Localization of low-melting regions in phage T7 DNA

DNA overstretching in the presence of glyoxal: structural evidence of force-induced DNA melting

When a long DNA molecule is stretched beyond its B-form contour length, a transition occurs in which its length increases by a factor of 1.7, with very little force increase. A quantitative model was proposed to describe this transition as force-induced melting, where double-stranded DNA is converted into single-stranded DNA. The force-induced melting model accurately describes the thermodynamics of DNA overstretching as a function of solution conditions and in the presence of DNA binding ligands. An alternative explanation suggests a transformation into S-DNA, a double-stranded form which preserves the interstrand base pairing. To determine the extent to which DNA base pairs are exposed to solution during the transition, we held DNA overstretched to different lengths within the transition in the presence of glyoxal. If overstretching involved strand separation, then force-melted basepairs would be glyoxal-modified, thus essentially permanently single-stranded. Subsequent stretches confirm that a significant fraction of the DNA melted by force is permanently melted. This result demonstrates that DNA overstretching is accompanied by a disruption of the DNA helical structure, including a loss of hydrogen bonding.

Electron microscopic studies of sequence-specific recognition of duplex DNA by different ligands

The following ligands were used to study sequence specific recognition of duplex DNA by electron microscopic techniques: methyltransferases BspR1 and EcoR124 (recognition sequences GGCC and GAAN7RTCG, respectively), a biotinylated deoxyoligonucleotide 5'-CTCTCTCTCTCTCT-3' capable of forming triplex DNA, and PNA oligomer H-T10-LysNH2. For each ligand the best conditions for electron microscopic (EM) detection of stable specific complex formation were determined. It was demonstrated that EM allowed us to determine the position of the individual target site with an error of 15-20 bp, the relative affinities for individual target sites and kinetic parameters of the binding. These results open new possibilities for EM investigations of sequence-specific interactions with a wide range of other ligands of a similar nature. They also imply that a wide range of different sequences can be unambiguously and precisely mapped by EM and greatly extend the scope of EM applications for physical mapping of genomic DNA.

Testing the quality of electron microscope mapping data for DNA molecules with sequence-specific ligands

A procedure for the testing of Electron Microscope (EM) mapping data for DNA molecules with site-specific bound ligands is suggested. The difficulty of distinguishing DNA molecule ends on electron micrographs indicates that their true orientations are not known. This in turn presents problems in obtaining correct maps relating to their alignment, and complicates checking the maps' validity. For these reasons a computer simulation of the EM study of double-stranded DNA molecules with site-specific bound ligands was carried out. The knowledge of the true orientations of the simulated DNA molecules allowed us to examine their final orientations after alignment. We used the number of improper-oriented molecules as the quantitative measure of the map quality. Detailed investigation based on this parameter permitted us to invent the criterion for the map validity, and to suggest the procedure for the testing of alignment of real DNA molecules. This procedure implies multiple randomization of initial orientations of the DNA molecules and minute analysis of the final maps. Most of the molecular, statistical and experimental parameters inherent to EM investigation of site-specific binding, such as the number of specific binding sites (N), the mean number of bound ligands (A), the length of the DNA molecules (L), the specific/non-specific ratio of binding (K), together with the standard deviation of DNA molecule lengths (HL) were tested for their influence upon the quality of EM mapping data. An empirical equation for the ultimate values of these parameters has been found, allowing us to predict the success of EM mapping.

The effect of nucleotide substitution on DNA denaturation profiles

The melting profiles were obtained for DNA restriction fragments of approx. 1150 bp with deletion of one, five or six base pairs making them different from each other. In all cases the deletions caused a shift of one melting peak without affecting the positions of the other three peaks. The effect amounted to 0.28 +/- 0.03C upon the deletion of one GC pair. The melting of DNA fragments was also studied by electrophoresis in denaturing gradient gels. The deletion of one GC pair was shown to cause an appreciable shift of the electrophoretic denaturation profile.

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.

The nonequilibrium character of DNA melting: effects of the heating rate on the fine structure of melting curves

To investigate the effects of heating rate on the DNA melting profile and to test the predictions of the theory of slow relaxation processes in DNA melting (1) concerning these effects, we obtained differential melting curves for the Bsp I C1 fragment of T7 DNA (1461 bp) and the Sma I-Eco RI fragment of Col E1 DNA (1291 bp) at heating rates of 0.05 and 0.5 deg/min. At low ionic strength (0.02 M Na+) the heating rate has been shown to affect the position of the third peak in melting curve for C1 fragment. According to the melting maps (2), this peak corresponds to the unwinding of the section between the end of the molecule and the region already melted. At high ionic strength (0.2 M Na+), when the melting of this DNA is reversible (3), the position of the peaks does not depend on the heating rate. In the case of the Col E1 DNA fragment the heating rate affects, as might be expected from the melting maps (4), only the last peak, as the melting of the last section is always nonequilibrium. The results of the study are in good qualitative agreement and in satisfactory quantitative agreement with the theoretical predictions (1).