Abstract
A computer modeling of thermodynamic properties of a long DNA of N base pairs that includes ω interstrand crosslinks (ICLs), or ω chemical modifications involving one strand (monofunctional adducts, intrastrand crosslinks) has been carried out. It is supposed in our calculation that both types of chemical modifications change the free energy of the helix-coil transition at sites of their location by δF. The value δF>0 corresponds to stabilization, i.e. to the increase in melting temperature. It is also taken into account that ICLs form additional loops in melted regions and prohibit strand dissociation after full DNA melting. It is shown that the main effect of interstrand crosslinks on the stability of long DNA's is caused by the formation of additional loops in melted regions. This formation increases DNA melting temperature (Tm ) much stronger than replacing co base pairs of AT type with GC. A prohibition of strand dissociation after crosslinking, which strongly elevates the melting temperature of oligonucleotide duplexes, does not influence melting behavior of long DNA's (N≥1000 bp). As was demonstrated earlier for the modifications involving one or the other strand, the dependence of the shift of melting temperature δTm on the relative number of modifications r = ω/(2N) is a linear function for any δF, and δTm(r) = 0 for the ideal modifications (δF=0). We have shown that δTm(r) is the same for periodical and random distribution if the absolute value of δF is less 2 kcal. The absolute value of δTm(r) at δF>2 kcal and δF<−2 kcal is higher for periodical distribution. For interstrand crosslinks, the character of the dependence δTm(r) is quite different. It is nonlinear, and the shape of the corresponding curve is strongly dependent on δF. For “ideal” interstrand crosslinks (δF=0), the function δTm(r) is not zero. It is monotone positive nonlinear, and its slope decreases with r. If r<0.004, then the entropy stabilizing effect of interstrand crosslinking itself exceeds the influence of a distortion of the double helix at sites of their location. The resulting δTm(r) is positive even in the case of the infinite destabilization at sites of the ICLs (δF→ −∞). In general, stabilizing influence of interstrand crosslinks is almost fully compensated for by local structural distortions caused by them if 0< r <0.01 and −∞<δ F ≲−5 kcal per mole of ICLs. The absolute value of δTm(r) in this case is ∼10 times lower than for ideal ICLs as well as for local destabilization without crosslinking. Interstrand crosslinks formed by cisplatin do not change the melting temperature of long DNA's because of this compensation effect.
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