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The Poland-Fixman-Freire formalism was adapted for modeling of calorimetric DNA melting profiles, and applied to plasmid pBR 322 and long random sequences. We studied the influence of the difference (HGC -HAT ) between the helix-coil transition enthalpies of AT and GC base pairs on the calorimetric melting profile and on normalized calorimetric melting profile. A strong alteration of DNA calorimetrical profile with HGC -HAT was demonstrated. In contrast, there is a relatively slight change in the normalized profiles and in corresponding ordinary (optical) normalized differential melting curves (DMCs). For fixed HGC -HAT , the average relative deviation (S) between DMC and normalized calorimetric profile, and the difference between their melting temperatures (Tcal -Tm ) are weakly dependent on peculiarities of the multipeak fine structure of DMCs. At the same time, both the deviation S and difference (Tcal -Tm ) enlarge with the temperature melting range of the helix-coil transition. It is shown that the local deviation between DMC and normalized calorimetric profile increases in regions of narrow peaks distant from the melting temperature.

Although many anticancer drugs exert their biological activity by forming DNA interstrand crosslinks (ICLs), the thermodynamics of biologically relevant long crosslinked DNAs has not been intensively studied in contrast to short duplexes. Here, we carry out computer modeling of the shift of melting temperature of long DNAs caused by ICLs taking into account crosslinking effect in itself and concomitant local alterations in the free energy (δG) of the helix-coil transition at sites of ICLs. Depending on δG, DNA interstrand crosslinks at per nucleotide concentration r = 0.05 can change the melting temperature by value from -17 to +47°C, and the influence weakly depends on DNA sequence and GC content. A change in melting temperature caused by introduction of interstrand crosslinking in modified DNA at sites of modifications also depends on δG and varies from 0 to +12°C. Comparison with experiment for the three platinum crosslinking compounds demonstrates utility of the theoretical method for understanding how crosslinking compounds can influence the melting behavior. On the basis of the method, interdependence of local distortions and crosslinking in itself was studied for thermal effect of ICLs. A method for evaluating the nature of the structural alteration that produces a change in thermal stability for short crosslinked DNA is also proposed. The methods can be used for comparative thermodynamic characterization of various DNA crosslinking agents.

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 τ 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 ≈ Tm (Tm 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 τ base pairs in length does not markedly change the DMC for τ < 150 bp. However, the same prohibition strongly affects the average length of internal melted regions for much smaller τ's. The effect is already noticeable for τ = 1 bp and increases with τ. A tenfold increase in the entropy factor of all loops with length less than τ bp causes a noticeable alteration of the DMC for τ ≥ 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. © 2001 John Wiley & Sons, Inc. Biopolymers 58: 374–389, 2001