We analyze whether the "overstretched," or "S" form of double-stranded DNA consists of essentially separated, or essentially interacting, polynucleotide strands. Comparison of force-extension data for S-DNA and single-stranded DNA shows S-DNA to be distinct from both double helix and single-stranded forms. We use a simple thermodynamical model for tension-melted double-stranded DNA, which indicates that the overstretching transition near 65 piconewtons cannot be explained in terms of conversion of double helix to noninteracting polynucleotide strands. However, the single-strand-like response observed in some experiments can be explained in terms of "unpeeling" of large regions of one strand, starting from nicks on the original double helix. We show that S-DNA becomes unstable to unpeeling at large forces, and that at low ionic strength, or for weakly base-paired sequences, unpeeling can preempt formation of S-DNA. We also analyze the kinetics of unpeeling including the effect of sequence-generated free energy inhomogeneity. We find that strongly base-paired regions generate large barriers that stabilize DNA against unpeeling. For long genomic sequences, these barriers to unpeeling cannot be kinetically crossed until force exceeds approximately 150 piconewtons.
Most genetic regulatory mechanisms involve protein-DNA interactions. In these processes, the classical Watson-Crick DNA structure sometimes is distorted severely, which in turn enables the precise recognition of the specific sites by the protein. Despite its key importance, very little is known about such deformation processes. To address this general question, we have studied a model system, namely, RecA binding to double-stranded DNA. Results from micromanipulation experiments indicate that RecA binds strongly to stretched DNA; based on this observation, we propose that spontaneous thermal stretching f luctuations may play a role in the binding of RecA to DNA. This has fundamental implications for the protein-DNA binding mechanism, which must therefore rely in part on a combination of f lexibility and thermal f luctuations of the DNA structure. We also show that this mechanism is sequence sensitive. Theoretical simulations support this interpretation of our experimental results, and it is argued that this is of broad relevance to DNA-protein interactions.
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