Melting of crosslinked DNA: VI. Comparison of influence of interstrand crosslinks and other chemical modifications formed by antitumor compounds on DNA stability.

A computer modeling of thermodynamic properties of a long DNA of N base pairs that includes omega interstrand crosslinks (ICLs), or omega 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 deltaF. The value deltaF>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 omega 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>or=1000 bp). As was demonstrated earlier for the modifications involving one or the other strand, the dependence of the shift of melting temperature deltaTm on the relative number of modifications r=omega/(2N) is a linear function for any deltaF, and deltaTm(r) identical with 0 for the ideal modifications (deltaF=0). We have shown that deltaTm(r) is the same for periodical and random distribution if the absolute value of deltaF is less 2 kcal. The absolute value of deltaTm(r) at deltaF>2 kcal and deltaF<-2 kcal is higher for periodical distribution. For interstrand crosslinks, the character of the dependence deltaTm(r) is quite different. It is nonlinear, and the shape of the corresponding curve is strongly dependent on deltaF. For "ideal" interstrand crosslinks (deltaF=0), the function deltaTm(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 deltaTm(r) is positive even in the case of the infinite destabilization at sites of the ICLs (deltaF-->-infinity). In general, stabilizing influence of interstrand crosslinks is almost fully compensated for by local structural distortions caused by them if 0

The HMG1 ta(i)le.

We have studied structural changes in DNA/protein complexes using the CD spectroscopy, upon the interaction of HMG1-domains with calf thymus DNA at different ionic strengths. HMG1 protein isolated from calf thymus and recombinant HMG1-(A+B) protein were used. Recombinant protein HMG1-(A+B) represents a rat HMG1 lacking C-terminal acidic tail. At low ionic strength (15 mM NaCl) we observed similar behavior of both proteins upon interaction with DNA. Despite this, at higher ionic strength (150 mM NaCl) their interaction with DNA leads to a completely different structure of the complexes. In the case of HMG1-(A+B)/DNA complexes we observed the appearance of DNA fractions possessing very high optical activity. This could be a result of formation of the highly-ordered DNA structures modulated by the interaction with HMG1-domains. Thus the comparison studies of HMG1 and HMG1-(A+B) interaction with DNA show that negatively charged C-terminal tail of HMG1 modulates interaction of the protein with DNA. The striking difference of the behaviour of these two systems allows us to explain the functional role of multiple HMG1 domains in some regulatory and architectural proteins.