Effect of dangling ends on the stability of a DNA double helix.

The effect of 3' and 5' dangling ends has been studied on the stability of a self-complementary double-helix of d(ATGCGCAT) in 1 mol dm-3 NaCl-phosphate buffer. It was shown that the effect on the DNA was smaller than that on r(AUGCAU).     

Effect of low-molecular amines on DNA conformation and stability of the double helix]

Interaction of low-molecular amines (cystamine, cysteamine, cystaphose, asparagine, beta-alanine) with DNA was studied. The amines change the positive circular dichroism (CD) band of DNA as well as temperature and range width of melting. Effect of amines on DNA depends on ionic strength of the solvent, concentration and structure of the ligand. Monamines cause destabilization of DNA double helix followed by stabilization as ligand concentration increases. At concentrations stabilizing the double helix DNA conformation undergoes transition from the B- to C-form. The results obtained enable to relate the stabilizing effect of low-molecular amines and conformational B leads to C-transition to the non-specific interaction of ligand amino groups with DNA phosphates, and the destabilizing effect of monoamines of low concentrations to their interaction with bases, mainly in the denaturated sites of DNA. It is proposed that a stronger effectiveness of amines as compared to monovalent metals in the conformational shift of DNA towards the C-form is due to the additional effect of disturbance of hydrophobic interactions in DNA double helix.     

Influence of base sequence on the stability of the double helix of DNA.

On the basis of published measurements of the melting transitions of synthetic polydeoxyribonucleotides with known sequences we have determined the parameters of the interplane (stacking) interactions of base pairs in DNA over the range of ionic strengths from 0.01 to 0.1 M Na+. We found that deviations of the stacking-interaction energy from the mean value of 7-8 kcal/mole were extremely small and did not exceed 0.2 kcal/mole. We report an analysis of the influence of the heterogeneity of the stacking interactions on the melting parameters of polynucleotides with random sequences (models of natural DNA's). Inclusion of this effect does not significantly distort the linear dependence of the melting temperature on the relative content of G-C pairs and insignificantly affects the width of the helix-coil transition in DNA under normal conditions. However it is the heterogeneity of the stacking interactions that plays the crucial role in the melting of DNA under conditions where the difference between the relative stabilities of the A-T and G-C pairs tends to zero, as in concentrated solutions of tetraethylammonium and tetramethylammonium salts.     

Determination of stability of the DNA double helix in an aqueous medium

The possibility of determining the free energy of stabilization ΔG₀ of native DNA structure with the help of calorimetric data on heats ΔH of transition from the native to denaturated state is considered. Results of microcalorimetric measurements of heats of denaturation of T₂ phage DNA at, different values of pH and ionic strength of solution are given. Values of free energy of stabilization of the DNA native structure ΔG₀ under various conditions have been obtained. It is shown that under conditions close to physiological ΔG₀ approaches 1200 cal/mole per base pair.     

Base-stacking and base-pairing contributions into thermal stability of the DNA double helix

Two factors are mainly responsible for the stability of the DNA double helix: base pairing between complementary strands and stacking between adjacent bases. By studying DNA molecules with solitary nicks and gaps we measure temperature and salt dependence of the stacking free energy of the DNA double helix. For the first time, DNA stacking parameters are obtained directly (without extrapolation) for temperatures from below room temperature to close to melting temperature. We also obtain DNA stacking parameters for different salt concentrations ranging from 15 to 100 mM Na⁺. From stacking parameters of individual contacts, we calculate base-stacking contribution to the stability of A•T- and G•C-containing DNA polymers. We find that temperature and salt dependences of the stacking term fully determine the temperature and the salt dependence of DNA stability parameters. For all temperatures and salt concentrations employed in present study, base-stacking is the main stabilizing factor in the DNA double helix. A•T pairing is always destabilizing and G•C pairing contributes almost no stabilization. Base-stacking interaction dominates not only in the duplex overall stability but also significantly contributes into the dependence of the duplex stability on its sequence.     

Strong bending of the DNA double helix

During the past decade, the issue of strong bending of the double helix has attracted a lot of attention. Here, we overview the major experimental and theoretical developments in the field sorting out reliably established facts from speculations and unsubstantiated claims. Theoretical analysis shows that sharp bends or kinks have to facilitate strong bending of the double helix. It remains to be determined what is the critical curvature of DNA that prompts the appearance of the kinks. Different experimental and computational approaches to the problem are analyzed. We conclude that there is no reliable evidence that any anomalous behavior of the double helix happens when DNA fragments in the range of 100 bp are circularized without torsional stress. The anomaly starts at the fragment length of about 70 bp when sharp bends or kinks emerge in essentially every molecule. Experimental data and theoretical analysis suggest that kinks may represent openings of isolated base pairs, which had been experimentally detected in linear DNA molecules. The calculation suggests that although the probability of these openings in unstressed DNA is close to 10⁻⁵, it increases sharply in small DNA circles reaching 1 open bp per circle of 70 bp.     

Na2CO3 influence on DNA double helix stability: strong anion destabilizing effect

Addition of Na(2)CO(3) to almost salt-free DNA solution (5.10(-5)M EDTA, pH=5.7, T(m)=26.5 degrees C) elevates both pH and the DNA melting temperature (T(m)) if Na(2)CO(3) concentration is less than 0.004 M. For 0.004 M Na(2)CO(3), T(m)=58 degrees C is maximal and pH=10.56. Further increase in concentration gives rise to a monotonous decrease in T(m) to 37 degrees C for 1M Na(2)CO(3) (pH=10.57). Increase in pH is also not monotonous. The highest pH=10.87 is reached at 0.04 M Na(2)CO(3) (T(m)=48.3 degrees C). To reveal the cause of this DNA destabilization, which happens in a narrow pH interval (10.56/10.87) and a wide Na(2)CO(3) concentration interval (0.004/1M), a procedure has been developed for determining the separate influences on T(m) of Na(+), pH, and anions formed by Na(2)CO(3) (HCO(3)(-) and CO(3)(2-)). Comparison of influence of anions formed by Na(2)CO(3) on DNA stability with Cl(-) (anion inert to DNA stability), ClO(4)(-) (strong DNA destabilizing "chaotropic" anion) and OH(-) has been carried out. It has been shown that only Na(+) and pH influence T(m) in Na(2)CO(3) solution at concentrations lower than 0.001 M. However, the T(m) decrease with concentration for [Na(2)CO(3)]>/=0.004 M is only partly caused by high pH=10.7. Na(2)CO(3) anions also exert a strong destabilizing influence at these concentrations. For 0.1M Na(2)CO(3) (pH=10.84, [Na(+)]=0.2M, T(m)=42.7 degrees C), the anion destabilizing effect is higher 20 degrees C. For NaClO(4) (ClO(4)(-) is a strong "chaotropic" anion), an equal anion effect occurs at much higher concentrations approximately 3M. This means that Na(2)CO(3) gives rise to a much stronger anion effect than other salts. The effect is pH dependent. It decreases fivefold at neutral pH after addition of HCl to 0.1M Na(2)CO(3) as well as after addition of NaOH for pH greater than 11.2.     

NMR study of the effect of sugar-phosphate backbone ethylation on the stability and conformation of DNA double helix

Temperature variation studies of the imido proton NMR and 31P NMR resonances of the self-associated d(C-C-A-A-G-A-T-T-G-G) and d[C-C-A-A-G-p(Et)-A-T-T-G-G] duplexes (both the R and S diastereoisomers) and the heteroduplexes formed with their complementary strand d(C-C-A-A-T-C-T-T-G-G) were carried out in aqueous solution. Results demonstrate that phosphate backbone ethylation did not disrupt the interstrand hydrogen bonding involved in double-helix formation but perturbed the helix. The S isomer perturbed the duplex more than the R isomer. The line broadening patterns and faster fraying motion in the alkylated duplexes compared to those in the nonalkylated duplexes indicate that the perturbation introduced in the middle propagates along the backbone to the end of the duplex.     

Cytosine, the double helix and DNA self-assembly

DNA self-assembly has crucial implications in reading out the genetic information in the cell and in nanotechnological applications. In a recent paper, self-assembled DNA crystals displaying spectacular triangular motifs have been described (Zheng et al., 2009). The authors claimed that their data demonstrate the possibility to rationally design well-ordered macromolecular 3D DNA lattice with precise spatial control using sticky ends. However, the authors did not recognize the fundamental features that control DNA self-assembly in the lateral direction. By analysing available crystallographic data and simulating a DNA triangle, we show that the double helix geometry, sequence-specific cytosine–phosphate interactions and divalent cations are in fact responsible for the precise spatial assembly of DNA.     

Effect of N4-methylcytosine and 5-methylcytosine on the stability of the DNA helix

The thermodynamic parameters (delta H, delta S) of the helix-coil transition of self-complementary oligonucleotides d(CGCGCGCG), d(CG5mCGCGCG), d(CG4mCGCGCG), d(GGACCCGGGTCC), d(GGA5mCCCGGGTCC), and d(GGA4mCCCGGGTCC) were determined. The substitution of 4mC for C was found to decrease the melting temperature of the oligonucleotides. The destabilization effect of the two substitutions is equivalent to the change of A.T for G.C pair. The free energy decrease of the helix-coil transition due to the introduction of two 4mC into an octanucleotide was estimated to be 1,24 kcal/mol.     

Theory of the influence of oligonucleotide chain conformation on double helix stability

We consider theoretical aspects of reactions that form base pairs in a double helix. The equilibrium constant for such reactions depends on the probability of finding the two bases in the correct orientation for pairing. This probability can be expressed in terms of the spatial and angular distribution of one micleotide around the other. In this paper we use Monte-Carlo techniques to calculate the distribution of distances between chosen phosphates in nonhclical oligonucleotide backbones, using crystallographic data for bond lengths and angles, and a screened Coulomb potential for phosphate–phosphate interactions. The model chosen is one that predicts correctly the observed dimensions of an unperturbed polynucleotide chain. Knowledge of distance distribution functions permits calculation of the dependence on loop size of the probability of closing a single backbone strand into a hairpin helix. Our results agree roughly, although not exactly, with the semiempirical ring-weighting functions determined by Schefller. Elson, and Baldwin. Further results are a comparison of intramolecular and bimolecular helix nucleation equilibrium constants and a calculation of the stacking free energy in a double helix.     

Tau could protect DNA double helix structure

The hyperchromic effect has been used to detect the effect of tau on the transition of double-stranded DNA to single-stranded DNA. It was shown that tau increased the melting temperature of calf thymus DNA from 67 to 81 degrees C and that of plasmid from 75 to 85 degrees C. Kinetically, rates of increase in absorbance at 260 nm of DNA incubated with tau were markedly slower than those of DNA and DNA/bovine serum albumin used as controls during thermal denaturation. In contrast, rates of decrease in the DNA absorbance with tau were faster than those of controls when samples were immediately transferred from thermal conditions to room temperature. It revealed that tau prevented DNA from thermal denaturation, and improved renaturation of DNA. Circular dichroic spectra results indicated that there were little detectable conformational changes in DNA double helix when tau was added. Furthermore, tau showed its ability to protect DNA from hydroxyl radical (.OH) attacking in vitro, implying that tau functions as a DNA-protecting molecule to the radical.     

Force-induced melting of the DNA double helix. 2. Effect of solution conditions

In this paper, we consider the implications of the general theory developed in the accompanying paper, to interpret experiments on DNA overstretching that involve variables such as solution temperature, pH, and ionic strength. We find the DNA helix-coil phase boundary in the force-temperature space. At temperatures significantly below the regular (zero force) DNA melting temperature, the overstretching force, f(ov)(T), is predicted to decrease nearly linearly with temperature. We calculate the slope of this dependence as a function of entropy and heat-capacity changes upon DNA melting. Fitting of the experimental f(ov)(T) dependence allows determination of both of these quantities in very good agreement with their calorimetric values. At temperatures slightly above the regular DNA melting temperature, we predict stabilization of dsDNA by moderate forces, and destabilization by higher forces. Thus the DNA stretching curves, f(b), should exhibit two rather than one overstretching transitions: from single stranded (ss) to double stranded (ds) and then back at the higher force. We also predict that any change in DNA solution conditions that affects its melting temperature should have a similar effect on DNA overstretching force. This result is used to calculate the dependence of DNA overstretching force on solution pH, f(ov)(pH), from the known dependence of DNA melting temperature on pH. The calculated f(ov)(pH) is in excellent agreement with its experimental determination (M. C. Williams, J. R. Wenner, I. Rouzina, and V. A. Bloomfield, Biophys. J., accepted for publication). Finally, we quantitatively explain the measured dependence of DNA overstretching force on solution ionic strength for crosslinked and noncrosslinked DNA. The much stronger salt dependence of f(ov) in noncrosslinked DNA results from its lower linear charge density in the melted state, compared to crosslinked or double-stranded overstretched S-DNA.