Subunits of chromosomal DNA

A study of chromosomal DNA from Chinese hamster cells and chick fibroblasts by electron microscopy after partial denaturation revealed small regions which melted at 50° and could be stabilized by reaction with formaldehyde. The melted regions remained open so that their length and distribution along the DNA strands could be measured. The measurements indicated regularly spaced sites with low melting points at 0.4–0.5 micron intervals in most of the DNA. The length of the melted regions varied from those just visible to some as long as 0.4–0.5 microns, which probably represents the entire region between two successive sites with low melting points. A computer analysis of the spacings indicated a high probability of melted sites occurring every 2 microns along the DNA strands. Both of these spacings correspond to functional subunits of the DNA which can be isolated under appropriate metabolic conditions.     

A study of DNA denaturation in the ultracentrifuge

The melting transition of DNA in alkaline CsCl can be followed in the analytical ultracentrifuge. Equilibrium partially denatured states can be observed. These partially denatured DNA bands have bandwidths of up to several times those of native DNA. Less stable molecules melt early and are found at heavier densities in the melting region. An idealized ultracentrifuge melting transition is described. The melting transition of singly nicked PM-2 DNA resembles the idealized curve. The DNA profile is a Gaussian band at all points in the melt. DNA's from mouse, D. Melanogaster, M. lysodeikticus, T4, and T7 also show equilibrium bands at partially denatured densities, some of which are highly asymmetric. Simple sequence satellite DNA shows an all-or-none transition with no equilibrium bands at partially denatured densities. The temperature at which a DNA denatures is an increasing function of the (G + C) content of the DNA. The T_m does not show a molecular-weight dependence in the range 1.2 × 10⁶–1.5 × 10⁷ daltons (single strand) for mouse, M. lysodeikticus, or T4 DNA. The mouse DNA partially denatured bands do not change shape as a function of molecular weight. The T4 DNA intermediate band develops a late-melting tail at low molecular weight. M. lysodeikticus DNA bands at partially denatured densities become broader as the molecular weight is decreased. Mouse DNA is resolved into six Gaussian components at each point in the melting transition.     

Role of small loops in DNA melting

Short melted regions less than 100 base pairs (bp) in length are rarely found in the differential melting curves (DMC) of natural DNAs. Therefore, it is supposed that their characteristics do not affect DNA melting behavior. However, in our previous study, a strong influence of the form of the entropy factor of small loops on melting of cross-linked DNAs was established (D. Y. Lando, A. S. Fridman et al., Journal of Biomolecular Structure and Dynamics, 1997, Vol. 15, pp. 141-150; Journal of Biomolecular Structure and Dynamics, 1998, Vol. 16, pp. 59-67). Quite different dependencies of the melting temperature on the relative concentration of interstrand cross-links were obtained for the loop entropy factors given by the Fixman-Freire (Jacobson-Stockmayer) and Wartell-Benight relations. In the present study, the influence of the entropy factor of small loops on the melting of natural DNAs, cross-linked DNAs and periodical double-stranded polynucleotides is compared using computer simulation. A fast combined computational method for calculating DNA melting curves was developed for this investigation. It allows us to assign an arbitrary dependence of the loop entropy factor on the length of melted regions for the terms corresponding to small loops (less than tau bp in length). These terms are calculated using Poland's approach. The Fixman-Freire approach is used for long loops. Our calculations have shown that the temperature dependence of the average length of interior melted regions (loops) has a maximum at T approximately T(m) (T(m) is the DNA melting temperature) in contrast to the dependence of the total average length of melted regions, which increases almost monotonously. Computer modeling demonstrates that prohibition of formation of loops less than tau base pairs in length does not markedly change the DMC for tau < 150 bp. However, the same prohibition strongly affects the average length of internal melted regions for much smaller tau's. The effect is already noticeable for tau = 1 bp and increases with tau. A tenfold increase in the entropy factor of all loops with length less than tau bp causes a noticeable alteration of the DMC for tau > or = 30 bp. It is shown that DMCs are identical for the Wartell-Benight and for the Fixman-Freire (Jacobson-Stockmayer) form of the loop entropy factor. However, for low degree of denaturation, the average length of internal melted regions is 40% lower for the Wartell-Benight form due to the fluctuational opening of short AT-rich regions less than 10 bp in length. The same calculations carried out for periodical polynucleotides demonstrate a much stronger difference in melting behavior for different forms of entropy factors of short loops. The strongest difference occurs if the length of stable GC-rich and unstable AT-rich stretches is equal to 30 bp. However, the comparison carried out in this work demonstrates that the entropy factor of short loops influences melting behavior of cross-linked DNA much stronger than of unmodified DNA with random or periodical sequences.     

Denaturation mapping of R factor deoxyribonucleic acid.

The R factor NR1 consists of two components: a resistance transfer factor which harbors the tetracycline resistance genes (RTF-TC) and the r-determinants component which harbors the other drug resistance genes. Using partial denaturation mapping it is possible to distinguish the RTF-TC region from the r-determinants region of the composite R factor NR1 DNA which has a contour length of 37 mum and a density of 1.712 g/ml. The r-determinants region was a relatively undenatured 8.5-mum segment of the molecule when the deoxyribonucleic acid was partially denatured at pH 10.7. An RTF-TC genetic segregant of NR1 which had lost the r-determinants component had a contour length of 28.7 mum and a density of 1.710 g/ml. Characterization of an RTF-TC using partial denaturation mapping at pH 10.7 confirmed that the relatively undenatured 8.5-mum r-determinants segment of the composite R factor had been deleted. Circular, transitioned NR1 DNA molecules (1.716 to 1.718 g/ml), whose contour lengths were consistent with an RTF-TC plus an integral number of tandem copies of r-determinants, were also characterized by denaturation mapping. The relatively undenatured region in these molecules had a length equal to an integral number of copies of r-determinants and was located at the same site in the partially denatured RTF-TC as the single copy of r-determinants in the 37-mum composite NR1. This indicates that there is a unique integration site for r-determinants in the RTF-TC component. The R factor UCR122, a TC deletion mutant of NR1, was also characterized by denaturation mapping. The translocation of the TC resistance gene(s) on the denaturation map permitted the alignment of the denaturation map with the heteroduplex map of Sharp et al. (u073). Linear and circular monomeric and presumed multimeric r-determinants DNA molecules (p = 1.718 g/ml) were partially denatured at a higher pH (11.10). The r-determinants multimers showed a repeating 8.3-mum (monomeric) partial denaturation pattern indicating a head-to-tail arrangement of monomers in these poly-r-determinant molecules.     

Anatomy of herpes simplex virus DNA. II. Size, composition, and arrangement of inverted terminal repetitions.

Electron microscope studies on self-annealed intact single strands and on partially denatured molecules show that herpes simplex virus 1 DNA consists of two unequal regions, each bounded by inverted redundant sequences. Thus the region L (70 percent of the contour length of the DNA) separates the left terminal region a1b from its inverted repeat b'a'1, each of which comprises 6 percent of the DNA. The region S (9.4 percent of DNA) separates the right terminal region cas (4.3 percent of the DNA) from its inverted repeat a'sc'. The regions of the two termini which are inverted and repeated itnernally differ in topology. Thus, cas is guanine plus cytosine rich, whereas only the terminal 1 percent of the a1b region, designated as subregion a1, is guanine plus cytosine rich.     

Localization of low-melting regions in phage T7 DNA

Specific fragmentation of T7 DNA at glyoxal-fixed denatured regions by the S1 endonuclease followed by restriction analysis made it possible to localize four low-melting regions in phage T7 DNA. These regions have the following coordinates:0.5-1.2;14.8+/-0.3;46.3+/-0.5; 98.4+/-0.3 (in T7 DNA length units). The location of the low-melting regions was refined by means of electron-microscopic denaturation mapping and gel electrophoresis of partially denatured DNA. The obtained localization of the low-melting regions is consistent with the available data on the sequence of T7 DNA. The map of low-melting regions was compared with the genetic map of T7 DNA.Images     

Calculation of melting curves for DNA

A method is reported for calculating the melting curve of a DNA molecule of random base sequence, including in the formalism the dependence of the free energy of base pair formation on the size of a denatured section. Some explicit results are shown for a “typical” base sequence, in particular the probability of helix formation at individual base pairs in several different regions of the molecule and the amount of melting from the end of the chain. Particular attention is drawn to the variation of local melting behavior from one region of the molecule to another. It is found that sections rich in AT melt at relatively low temperatures with a fairly broad transition curve, whereas regions rich in GC pairs melt at higher temperatures (as expected) with a very abrupt, local transition curve. To account qualitatively for the results one may divide melting into two kinds of processes: (a) the nucleation and growth of denatured regions, and (b) the merging together of two denatured sections at the expense of the intervening helix. The first of these processes dominates in the first stages of melting, and leads to rather broad local melting curves, whereas the second process predominates in the later stages, and occurs, in a particular part of the molecule, over a very narrow temperature range. It is estimated that the average length of a helix plus adjacent coil section at the midpoint of the transition is approximately 600 base pairs. Since transition curves which measure the local melting behavior reflect local compositions fluctuations, these curves contain information about the broad outlines of base sequence in the molecule. Some suggestions are made concerning experiments by which this potential information source could be exploited. In particular, it is pointed out that one might hope to map AT or GC rich regions at particular genetic loci in a biologically active DNA molecule. Values of the relevant parameters found earlier for the transition of homopolymers produce melting curves for a DNA of random base sequence which are in good agreement with the experimental transition curve for T2 phage DNA. Hence the present theoretical picture of the melting of polynucleotides is at least internally self-consistent.     

Thermal denaturation of chromatin and lysine copolymer-DNA complexes. Effects of ethylene glycol.

Chromatin was thermally denatured in the presence and absence of 1M ethylene glycol using a technique whereby both the hyperchromism and ellipticity are monitored simultaneously. Model complexes containing poly(L -Lys) or poly(L -Lys, L -Ala, Gly) and DNA were similarly melted in order to assist in interpreting the chromatin results. In both cases a general pattern emerged whereby ethylene glycol perturbed the resultant melting profile, showing increased hyperchromicity, ellipticity, and premelt slope. In addition, ethylene glycol destabilizes and reduces the high melting region of polypeptide-bound DNA and the extent of higher ordered structure in model complexes and chromatin. These results emphasize the importance of hydrophobic forces in polypeptide–polypeptide and polypeptide–DNA interactions.     

DNase I footprinting and enhanced exonuclease function of the bipartite Werner syndrome protein (WRN) bound to partially melted duplex DNA.

Werner syndrome is a premature aging and cancer-prone hereditary disorder caused by deficiency of the WRN protein that harbors 3' -->5' exonuclease and RecQ-type 3' --> 5' helicase activities. To assess the possibility that WRN acts on partially melted DNA intermediates, we constructed a substrate containing a 21-nucleotide noncomplementary region asymmetrically positioned within a duplex DNA fragment. Purified WRN shows an extremely efficient exonuclease activity directed at both blunt ends of this substrate, whereas no activity is observed on a fully duplex substrate. High affinity binding of full-length WRN protects an area surrounding the melted region of the substrate from DNase I digestion. ATP binding stimulates but is not required for WRN binding to this region. Thus, binding of WRN to the melted region underlies the efficient exonuclease activity directed at the nearby ends. In contrast, a WRN deletion mutant containing only the functional exonuclease domain does not detectably bind or degrade this substrate. These experiments indicate a bipartite structure and function for WRN, and we propose a model by which its DNA binding, helicase, and exonuclease activities function coordinately in DNA metabolism. These studies also suggest that partially unwound or noncomplementary regions of DNA could be physiological targets for WRN.     

The denaturation transition of DNA in mixed solvents

The helix-to-coil denaturation transition in DNA has been investigated in mixed solvents at high concentration using ultraviolet light absorption spectroscopy and small-angle neutron scattering. Two solvents have been used: water and ethylene glycol. The "melting" transition temperature was found to be 94 degrees C for 4% mass fraction DNA/d-water and 38 degrees C for 4% mass fraction DNA/d-ethylene glycol. The DNA melting transition temperature was found to vary linearly with the solvent fraction in the mixed solvents case. Deuterated solvents (d-water and d-ethylene glycol) were used to enhance the small-angle neutron scattering signal and 0.1M NaCl (or 0.0058 g/g mass fraction) salt concentration was added to screen charge interactions in all cases. DNA structural information was obtained by small-angle neutron scattering, including a correlation length characteristic of the inter-distance between the hydrogen-containing (desoxyribose sugar-amine base) groups. This correlation length was found to increase from 8.5 to 12.3 A across the melting transition. Ethylene glycol and water mixed solvents were found to mix randomly in the solvation region in the helix phase, but nonideal solvent mixing was found in the melted coil phase. In the coil phase, solvent mixtures are more effective solvating agents than either of the individual solvents. Once melted, DNA coils behave like swollen water-soluble synthetic polymer chains.     

Equilibrium melting of plasmid ColE1 DNA: electron-microscopic visualization.

The fine structure of the melting curve for the linear colE1 DNA has been obtained. To find the ColE1 DNA regions corresponding to peaks in the melting curve's fine structure, we fixed the melted DNA regions with glyoxal /12/. Electron-microscopic denaturation maps were obtained for nine temperature points within the melting range. Thereby the whole process of colE1 DNA melting was reconstructed in detail. Spectrophotometric and electron microscopic data were used for mapping the distribution of Gc-pairs over the DNA molecule. The most AT-rich DNA regions (28 and 37% of GC-pairs), 380 and 660 bp long resp., are located on both sides of the site of ColE1 DNA's cleavage by EcoR1 endonuclease. The equilibrium denaturation maps are compared with maps obtained by the method of Inman /20/ for eight points of the kinetic curve of ColE1 DNA unwinding by formaldehyde.     

Fine structures in denaturation curves of bacteriophage lambda DNA. Their relation to the intramolecular heterogeneity in base compositon.

Precise recording of polyphasic optical melting curves was carried out for three kinds of bacteriophage lambda DNA differing in length (lambdac1857s7, lambdacIb2 and lambdacIb2b5). Each of denaturation steps in melting profiles was characterized by two parameters, the melting temperature and the relative size. Any difference in fine structures in melting profiles was not recognized between the intact lambdacI857s7DNA and the DNA fragmented into halves. The change in fine structures in melting profiles caused by the deletions of the b2 and b5 region agreed qualitatively well with the prediction based on the physical and the genetical maps of phage lambda chromosome. The combined results indicate that, first, the well-known linear relationship between melting temperature and G+C content may apply also to each of denaturation steps in polyphasic melting curves due to heterogeneity of nucleotide distribution in a single DNA species, and, second, the effect of molecular ends on melting fine structures can be neglected at moderate salt concentration (0.01 M less than or equal to Na+ less than or equal to 0.2 M) for such a high molecular weight DNA. The heterogeneous distribution of nucleotides was derived for lambdaDNA and for its b2 and b5 regions.     

Intramolecular DNA melting between stable helical segments: melting theory and metastable states.

Melting of DNA in a segment bounded at both ends by regions of greater stability during electrophoresis in denaturing gradient gels show complex properties, not accommodated with standard melting theory. Compact bands of some DNA molecules become anomalously broadened at the retardation level in a denaturing gradient, or double bands may appear in a uniform denaturant concentration. These properties are associated only with molecules for which the distribution of stability calculated by the Poland-Fixman-Freire algorithms indicates that the region of lowest stability does not extend to an end of the molecule. Retention of helicity at the ends is shown by the difference in the effect of base substitution in the end domains and in the least stable domain. Both the appearance of double bands and band broadening can be explained by invoking a hypothetical metastable intermediate in melting, which is converted into the equilibrium melted form at a relatively slow rate, depending on both denaturant concentration and field strength. A kinetic model permits plausible rate constants to be inferred from the patterns. Despite the increased band width, sequence variants with base changes in the least stable domain result in readily detectable band shifts in the gradient.     

The kinetics of DNA helix-coil subtransitions

The kinetic analysis of individual helix-coil subtransitions were performed by comparing melting and renaturation profiles obtained at different temperature change rates. The duration of the three transition stages and its dependence on temperature and ionic strength were determined for a T7 phage DNA fragment. The obtained temperature dependence of the melting time for a stretch flanked by melted regions is in quantitative agreement with that predicted by the theory of slow processes (V.V. Anshelevich, A.V. Vologodskii, A.V. Lukashin, M.D. Frank-Kamenetskii, Biopolymers 23, 39 (1984)). The reasons are discussed for the increasing relaxation time of this stretch in the middle of its transition with decreasing ionic strength. The zipping kinetics of a melted region under essentially nonequilibrium conditions was examined for T7 fragment and pAO3 DNAs. The obtained temperature dependence of the zipping time is in quantitative agreement with calculations based on the theory of slow processes. The renaturation times of stretches flanked by helical regions proved fairly small even at a low ionic strength. These times are several orders of magnitude smaller than the renaturation times of the same stretches with one helical boundary. A formal application of the theory of slow processes failed to account for the small renaturation times of stretches that are zipped from both ends. This is probably due to the non-allowance for the changing entropy of the loop linking two helix-coil boundaries migrating towards each other. Slow processes have been revealed in the intramolecular melting of Col E1 DNA at a high ionic strength. The reason for the long relaxation time of one subtransition is the large size of the loop that separates the melting stretch from the helical part of the molecule. This result can be accounted for by the theory of slow processes.     

Electron microscope maps of SA7 DNA melting

Electron microscopic denaturation maps corresponding to the first peaks of the differential melting curve of SA7 DNA were constructed by fixation of partly denatured molecules with glyoxal at temperatures within the melting range. These maps were oriented with respect to the functional map of the virus genome. The localization and the size of the most AT-rich SA7 DNA regions were determined.     

The thermal denaturation of DNA: average length and composition of denatured areas

A spectral study of melting curves of DNA ranging from 73 to 32% AT indicates that the base ratio of sequences melting within DNA are a linear function of temperature. A study of partially denatured DNA by electron microscopy, reversible renaturation and fractionation on hydroxylapatite suggests that the melting curve of DNA represents the melting of sequences which average 3-4 million daltons in length. These sequences appear to be a combination of two areas, one which is high in AT and denatures in the first three-quarters of the melting curve, and one which is high in GC and denatures in the final quarter. The length of these sequences appears to vary between 1.5-6 million daltons.     

Determination of Melting Sequences in DNA and DNA-Protein Complexes by Difference Spectra

A graphical formula is presented for determining the base ratio of melted DNA. By use of this formula, the composition of sequences which melt in different portions of the melting curves of Clostridium DNA, Escherichia coli DNA, and mouse DNA were determined. As the DNA melts, the per cent of adenine and thymine (AT) in the melted sequences decreases linearly with temperature. The average composition of sequences which melt in a given part of the melting curve is proportional to the base ratio of the DNA. The concentration and average composition of sequences were determined for three parts of the melting curves of the DNA samples, and a frequency distribution curve was constructed. The curve is symmetrical and has a maximum at about 56% AT. The distribution of GC-rich sequences on the E. coli chromosome was estimated by shearing, partially melting, and fractionating the DNA on hydroxylapatite. GC-rich sequences appear to occur every thousand base pairs, and have a maximum length of about 180 base pairs. The graphical formula was applied to the determination of the composition of sequences which melt in different parts of the melting curve of chromatin. Throughout the melting curve, the composition of the melting sequences is about 60% AT, which appears to suggest that relatively long sequences are melting simultaneously. Their melting temperature may be a function of the composition of the protein on different parts of the DNA. The problem of light scattering in DNA-protein and DNA was also investigated. A formula is presented which corrects for light scattering by relating the intensity of the scattered light to the rate of change of absorbance of DNA with wavelength.     

Partial denaturation of mouse DNA in preparative CsCl density gradients at alkaline pH.

A new technique--partial denaturation of DNA in equilibrium CsCl density gradients at pH 11.4--is used to determine the distribution of intermediate states in the melting of mouse DNA. When the technique is applied in the preparative ultracentrifuge, the DNA is fractionated according to stability. Neutralization of the partially denatured fractions results in the recovery of most of the DNA in its native form. The individual fractions are more homogeneous than the total DNA: they have decreased density heterogeneity (smaller band widths), neutral CsCl buoyant densities that differ from the average, and more homogeneous melting profiles with melting temperatures that differ from the average.     

Why is the denaturation process of super-helical DNA so uncooperative?

A theoretical model is proposed for the helix-coil transition in circular covalently closed DNA. In the melting interval the topological constrains for such a molecule are considered to affect both the inner state of the melted regions and the spatial configuration of the whole molecule ("writhing"). A good agreement is achieved between the theoretically calculated and experimentally obtained parameters of the denaturation process. A conclusion is drawn, that at the early stages of thermodenaturation (approximately till the transition midpoint) the effect of topological constrains is realised mainly through the writhing of the molecule. The denatured regions exist in the form of relaxed loops.