and poly(L -alanylglycine) in the antiparallel chain-pleated sheet structure have been calculated, using the force field for polyglycine I from the previous paper (Biopolymers 15 , 2439–2464) plus additional force constants for the methyl group. The agreement with observed ir and Raman bands is very good. This substantiates the excellent transferability of the force field, since polyglycine I was shown to have a rippled-sheet structure. The amide I and amide II mode splittings are very well accounted for by transition dipole coupling, showing that subtle structural differences are sensitively manifested through this mechanism.     

Development of an AMBER-compatible transferable force field for poly(ethylene glycol) ethers (glymes)

An all-atom force field consistent with the general AMBER force field (GAFF) format for poly(ethylene glycol) dimethyl ether (diglyme or G2) was developed by fitting to experimental liquid densities and dielectric constants. Not surprisingly, the new force field gives excellent agreement with experimental liquid phase densities and dielectric constants over a wide temperature range. Other dynamic and thermodynamic properties of liquid G2 such as its self-diffusion coefficient, shear viscosity, and vaporization enthalpy were also calculated and compared to experimental data. For all of the properties studied, the performance of the proposed new force field is better than that of the standard GAFF force field. The force field parameters were transferred to model two other poly(ethylene glycol) ethers: monoglyme (G1) and tetraglyme (G4). The predictive ability of the modified force field for G1 and G4 was significantly better than that of the original GAFF force field. The proposed force field provides an alternative option for the simulation of mixtures containing glymes using GAFF-compatible force fields, particularly for electrochemical applications. The accuracy of a previously published force field based on the OPLS-AA format and the accuracies of two modified versions of that force field were also examined for G1, G2, and G4. It was found that the original OPLS-AA force field is superior to the modified versions of it, and that it has a similar accuracy to the proposed new GAFF-compatible force field.

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Graphical abstract Transferability of an AMBER-compatible force field parameterized for G2 to other glymes

     

Monoclonal antibodies specific for poly(dG) X poly(dC) and poly(dG) X poly(dm5C)

Most duplex DNAs that are in the "B" conformation are not immunogenic. One important exception is poly(dG) X poly(dC), which produces a good immune response even though, by many criteria, it adopts a conventional right-handed helix. In order to investigate what features are being recognized, monoclonal antibodies were prepared against poly(dG) X poly(dC) and the related polymer poly(dG) X poly(dm5C). Jel 72, which is an immunoglobulin G, binds only to poly(dG) X poly(dC), while Jel 68, which is an immunoglobulin M, binds approximately 10-fold more strongly to poly(dG) X poly(dm5C) than to poly(dG) X poly(dC). For both antibodies, no significant interaction could be detected with any other synthetic DNA duplexes including poly[d(Gm5C)] X poly[d(Gm5C)] in both the "B" and "Z" forms, poly[d(Tm5Cm5C)] X poly[d(GGA)], and poly[d(TCC)] X poly[d(GGA)], poly(dI) X poly(dC), or poly(dI) X poly(dm5C). The binding to poly(dG) X poly(dC) was inhibited by ethidium and by disruption of the DNA duplex, confirming that the antibodies were not recognizing single-stranded or multistranded structures. Furthermore, Jel 68 binds significantly to phage XP-12 DNA, which contains only m5C residues and will precipitate this DNA in the absence of a second antibody. The results suggest that (dG)n X (dm5C)n sequences in natural DNA exist in recognizably distinct conformations.     

Effect of partial atomic charges on the calculated free energy of solvation of poly(vinyl alcohol) in selected solvents

It is well-known that properties of poly(vinyl alcohol) (PVA) in the pure and solution states depend largely on the hydrogen bonding networks formed. In the context of molecular simulation, such networks are handled through the Coulombic interactions. Therefore, a good set of partial atom charges (PACs) for simulations involving PVA is highly desirable. In this work, we calculated the PACs for PVA using a few commonly used population analysis schemes with a hope to identify an accurate set of PACs for PVA monomers. To evaluate the quality of the calculated parameters, we have benchmarked their predictions for free energy of solvation (FES) in selected solvents by molecular dynamics simulations against the ab initio calculated values. Selected solvents were water, ethanol and benzene as they covered a range of size and polarity. Also, PVA with different tacticities were used to capture their effect on the calculated FESs. Based on our results, neither PACs nor FESs are affected by the chain tacticity. While PACs predicted by the Merz-Singh-Kollman scheme were close to original values in the OPLS-AA force field in way that no significant difference in properties of pure PVA was observed, free energy of solvation calculated using such PACs showed greater agreement with ab initio calculated values than those calculated by OPLS-AA (and all other schemes used in this work) in all three solvents considered.     

Interactions of poly(amino acids) in aqueous solution with charged model surfaces--analysis by colloidal probe

Biomolecules in a confined solution environment may be subject to electrostatic forces with a range up to 100 nm, while van der Waals interaction will account for shorter-range forces. The response of two model poly(amino acids)--poly-L-lysine and poly-L-glutamic acid--has been investigated for a silica/Si-oxide surface at pH 6. The model amino acids were adsorbed, or covalently coupled, to colloidal probes consisting of a microsphere attached to a force-sensing lever. The methodology was based on sensing interaction between the probe and a flat surface through carrying out force versus distance analysis with a scanning force microscope. The results were analyzed within the framework of the conventional DLVO theory. The outcomes illustrate both repulsive and attractive long-range interactions that will hinder, or promote, colloidal biospecies in solution entering the region of attractive short-range interactions at the physical interface. Large 'snap-on' distances were observed for some systems and have been ascribed to compression of the 'soft' functionalized layers. Those observations and measurements of adhesion provided insight into conformation of the adsorbed species and strength of attachment. The results have implications for the efficacy of methods and devices that seek to exploit the properties of micro/nano-fluidic systems.     

Thermodynamics of interactions of TAlPyP4 and AgTAlPyP4 porphyrins with poly(rA)poly(rU) and poly(rI)poly(rC) duplexes

We employed UV light absorption and circular dichroism (CD) spectroscopic measurements to study the binding of novel water-soluble porphyrins meso-tetra-(4N-allylpyridyl)porphyrin [TAlPyP4], and its Ag containing derivative to the poly(rA)poly(rU) and poly(rI)poly(rC) RNA duplexes. Our results suggest that TAlPyP4 associate with the duplexes via intercalation, whereas the conservative CD spectra indicates that AgTAlPyP4 preferably binds via outside self-stacking mode. We used our determined binding isotherms for each ligand-RNA binding event to calculate the binding constant, Kb, and binding free energy, DeltaGb = -RTlnKb. By performing these experiments as a function of temperature, we evaluated the van't Hoff binding enthalpies, DeltaH. The binding entropies, DeltaSb, were calculated as DeltaSb = (DeltaHb - DeltaGb)/T. We interpret our data in terms of specific interactions that stabilize/destabilize each ligand-RNA complex studied in this work. Taken together, our data provide important new information about the thermodynamics of interactions of porphyrins with nucleic acids.     

Stopped-flow kinetic analysis of the interaction of anthraquinone anticancer drugs with calf thymus DNA, poly[d(G-C)].poly[d(G-C)], and poly[d(A-T)].poly[d(A-T)]

The sodium dodecyl sulfate driven dissociation reactions of daunorubicin (1), mitoxantrone (2), ametantrone (3), and a related anthraquinone without hydroxyl groups on the ring or side chain (4) from calf thymus DNA, poly[d(G-C)]2, and poly[d(A-T)]2 have been investigated by stopped-flow kinetic methods. All four compounds exhibit biphasic dissociation reactions from their DNA complexes. Daunorubicin and mitoxantrone have similar dissociation rate constants that are lower than those for ametantrone and 4. The effect of temperature and ionic strength on both rate constants for each compound is similar. An analysis of the effects of salt on the two rate constants for daunorubicin and mitoxantrone suggests that both of these compounds bind to DNA through a mechanism that involves formation of an initial outside complex followed by intercalation. The daunorubicin dissociation results from both poly[d(G-C)]2 and poly[d(A-T)]2 can be fitted with a single exponential function, and the rate constants are quite close. The ametantrone and 4 polymer dissociation results can also be fitted with single exponential curves, but with these compounds the dissociation rate constants for the poly[d(G-C)]2 complexes are approximately 10 times lower than for the poly[d(A-T)]2 complexes. Mitoxantrone also has a much slower dissociation rate from poly[d(G-C)]2 than from poly[d(A-T)]2, but its dissociation from both polymers exhibits biphasic kinetics. Possible reasons for the biphasic behavior with the polymers, which is unique to mitoxantrone, are selective binding and dissociation from the alternating polymer intercalation sites and/or dual binding modes of the intercalator with both side chains in the same groove or with one side chain in each groove.     

Unique poly(dA).poly(dT) B'-conformation in cellular and synthetic DNAs

Poly(dA).poly(dT), but not B-form DNA, is specifically recognized by experimentally induced anti-kinetoplast or anti-poly(dA).poly(dT) immunoglobulins. Antibody binding is completely competed by poly(dA).poly(dT) and poly(dA).poly(dU) but not by other single- or double-stranded DNA sequences in a right-handed B-form. Antibody interaction with poly(dA).poly(dT) depends on immunoglobulin concentration, incubation time and temperature, and is sensitive to elevated ionic strengths. Similar conformations, for example, (dA)4-6 X (dT)4-6, in the kinetoplast DNA of the parasite Leishmania tarentolae are also immunogenic and induce specific anti-poly(dA).poly(dT) antibodies. These antibody probes specifically recognize nuclear and kinetoplast DNA in fixed flagellated kinetoplastid cells as evidenced by immunofluorescence microscopy. Anti-poly(dA).poly(dT) immunofluorescence is DNase-sensitive and competed by poly(dA).poly(dT), but not other classical double-stranded B-DNAs. Thus, these unique cellular B'-DNA helices are immunogenic and structurally similar to synthetic poly(dA).poly(dT) helices in solution.     

High pressure fourier transform infrared spectroscopy of poly(dA)poly(dT), poly(dA) and poly(dT)

The effect of hydrostatic pressure upon the DNA duplex, poly(dA)poly(dT), and its component single strands, poly(dA) and poly(dT) has been studied by fourier-transform infrared spectroscopy (FT-IR). The spectral data indicate that at 28 degrees C and pressures up to 12 kbar (1200 MPa) all three polymers retain the B conformation. Pressure causes the band at 967 cm(-1), arising from water-deoxyribose interactions, to shift to higher frequencies, a result consistent with increased hydration at elevated pressures. A larger pressure-induced frequency shift in this band is observed in the single stranded polymers than in the double stranded molecule, suggesting that the effect of pressure on the hydration of single strands may be greater than upon a double stranded complex. A pressure-dependent hypochromicity in the bands attributed to base stacking indicates that pressure facilitates the base stacking in the three polymers, in agreement with previous assessments of the importance of stacking in the stabilization of DNA secondary structure at ambient and high pressures.     

Reconstitution and poly(ADP-ribosyl)ation of proteolytically fragmented poly(ADP-ribose) synthetase

Calf thymus poly(ADP-ribose) synthetase (Mr = 120,000) is cleaved with papain into two fragments of M(r) = 74,000 and 46,000 and also split with chymotrypsin into two fragments of M(r) = 66,000 and 54,000. Each fragment purified to homogeneity is enzymatically inactive, but combined incubation of the 74,000 and 46,000 fragments in the presence of DNA restored 20% of the enzyme activity. In contrast, combined incubation of the 66,000 and 54,000 fragments does not restore any enzyme activity. In the former incubation, autopoly(ADP-ribosyl)ation reaction occurs exclusively on the 74,000 fragment. When each fragment is incubated with [adenine-U-14C]NAD in the presence of DNA and a catalytic amount of the native enzyme, poly(ADP-ribosyl)action occurs in the overlapped portion (22,000) of the 66,000 fragment and the 74,000 fragment. Nevertheless, the purified 22,000 fragment is a poor acceptor for poly(ADP-ribosyl)ation. The degree of poly(ADP-ribosyl)ation of the proteolytic fragments is significantly reduced by increasing NaCl concentration, probably due to the lack of the interaction between the enzyme fragments and DNA. These results, taken together, indicate that DNA is indispensable for the reconstitution of the catalytic activity as well as the poly(ADP-ribosyl)ation of the fragmented enzyme.     

Central role for the Werner syndrome protein/poly(ADP-ribose) polymerase 1 complex in the poly(ADP-ribosyl)ation pathway after DNA damage

A defect in the Werner syndrome protein (WRN) leads to the premature aging disease Werner syndrome (WS). Hallmark features of cells derived from WS patients include genomic instability and hypersensitivity to certain DNA-damaging agents. WRN contains a highly conserved region, the RecQ conserved domain, that plays a central role in protein interactions. We searched for proteins that bound to this region, and the most prominent direct interaction was with poly(ADP-ribose) polymerase 1 (PARP-1), a nuclear enzyme that protects the genome by responding to DNA damage and facilitating DNA repair. In pursuit of a functional interaction between WRN and PARP-1, we found that WS cells are deficient in the poly(ADP-ribosyl)ation pathway after they are treated with the DNA-damaging agents H2O2 and methyl methanesulfonate. After cellular stress, PARP-1 itself becomes activated, but the poly(ADP-ribosyl)ation of other cellular proteins is severely impaired in WS cells. Overexpression of the PARP-1 binding domain of WRN strongly inhibits the poly(ADP-ribosyl)ation activity in H2O2-treated control cell lines. These results indicate that the WRN/PARP-1 complex plays a key role in the cellular response to oxidative stress and alkylating agents, suggesting a role for these proteins in the base excision DNA repair pathway.     

Studies of interaction between poly(allylamine hydrochloride) and double helix DNA by spectral methods

DNA interaction with cationic polyelectrolytes promises to be a versatile and effective synthetic transfection agent. This paper presents the study on interaction between a simple artificial cationic polymer, poly(allylamine hydrochloride) (PAA), and herring sperm DNA (hsDNA) using several spectroscopic methods, including light scattering, microscopic FTIR-, CD-spectroscopy and so on. The results show that PAA interacts with DNA through both the phosphate groups and the nitrogenous bases of DNA. The formation of DNA/PAA complex may change the micro-environment of double helix of DNA from B- to C-form and the great changes in DNA morphology occur when N:P ratio is near to 1.0. At the same time, the spectroscopic changes of ethidium bromide (EB) on its binding to DNA are utilized to study the interaction between PAA and DNA. Reversion of the maximum absorption wavelength (numax), reduction of induced circular dichroism and decrease in fluorescence intensity of DNA-EB on addition of PAA indicate that the formation of the complex between DNA and PAA is not in favor of the interaction between DNA and EB. The binding constant of EB and the number of binding sites per nucleotide decrease with increase in the concentrations of PAA, indicating noncompetitive inhibition of EB binding to DNA in the presence of PAA. It is also proved that the formation of the DNA/PAA complex is influenced by pH value and ionic strength.