Molecular electrotatic potential of a triple stranded helix: Poly(dT)·poly(dA)·poly(dT)

The molecular electrostatic potential of the triple helix poly(dT)·tpoly(dA)·poly(dT) is calculated, and the results are examined in relation to those obtained for its component double and single helical parts. For the double helix presenting the standard Watson–Crick hydrogen bonds, the deepest potentials are formed on the side of the major groove, a situation similar to that observed in the A-DNA duplex. For the double helix presenting Hoogsteen-type hydrogen bonds the deepest potentials lie in the major groove, on the side of the pyrimidine strand. In the triple helix the deepest potentials are located in the major groove in a narrow zone over the thymine bases of the Watson–Crick pair.     

Simultaneous binding of meso-tetrakis(N-methylpyridinium-4-yl)porphyrin and 4',6-diamidino-2-phenylindole at the minor grooves of poly(dA).poly(dT) and poly[d(A-T)(2)]: fluorescence resonance energy transfer between DNA bound drugs

The spectral properties of meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (TMPyP) bound to poly(dA).poly(dT) and poly[d(A-T)(2)] in the presence and in the absence of 4',6-diamidino-2-phenylindole (DAPI) have been studied. DAPI fits deeply into the minor groove of both poly(dA).poly(dT) and poly[d(A-T)(2)], and TMPyP is also situated at the minor groove. The nature of the absorption, circular dichroism (CD), and flow linear dichroism (LD) spectra of the TMPyP-poly(dA).poly(dT) and -poly[d(A-T)(2)] complexes in the Soret band is essentially unaffected whether the minor groove is blocked by DAPI or not, although small variations been noticed in the presence of DAPI. Furthermore, a close analysis of the reduced LD spectrum in the Soret band results in angles of approximately 80 degrees and 55 degrees between transition moments of the TMPyP and DNA helix axes in the absence of DAPI. All these observations indicate that the side of TMPyP whose structure resembles that of classical minor groove binding drugs does not fit deeply into the minor groove. This suggests that TMPyP binds across the minor groove: two positively charged pyridiniumyl rings interact electrostatically with negatively charged phosphate groups of DNA. When DAPI and TMPyP are simultaneously bound to poly(dA).poly(dT) or poly[d(A-T)(2)], the fluorescence intensity of DAPI decreases as TMPyP concentration increases, indicating that the excited energy of DAPI is transferred to TMPyP.     

Theoretical study of the interaction of tetramethylammonium with double-stranded oligonucleotides

Computations are performed on the interaction specificities of tetramethylammonium (TMA) for double-stranded oligonucleotides held in the B conformation. The effects of base sequence and chain length are investigated. In the short oligomers (helices formed from dinucleoside monophosphates and trinucleoside diphosphates), the interaction energies of TMA are larger in the major groove of (dG)_n · (dC)_n than in the minor groove of either (dA)_n · (dT)_n or (dA—dT)_n. Upon lengthening the oligomers, and owing to the gradual shaping of the grooves of the helix and cumulative effect of the phosphates, TMA is shown to increasingly favor the minor groove of (dA)_n · (dT)_n with respect to the major groove of (dG)_n · (dC)_n, with a sizeable energy difference computed at the pentanucleoside hexaphosphate level. The binding of TMA in the minor groove of (dA)_n · (dT)_n involves stabilizing contacts with several sites, on the bases and on the deoxyriboses. Configurations locating the cation closer to the thymine strand are slightly preferred over configurations locating it closer to the adenine strand.     

Denaturation of Drew-Dickerson DNA in a high salt concentration medium: molecular dynamics simulations

We have performed molecular dynamics simulation on B-DNA duplex (CGCGAATTGCGC) at different temperatures. The DNA was immerged in a salt-water medium with 1 M NaCl concentration to investigate salt effect on the denaturation process. At each temperature, configurational entropy is estimated using the covariance matrix of atom-positional fluctuations, from which the melting temperature (T(m)) was found to be 349 K. The calculated configuration entropy for different bases shows that the melting process involves more peeling (including fraying from the ends) conformations, and therefore the untwisting of the duplex and peeling states form the transition state of the denaturation process. There is a narrow minor groove in the AATT sequence that becomes wider by increasing temperature which disappears at high temperatures, especially above the melting temperature. We have also calculated the fraction of denatured base pairs, f-curve, from which T(m) was found to be 340 K, close to experimental value of 341 K. We found that DNA at high salt concentrations has few hydrogen bonds even at temperatures higher than the T(m). Our calculations show the fact that adding salt leads to increase of T(m) and stabilization of DNA.     

Two-dimensional sheet based on C–H···N hydrogen bonds within an organic cocrystal: a crystallographic,spectroscopic and theoretical study

The cocrystal containing 1,2,4,5-tetracyanobenzene (TCNB) and trans-1,2-bis(4-pyridyl)ethylene (4,4′-BPE) has been realised (TCNB)·(4,4′-BPE) 1. Compound 1 produces a two-dimensional sheet based on two different types of C–H···N hydrogen bonds. Each molecule within the cocrystal functions as both a donor and an acceptor of hydrogen bonds. Weak hydrogen bonds such as these, acting as the driving force to produce a polymeric assembly, are not investigated as frequently as stronger and more traditional O–H···O and O–H···N hydrogen bonds within multicomponent cocrystals. The existence of the different types of C–H···N hydrogen bonds was confirmed by single-crystal X-ray diffraction as well as infrared spectroscopy. The overall interaction energies for both types of hydrogen bonds were determined by computational calculations at various levels of theory.     

Site‐Directed Spin‐Labeling of DNA by the Azide–Alkyne ‘Click’ Reaction: Nanometer Distance Measurements on 7‐Deaza‐2′‐deoxyadenosine and 2′‐Deoxyuridine Nitroxide Conjugates Spatially Separated or Linked to a ‘dA‐dT’ Base Pair

Nucleobase‐directed spin‐labeling by the azide‐alkyne ‘click’ (CuAAC) reaction has been performed for the first time with oligonucleotides. 7‐Deaza‐7‐ethynyl‐2′‐deoxyadenosine ( 1 ) and 5‐ethynyl‐2′‐deoxyuridine ( 2 ) were chosen to incorporate terminal triple bonds into DNA. Oligonucleotides containing 1 or 2 were synthesized on a solid phase and spin labeling with 4‐azido‐2,2,6,6‐tetramethylpiperidine 1‐oxyl (4‐azido‐TEMPO, 3 ) was performed by post‐modification in solution. Two spin labels ( 3 ) were incorporated with high efficiency into the DNA duplex at spatially separated positions or into a ‘dA‐dT’ base pair. Modification at the 5‐position of the pyrimidine base or at the 7‐position of the 7‐deazapurine residue gave steric freedom to the spin label in the major groove of duplex DNA. By applying cw and pulse EPR spectroscopy, very accurate distances between spin labels, within the range of 1–2 nm, were measured. The spin–spin distance was 1.8±0.2 nm for DNA duplex 17 ( dA*^7,10 ) ?11 containing two spin labels that are separated by two nucleotides within one individual strand. A distance of 1.4±0.2 nm was found for the spin‐labeled ‘dA‐dT’ base pair 15 ( dA*⁷ ) ?16 ( dT*⁶ ). The ‘click’ approach has the potential to be applied to all four constituents of DNA, which indicates the universal applicability of the method. New insights into the structural changes of canonical or modified DNA are expected to provide additional information on novel DNA structures, protein interaction, DNA architecture, and synthetic biology.     

Hydrogen-bonded supramolecular motifs in crystal structures of trimethoprim barbiturate monohydrate (I) and 2-amino-4,6-dimethylpyrimidinium barbiturate trihydrate (II)

In the present study, we report the crystal structures of two organic salts, namely 2,4-diamino-5-(3′,4′,5′-trimethoxybenzyl)pyrimidinium (TMP) barbiturate monohydrate (TMPBAR) (I), 2-amino-4,6-dimethylpyrimidinium (AMPY) barbiturate trihydrate (AMPYBAR) (II). In both complexes, one ring nitrogen of TMP and AMPY are protonated as a result of proton transfer from the−CH₂ group of barbituric acid. In compound (I), the TMP cation and barbiturate anion are paired through twoN−H···O and one N−H···N hydrogen bonds. This pair further self-organizes through N−H···O hydrogen bonds to generate an array of six hydrogen bonds. These arrays are further cross-linked by N−H···O hydrogen bonds forming a sheet-like structure. The water molecule is also embedded in the sheet via O−H···O and C−H···O hydrogen bonds, forming a rosette-like supramolecular motif. TMP cations are also bridged by alternating water molecules via C−H···O and O−H···N hydrogen bonds. In compound (II), the symmetrical barbiturate anions self-organize on both sides through N−H···O hydrogen bonds generating a supramolecular chain. These chains are cross-linked by the three water molecules. A pair of barbiturate anions and two water molecules constitute an array of four hydrogen bonds (DADA quadruple array). These arrays are cross-linked by another water molecule. 2-Amino-4,6-dimethylpyrimidine cations are paired through N−H···N hydrogen bonds. These pairs are bridged by three water molecules generating a supramolecular ribbon. The barbiturate chains and base pairs are arranged in an alternate manner via N−H···O and O−H···O hydrogen bonds to generate a 3-D network.     

Thermodynamic profiles of the DNA binding of benzophenanthridines sanguinarine and ethidium: A comparative study with sequence specific polynucleotides

Energetics of the binding of two known classical DNA intercalating molecules, ethidium and sanguinarine with four sequence specific polynucleotides, poly(dG-dC).poly(dG-dC), poly(dG).poly(dC), poly(dA-dT).poly(dA-dT), and poly(dA).poly(dT) have been compared under identical conditions. The binding of both the molecules was characterized by strong stabilization of the polynucleotides against thermal strand separation in optical melting as well as differential scanning calorimetry studies. Isothermal titration calorimetry results revealed that the binding of both sanguinarine and ethidium to poly(dG-dC).poly(dG-dC), poly(dA-dT).poly(dA-dT), and poly(dG).poly(dC) was exothermic and favoured by negative enthalpy changes. On the other hand, the binding of both molecules to poly(dA).poly(dT) was endothermic and entropy driven. The binding affinity values obtained from isothermal titration calorimetry data was in close proximity to that derived from thermal melting data. The heat capacity changes obtained from temperature dependence of the enthalpy change gave negative values in the range (?0.4 to 1.25) kJ · mol^?1 · K^?1 for the binding of ethidium and sanguinarine to these polynucleotides. The variations in the values indicate important differences in the formation of the complexes. New insights into the energetics and specificity aspects of interaction of these molecules to DNA have emerged from these studies.     

Aminoglycoside-nucleic acid interactions: remarkable stabilization of DNA and RNA triple helices by neomycin

The stabilization of poly(dA).2poly(dT) triplex, a 22-base DNA triplex, and poly(rA).2poly(rU) triple helix by neomycin is reported. The melting temperatures, the association and dissociation kinetic parameters, and activation energies (E(on) and E(off)) for the poly(dA).2poly(dT) triplex in the presence of aminoglycosides and other triplex binding ligands were determined by UV thermal analysis. Our results indicate that: (i) neomycin stabilizes DNA triple helices, and the double helical structures composed of poly(dA).poly(dT) are virtually unaffected. (ii) Neomycin is the most active and triplex-selective stabilization agent among all aminoglycosides, previously studied minor groove binders, and polycations. Its selectivity (DeltaT(m3-->2) vs DeltaT(m2)(-->)(1)) exceeds most intercalating drugs that bind to triple helices. (iii) Neomycin selectively stabilizes DeltaT(m3)(-->)(2) for a mixed 22-base DNA triplex containing C and T bases in the pyrimidine strand. (iv) The rate constants of formation of triplex (k(on)) are significantly enhanced upon increasing molar ratios of neomycin, making triplex association rates closer to duplex association rates. (v) E(on) values become more negative upon increasing concentration of aminoglycosides (paromomycin and neomycin). E(off) values do not show any change for most aminoglycosides except neomycin. (vi) Aminoglycosides can effectively stabilize RNA [poly(rA).2poly(rU)] triplex, with neomycin[being one of the most active ligands discovered to date (second only to ellipticine). (vii) The stabilization effect of aminoglycosides on triple helices is parallel to their toxic behavior, suggesting a possible role of intramolecular triple helix (H-DNA) stabilization by the aminoglycosides.     

Calorimetric and thermal analysis studies on the binding of phenothiazinium dye thionine with DNA polynucleotides

Binding of the phenothaizinium dye thionine with four sequence specific deoxyribopolynucleotides, poly(dG-dC).poly(dG-dC), poly(dG).poly(dC), poly(dA-dT).poly(dA-dT), and poly(dA).poly(dT) has been investigated by means of thermal helix melting, isothermal titration calorimetry, and differential scanning calorimetry experiments. The binding affinity values evaluated from isothermal titration calorimetry suggests that thionine exhibits the highest binding affinity to poly(dG-dC).poly(dG-dC). The binding to poly(dG-dC).poly(dG-dC), poly(dA-dT).poly(dA-dT), and poly(dG).poly(dC) is exothermic and favoured by negative enthalpy changes while binding to poly(dA).poly(dT) is endothermic and anomalous. The values of heat capacity changes of the interaction are negative and in the range (?0.4 to ?0.5) kJ · K^?1 · mol^?1. The binding is characterized by strong stabilization of the polynucleotides against thermal strand separation. The binding affinity values derived from thermal melting data are in excellent agreement with those obtained from isothermal titration calorimetry data. Insights into the energetic aspects and guanine–cytosine selectivity of the DNA interaction of thionine have been obtained from these studies.     

Rapid Location of the Preferred Interaction Sites between Small Polar Molecules and Macromolecules. II. Binding of Water to a Model Segment of B-DNA

The procedure developed in Part I of this series is applied to the homopolymeric sequences poly(dA) · poly(dT) and poly(dG) · poly(dC) on the double helical structure of B-DNA. Some aspects of the base sequence influence on the polymer's attraction for water molecule are described. The results are used to discuss the general hydration features of those systems in relation to recent experimental studies of DNA single crystals.     

The effect of methyl group on the cooperativity between three types of hydrogen bond: O?H···O,C?H···O,and O?H···π

The effect of the methyl group on the cooperativity between three types of hydrogen bond (O H···O, C H···O, and O H···π) in cyclic complex involving an acetylene and two waters has been studied on the basis of high-level ab initio calculations. The total interaction energy of three hydrogen bonds increases as the number of methyl group in the complex increases. The binding distances of O H···π and O H···O hydrogen bonds shorten, while that of C H···O hydrogen bond elongates with increasing methyl group. This indicates that addition of methyl group leads to enhancement of O H···π and O H···O hydrogen bonds, and weakening of C H···O hydrogen bond, as also shown in frequency shift, chemical shifts, charge populations, and stabilization energies of orbital interactions. Although the presence of methyl group has a complicated effect on different type of hydrogen bond, the cooperativity of three hydrogen bonds increases in general with the addition of methyl group. © 2007 Wiley Periodicals, Inc. Int J Quantum Chem, 2008     

Conformational studies of double-helical polynucleotides by the method of pair-wise potential functions

Double-helical polynucleotide conformations, poly(dA)·poly(dT), poly(d(A-T))·poly(d(T-A))·poly(dG)·poly(dC), and poly(d(G-C))·poly(d(C-G)) are analyzed by the atom–atom potential method. The energy optimization is carried out in the space of eight independent geometric parameters using analytical procedures for the constraints, taking into account the flexibility of the β-D -deoxyribose rings. At the first stage, the full screening of atomic partial charges was assumed. The structures of the calculated B and the A forms of DNA are characterized by low energy and absence of short contacts; the dihedral angles are near the average values in the monomers. With the typical energy difference of 3–5 kcal/mol nucleotide pairs in all cases, the B form is more preferable as compared to the A form. At the final step the effect of the Coulomb term is evaluated for poly(dA)·poly(dT) using various values of the effective dielectric constant (? = 28, 24, 20, 18, 14, 12, 10, 8, 6, 4, and 1). If ? ?24, the energy optimization leads A to B. We discuss the stereochemical details of the intermediate conformations on the A–B path and hypothesize the nature of stability of the A and the B forms and the mechanism of the A–B transition.     

Unsymmetrical 1-naphthyltellurium(IV) dihalides: the interplay of Te···Br,C–H···Br and C–H···π interactions in the crystal structure of (1-naphthyl)(4-methylphenyl)tellurium(IV) dibromide

The crystal structure of (1-naphthyl)(4-methyl- phenyl)tellurium(IV) dibromide, the first unsymmetrical naphthyl containing diorganotellurium(IV) dibromide, shows the formation of one-dimensional supramolecular arrays where Te···Br secondary bonds link two parallel rows of molecules in a gear-teethed fashion. The weaker C–H···Br and C–H···π hydrogen bonds play important role in the formation of three-dimensional crystal lattice by cross linking these supramolecular motifs.     

All‐atom Molecular Dynamic Simulations Combined with the Chemical Shifts Study on the Weak Interactions of Ethanol‐water System

All‐atom molecular dynamics (MD) simulation combined with chemical shifts was performed to investigate the interactions over the entire concentration range of the ethanol (EtOH)‐water system. The results of the simulation were adopted to explain the NMR experiments by hydrogen bonding analysis. The strong hydrogen bonds and weak C–H···O contacts coexist in the mixtures through the analysis of the radial distribution functions. And the liquid structures in the whole concentration of EtOH‐water mixtures can be classified into three regions by the statistic analysis of the hydrogen‐bonding network in the MD simulations. Moreover, the chemical shifts of the hydrogen atom are in agreement with the statistical results of the average number hydrogen bonds in the MD simulations. Interestingly, the excess relative extent of η_rel^E calculated by the MD simulations and chemical shifts in the EtOH aqueous solutions shows the largest deviation at x_EtOH≈0.18. The excess properties present good agreement with the excess enthalpy in the concentration dependence.     

Polyplexes of poly(methylaminophosphazene): energetics of DNA melting

The interaction of DNA with a synthetic biocompatible and biodegradable cationic polymer, poly(methylaminophosphazene) hydrochloride (PMAP·HCl), was investigated by high-sensitivity differential scanning calorimetry under conditions of strong and weak electrostatic interactions of the macroions. Thermodynamic parameters of the DNA double-helix melting were determined as a function of pH and the PMAP·HCl/DNA weight ratio. PMAP·HCL was shown to reveal two functions with respect to DNA: the polyelectrolyte function and the donor-acceptor one. The first function stabilizes the helical conformation of DNA, and the second one destabilizes it. The stabilizing effect of PMAP·HCl is of entropic origin, related to a displacement of mobile counterions from the DNA's nearest surroundings by the poly(methylaminophosphazene) charged groups. The donor-acceptor function of poly(methylaminophosphazene) dominates when its electrostatic interaction with DNA is either saturated (in the complex coacervate phase at high poly(methylaminophosphazene) concentrations) or completely suppressed (in a salt medium when the polycation carries a small charge). Under these conditions, poly(methylaminophosphazene) destabilizes DNA. It preferentially binds to the DNA coil form likely via the formation of multiple labile hydrogen bonds with the donor-acceptor groups of DNA.     

Crystal structure of poly(m-phenylene isophthalamide)

The crystal structure of poly(m-phenyulene isophthalamide) was determined by x-ray analysis. The triclinic cell, with a = 5.27 Å, b = 5.25 Å, c (fiber axis) = 11.3 Å, α = 111.5°, β = 111.4° and γ = 88.0° and space group P1, contains one monomeric unit. The crystal density is 1.47 g/cc. The molecules in the crystal are contracted by 1 Å per monomeric unit from the fully extended conformation, and the planes of the benzene rings and adjacent amide groups make angles of about 30°. The crystal is composed of molecular chains connected by N? H···O hydrogen bonds along the a and b axes forming a “jungle gym” network structure. The low tensile modulus of this polymer as compared with that of poly(p-phenylene terephthalamide) is attributed to the contracted molecular conformation.     

Exploring concerted effects of base pairing and stacking on the excited‐state nature of DNA oligonucleotides by DFT and TD‐DFT studies

We have taken (dA)₅, (dT)₅, and (dA)₅·(dT)₅ as model systems to study concerted effects of base pairing and stacking on excited‐state nature of DNA oligonucleotides using density functional theory (DFT) and time dependent DFT methods. The spectroscopic states are determined to be of a partial A → A charge‐transfer nature in the A·T oligonucleotides. The T → T charge‐transfer transitions produce dark states, which are hidden in the energy region of the steady‐state absorption spectra. This is different from the previous assignment that the T → T charge‐transfer transition is responsible for a shoulder at the red side of the first strong absorption band. The A → T charge‐transfer states were predicted to have relatively high energies in the A·T oligonucleotides. The present calculations predict that the T → A charge‐transfer states are not involved in the spectra and excited‐state dynamics of the A·T oligonucleotides. In addition, the influence of base pairing and stacking on the nature of the ¹nπ* and ¹ππ* states are discussed in detail. © 2010 Wiley Periodicals, Inc. Int J Quantum Chem, 2011     

On the stability of double stranded nucleic acids

We present the first pressure-versus-temperature phase diagram for the helix-to-coil transition of double stranded nucleic acids. The thermodynamic stability of a nucleic acid duplex is a complex function of temperature and pressure and strongly depends on the denaturation temperature, T(M), of the duplex at atmospheric pressure. Depending upon T(M), pressure, and temperature, the phase diagram shows that pressure may stabilize, destabilize, or have no effect on the conformational state of DNA. To verify the phase diagram, we have conducted high-pressure UV melting experiments on poly(dIdC)poly(dIdC), a DNA duplex, poly(rA)poly(rU), an RNA duplex, and poly(dA)poly(rU), a DNA/RNA hybrid duplex. The T(M) values of these duplexes have been modulated by altering the solution ionic strength. Significantly, at low salt, these three duplexes have helix-to-coil transition temperatures of 50 degrees C or less. In agreement with the derived phase diagram, we found that the polymeric duplexes were destabilized by pressure if the T(M) is < approximately 50 degrees C. However, these duplexes were stabilized by pressure if the T(M) is > approximately 50 degrees C. The DNA/RNA hybrid duplex, poly(dA)poly(rU), with a T(M) of 31 degrees C in 20 mM NaCl undergoes a pressure-induced helix-to-coil transition at room temperature. This is the first report of pressure-induced denaturation of a nucleic acid duplex and provides new insights into the molecular forces stabilizing these structures.     

Fluorescence of the DNA double helix (dA)20 x (dT)20 studied by femtosecond spectroscopy--effect of the duplex size on the properties of the excited states

The fluorescence of the DNA double-stranded oligomer (dA)20 x (dT)20 is studied at room temperature by fluorescence up-conversion at times shorter than 10 ps. The profile of the up-conversion spectra is similar to that of the steady-state fluorescence spectrum, showing that the majority of the photons are emitted within the probed time scale. At all the probed wavelengths, the fluorescence decays are slower than those of the monomeric chromophores dAMP and TMP. The fluorescence anisotropy decays show strong wavelength dependence. These data allow us to conclude that energy transfer takes place in this double helix and that this process involves exciton states. The spectral and dynamical properties of the oligomer are compared to those of the polymer poly(dA) x poly(dT), composed of about 2000 base pairs, reported previously. The oligomer absorption spectrum is characterized by a smaller hypsochromic shift and weaker hypochromism compared to the polymer. Moreover, the fluorescence decays of (dA)20 x (dT)20 are twice as fast as those of poly(dA) x poly(dT), and its fluorescence anisotropy decays more slowly. These differences are the fingerprints of a larger delocalization of the excited states induced by an increase in the size of the duplex.