Melting of short DNA fragments. Relation between the nucleation constant of a spiral region and the ionic strength

Melting of two DNA duplexes of known nucleotide sequences containing 14 and 36 base pairs has been investigated within the range of ionic strength from 0.2 to 0.02 M [Na+]. The values of melting enthalpy of base pair delta H were measured for the duplex of 14 base pairs in the solutions of varying ionic strength. The values of delta H were obtained from slopes of linear plots of reciprocal melting temperature versus logarithm of oligonucleotide chains concentration. In the aforementioned range the decrease of the ionic strength causes a 5% decrease of delta H. By fitting the theoretical profiles to the experimental ones the ionic strength dependence of the nucleation constant beta was measured for DNA fragments of various lengths. With the decrease of the ionic strength the value of beta drops 2 times for the short duplex and 8 times for the long one.     

A Mesoscale Model of DNA and Its Renaturation

A mesoscale model of DNA is presented (3SPN.1), extending the scheme previously developed by our group. Each nucleotide is mapped onto three interaction sites. Solvent is accounted for implicitly through a medium-effective dielectric constant and electrostatic interactions are treated at the level of Debye-Hückel theory. The force field includes a weak, solvent-induced attraction, which helps mediate the renaturation of DNA. Model parameterization is accomplished through replica exchange molecular dynamics simulations of short oligonucleotide sequences over a range of composition and chain length. The model describes the melting temperature of DNA as a function of composition as well as ionic strength, and is consistent with heat capacity profiles from experiments. The dependence of persistence length on ionic strength is also captured by the force field. The proposed model is used to examine the renaturation of DNA. It is found that a typical renaturation event occurs through a nucleation step, whereby an interplay between repulsive electrostatic interactions and colloidal-like attractions allows the system to undergo a series of rearrangements before complete molecular reassociation occurs.     

Specificity-enhanced hot-start PCR: addition of double-stranded DNA fragments adapted to the annealing temperature

A new method to produce hot-start conditions in PCR is described. Short double-stranded DNA fragments were found to inhibit the activity of DNA polymerases from Thermus aquaticus and Thermus flavus. This inhibition is not sequence specific, but exclusively dependent on the melting temperature of the fragments as shown by its correlation to their melting curves as measured. This property is exploited by adding fragments of the appropriate length to the PCR mixture during the reaction setup and thereby preventing the DNA polymerases from extending primers annealed nonspecifically at lower than the optimal temperature. By amplifying ten copies of phage lambda DNA in the presence of 2 micrograms of nonspecific DNA, it is shown for three different primer pairs how the melting temperatures of the double-stranded DNA fragments have to be adapted to the cycle profiles to obtain predominantly specific products in the 0.5 microgram range.     

Electron microscopy of the melting of sequenced DNA

Differential melting curves (DMCs) of DNAs pA03 and pBR322 in solutions of different ionic strength (0.02 and 0.2M Na⁺) were obtained. A previously developed procedure of glyxal fixation of partially denatured DNA molecules at temperatures within the melting range was used to construct electron-microscopic melting maps for pBR322 and pAO3 plasmid DNA and for the replicative form of bacteriophage ?X174 DNA, allowing the melting of these DNA molecules to be followed in solutions of low (0.1 × SSC) and high (1 × SSC) ionic strength. In spite of the fact that the melting was at nonequilibrium at the low ionic strength, the melting maps for the two kinds of solutions practically coincided. Experimental data are compared with theoretical calculations based on the Fixman-Freire algorithm. The conclusion is that the melting pattern of these DNAs is, on the whole, correctly described by the theory, although there are appreciable differences between the theoretical and experimental differential melting curves. We have also determined the relation between the melting temperature of a region and its GC content, with allowances made for the boundary conditions of melting in 0.1 × SSC and 1 × SSC solutions, and have analyzed the theoretical shape of peaks of the DMCs.     

Salt dependence and thermodynamic interpretation of the thermal denaturation of small DNA restriction fragments.

The influence of cation concentration on the thermal denaturation of DNA restriction fragments from the E. coli lac regulatory region and from pVH51, ranging in size from 43- to 880- bp, is described. Upon increasing the ionic strength, the melting transitions broaden in a cooperative manner at salt concentrations characteristic for the specific fragment. For three fragments studied in detail, the salt concentration dependence at the midpoint varied between 0.03 and 0.19 M Na+. Along with the broadening, the melting transitions become more symmetrical. This result is discussed with respect to the irreversibility of melting transitions at low ionic strength. After a cooperative broadening, the shape of the melting curves remains constant up to salt concentrations of 0.5 M Na+. The dTM/dlog[Na+] values for three fragments fall between 15.7 and 16.7. An easily applicable approximation of the van't Hoff equation is used to evaluate the enthalpies of 13 transitions arising from the denaturation of 43 to 600 bp. The results of this analysis are compared to calculations of the expected enthalpies based on calorimetric measurements. The TMs of most transitions were directly related to the base composition, but several deviations from the predicted behavior were observed. The possible influences of fragment length and sequence on the thermal stability are discussed. The experimental and mathematical procedure to resolve a thermal denaturation transition with a width f 0.17 +/- 0.01 degrees and its distinction from another preceeding transition only approximately 0.15 degrees away in an 880-bp Hae III fragment from pVH51 is described. This transition is about half as wide as the smallest one reported to date.     

The ionic strength dependence of the cooperativity factor for DNA melting

The melting temperature for the d(AT)24.d(AT)24 stretch, located inside the DNA helix and terminally, have been determined in a wide range of ionic strength values (0.01 - 1 M Na+). The cooperativity factor was calculated from the shifts in the melting temperature of the stretch due to its different boundary conditions. With the sodium concentration decreasing from 1 M to 0.01 M the cooperativity factor dropped by three orders of magnitude, its change being less marked at high than at low ionic strength.     

DNA orientation in shear flow

The linear dichroism (LD) has been measured for DNA molecules 239–164,000 base pairs long oriented in shear flow over a large range of velocity gradients (30–3,000 s ^?1) and ionic strengths (2–250 mM). At very low gradients, the degree of DNA orientation increases quadratically with the applied shear as predicted by the Zimm theory [J. Zimm, (1956) Chemical Physics, Vol. 24, p. 269]. At higher gradients, the orientation of fragments ≥ 7 kilobase pairs (kbp) increases linearly with increasing shear, whereas the orientation of fragments ≥ 15 kbp shows a more complicated dependence. In general, the orientation decreases with increasing ionic strength throughout the studied ionic strength interval, owing to a decrease in the persistence length of the DNA. The effect is most dramatic at ionic strengths below 10 mM, and is more pronounced for longer DNA fragments. For fragments ≥ 15 kbp and velocity gradients ≥ 100 s^?1, the orientation can be adequately described by the empirical relation: LD^r= –(k₁-G)/(k₂ + G), where k₁is a linear function of the square root of the ionic strength and k₂ depends on the DNA contour length. Since the DNA persistence length can be represented as a linear function of the reciprocal square root of the ionic strength [D. Porschke, (1991) Biophysical Chemistry, Vol. 40, p. 169], extrapolation of the empirical relation provides information about the stiffness of the DNA fibers. © 1993 John Wiley & Sons, Inc.     

Melting of oligodeoxynucleotides with various structures

Effects of DNA fragments end structures on their melting profiles were studied experimentally and theoretically. We examined melting of hairpins and dumbbells obtained from 62-bp-long linear DNA duplex which is a perfect palindromic sequence. To fit theoretical melting profile to experimental ones additional theoretical parameters were incorporated into the standard statistical mechanical helix-coil transition theory. From comparison theoretical and experimental melting profiles theoretical parameters connected with end-structure effects were evaluated. Analysis revealed the stabilization effect of the hairpin loops and helix ends with respect to DNA duplex melting. Both type of ends make melting these oligodeoxynucleotides more cooperative than predicted by the standard helix-coil transition theory. At low ionic strength ([Na+] less than 0.04 M) this effect becomes so pronounced that melting of the DNA duplexes 30-40 bp-long conforms to the two state model. From the analysis experimental data obtained for dumbbell structures loop-weighting factor for single-stranded loop consisting of 132 nucleotides was determined. This parameter decreases 10 times with the ionic strength decreasing by an order of magnitude from 0.2 to 0.02 M Na+.     

DNAase hydrolysis of chromatin DNA in intact sea urchin sperm cells. Effect of the ionic strength on the digestion parameters.

Chromatin DNA in intact functional Sphaerechinus granularis sperm cells has been digested with micrococcal nuclease at three different ionic strength conditions. The results show a highly-flexible chromatin organization similar to that found in sperm heads. The rate of digestion, the limit value of acid-soluble material and the fragmentation pattern show that the sensitivity of nucleosome and internucleosome DNA regions to nuclease hydrolysis depends on a delicate balance of polar and non polar interactions. At low ionic strength, both nucleosome and internucleosome regions are rapidly and completely hydrolysed at the same time and a transient subunit fragment of 120 b.p. average length is formed. At high ionic strength, internucleosome regions are preferentially hydrolysed; there is a limit digest value and a stable subunit fragment of 140 b.p. average length is formed. A supernucleosome organization in the high ionic strength environment of the sperm cells is suggested by the transient preferential formation of heptamers of nucleosome DNA fragments.     

DNA persistence length revisited

DNA restriction fragments ranging from 79 to 789 base pairs in length have been characterized by transient electric birefringence (TEB) measurements at various temperatures between 4 and 43 degrees C. The DNA fragments do not contain runs of four or more adenine residues in a row and migrate with normal electrophoretic mobilities in polyacrylamide gels, indicating that they are not intrinsically curved or bent. The low ionic strength buffers used for the measurements contained 1 mM Tris Cl, pH 8.0, EDTA, and variable concentrations of Na(+) or Mg(2+) ions. The rotational relaxation times were obtained by fitting the TEB field-free decay signals with a nonlinear least-squared fitting program; the decay of the birefringence was monoexponential for fragments < or = 241 base pair (bp) in length and multiexponential for larger fragments. The terminal relaxation times, characteristic of the end-over-end rotation of the DNA molecules, were then used to determine the persistence length (p) and hydrodynamic radius (r) of DNA as a function of temperature and ionic strength, using several different hydrodynamic models. The specific values obtained for p and r are model dependent. The wormlike chain model of P. J. Hagerman and B. H. Zimm (Biopolymers 1981, Vol. 20, pp. 1481-1502) combined with the revised Broersma equation (J. Newman et al., Journal of Mol Biol 1997, Vol. 116, pp. 593-606) appears to be the most suitable for describing the flexibility of DNA in low ionic strength solutions. The values of p and r obtained from the global least squares fitting of this equation are independent of DNA length, and the deviations of the individual values from the average are reasonably small. The consensus r value calculated for DNA in various low ionic strength solutions containing 1 mM Tris buffer is 14.7 +/- 0.4 A at 20 degrees C. The consensus p values decrease from 814 approximately 564 A in solutions containing 1 mM Tris buffer plus 0.2-1 mM NaCl and decrease still further to 440 A in solutions containing 0.2 mM Mg(2+) ions. The persistence length exhibits a shallow maximum at 20 degrees C and decreases slowly upon either increasing or decreasing the temperature, regardless of the model used to fit the data. By contrast, the consensus values of the hydrodynamic radius are independent of temperature. The calculated persistence lengths and hydrodynamic radii are compared with other data in the literature.     

Melting of Oligodeoxynucleotides with Various Structures

Abstract

Effects of DNA fragments end structures on their melting profiles were studied experimentally and theoretically. We examined melting of hairpins and dumbbells obtained from 62- bp-long linear DNA duplex which is a perfect palindromic sequence. To fit theoretical melting profile to experimental ones additional theoretical parameters were incorporated into the standard statistical mechanical helix-coil transition theory. From comparison theoretical and experimental melting profiles theoretical parameters connected with end- structure effects were evaluated. Analysis revealed the stabilization effect of the hairpin loops and helix ends with respect to DNA duplex melting. Both type of ends make melting these oligodeoxynucleotides more cooperative than predicted by the standard helix-coil transition theory. At low ionic strength ([Na⁺] < 0.04 M) this effect becomes so pronounced that melting of the DNA duplexes 30–40 bp-long conforms to the two state model.

From the analysis experimental data obtained for dumbbell structures loop-weighting factor for single-stranded loop consisting of 132 nucleotides was determined. This parameter decreases 10 times with the ionic strength decreasing by an order of magnitude from 0.2 to 0.02 M Na⁺.     

Flow birefringence of T7 phage DNA: Dependence on salt concentration

We have determined extinction angles and flow birefringence of T7 bacteriophage DNA over a wide range of shear, polymer concentration, and solvent ionic strength. From these data, information on the simple salt dependence of coil permeability to solvent and on short-range intrachain interactions (persistence length) was obtained. At all ionic strengths, our results are consistent with a partially draining coil in the Gaussian subchain dynamical theory of Rouse-Zimm-Tschoegl-Bloomfield. Salt dependence of persistence length is comparable to, although somewhat less than, that obtained previously using similar methods with a fivefold higher-molecular-weight DNA (T2 bacteriophage DNA). Possible reasons for observed discrepancies are analyzed, and the results of this work are compared in detail to other current studies of solvent ionic strength dependence in persistence length and hydrodynamic properties of DNA.     

Denaturation of mouse satellite DNA upon melting of chromatin in solution

The denaturation of mouse satellite DNA upon melting of chromatin in solution of low ionic strength has been studied. A procedure for preparation of partially denaturated chromatin was developed which enabled the isolation of double-stranded (non-denatured) DNA sequences according to their thermal stability in chromatin. The content of mouse satellite DNA in these DNA sequences was determined by hybridization with RNA, complementary to satellite DNA in order to find the temperature interval of denaturation of satellite DNA. It was found that the melting temperature of satellite DNA in chromatin was lower than that of the total DNA. The results are discussed in relation to previously reported anomalous behaviour of satellite DNA upon melting of chromatin on hydroxyapatite.     

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.     

Monitoring of fluorescence during DNA melting as a method for discrimination and detection of PCR products in variety identification

DNA melting curves of genotype-specific PCR fragments were used to differentiate between species and amongst varieties of cereals. Melting curves were generated by ramping the temperature of PCR fragments through their dissociation temperature in the presence of a double-stranded DNA binding dye. Genotypes were discriminated by differences in the position and shape of the melting curve which is a function of the fragment's sequence, length and GC content. Amplification of 5S ribosomal RNA genes generated species-specific fragments for six of the major cereal crops. Of the 15 possible pairwise comparisons, 13 distinctions could be reliably made using melting curve position data. Wheat varieties were identified by the melting profiles of PCR products generated using microsatellite primers. DNA melting curve analysis was conveniently coupled with capillary-PCR using a LightCycler instrument to provide a rapid method of genotyping in cereals.     

Comparison between histones FV and F2a2 of chicken erythrocyte. II. Interaction with homologous DNA.

The conformation and stability of artificial complexes between chicken erythrocyte DNA and homologous histones FV and F2a2 was studied by circular dichroism (CD) and thermal denaturation followed by both absorbance and CD measurements. The complexes are made after a stepwise potassium fluoride gradient dialysis without urea and studied at low ionic strength (10-minus 3 M). 1) No structural changes of the DNA can be detected up to r equals 0.2 with FV and r equals 0.6 for F2a2. With FV at higher values of r the CD spectrum is altered, indicating the organization of DNA and histones in some kind of aggregate. 2) The conformation of histone molecules inside the complexes is not related to the ionic strength of the medium but to an effective ionic environment close to 0.1 M. This ionic strength would also correspond to the melting temperature of histone-covered DNA. 3) From the analysis of the absorbance melting profile the length of DNA covered with an histone molecule can be estimated. A good agreement is found between the negative charge of this piece of DNA and the net positive charge of the histone. 4) Since the CD transition at 227 nm occurs before the second absorbance transition at 280 nm, the DNA is stabilized no longer by native histone but partially or fully denatured histones. The helical regions of the histone molecule are not involved in the binding process, which appears to be almost purely coulombian and most likely related to some structural fit between the pattern of negative charges in the DNA helix and that of positive charges along the peptide chain.     

Helix-coil transition in nucleoprotein. Effect of ionic strength on thermal denaturation of polylysine-DNA complexes

Thermal denaturation of direct-mixed and reconstituted polylysine–DNA complexes in 2.5 × 10^?4 M EDTA, pH 8.0 and various concentrations of NaCl has been studied. For both complexes, increasing ionic strength of the solution raises T_m, the melting temperature of free base pairs. The linear dependence of T_m on log Na⁺ indicates that the concept of electrostatic shielding on phosphate lattice of an infinitely long pure DNA by Na⁺ can be applied to short free DNA segments in a nucleoprotein. For a direct-mixed polylysine–DNA complex, the melting temperature of bound base pairs T_m′ remains constant at various ionic strengths. On the other hand, the T_m′ in a reconstituted polylysine–DNA complex is shifted to lower temperature at higher ionic strength. This phenomenon occurs for reconstituted complex with long polylysine of one thousand residues or short polylysine of one hundred residues. It is shown that such a decrease of T_m′ is not due to a reduction of coupling melting between free and bound regions in a complex when the ionic strength is raised. It is also not due to intermolecular or intramolecular change from a reconstituted to a direct-mixed complex. It is suggested that this phenomenon is due to structural change on polylysine-bound regions by ionic strength. It is suggested further that Na⁺ may replace water molecules and bind polylysine-bound regions in a reconstituted complex. Such a dehydration effect destabilizes these regions and lowers T_m′. This explanation is supported by circular dichroism (CD) results.     

Investigation of the flexibility of DNA using transient electric birefringence

In the preceding article, a Monte Carlo analysis was presented which provides a quantitative numerical relationship between the rotational diffusion coefficients, as measured by the decay of optical anisotropy following an electric field pulse, and the flexibility (persistence length) of short, wormlike chains. In the present article, the results of the foregoing analysis are applied to the observed rates of decay of birefringence for a series of sequenced DNA fragments ranging in size from 104 to 910 base pairs. Under the conditions used in this study, the DNA fragments exist as native, duplex molecules. Furthermore, conditions are defined in which the observed relaxation times are not dependent on DNA concentration, field strength, or the duration of the pulse. It is pointed out that the ionic atmosphere associated with a wormlike polyion does not exert any significant (direct) influence on the rotational diffusion of the polyion and, therefore, that the rotational relaxation times are a true measure of the configurations of the DNA molecules in solution. Moreover, excluded-volume effects are shown not to be significant for the moderately short molecules employed in this study. The major conclusion of this study is that there is no strong ionic strength dependence of the persistence length for ionic strengths above 1 mM and that the persistence length, under conditions where electrostatic contributions are negligible, is approximately 500 Å. For ionic strengths significantly lower than 1 mM, electrostatic contributions to the stiffness of DNA become significant.