24 research outputs found

    The Tension on dsDNA Bound to ssDNA/RecA Filaments May Play an Important Role in Driving Efficient and Accurate Homology Recognition and Strand Exchange

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    It is well known that during homology recognition and strand exchange the double stranded DNA (dsDNA) in DNA/RecA filaments is highly extended, but the functional role of the extension has been unclear. We present an analytical model that calculates the distribution of tension in the extended dsDNA during strand exchange. The model suggests that the binding of additional dsDNA base pairs to the DNA/RecA filament alters the tension in dsDNA that was already bound to the filament, resulting in a non-linear increase in the mechanical energy as a function of the number of bound base pairs. This collective mechanical response may promote homology stringency and underlie unexplained experimental results

    RecA homology search is promoted by mechanical stress along the scanned duplex DNA

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    A RecA–single-stranded DNA (RecA–ssDNA) filament searches a genome for sequence homology by rapidly binding and unbinding double-stranded DNA (dsDNA) until homology is found. We demonstrate that pulling on the opposite termini (3′ and 5′) of one of the two DNA strands in a dsDNA molecule stabilizes the normally unstable binding of that dsDNA to non-homologous RecA–ssDNA filaments, whereas pulling on the two 3′, the two 5′, or all four termini does not. We propose that the ‘outgoing’ strand in the dsDNA is extended by strong DNA–protein contacts, whereas the ‘complementary’ strand is extended by the tension on the base pairs that connect the ‘complementary’ strand to the ‘outgoing’ strand. The stress resulting from different levels of tension on its constitutive strands causes rapid dsDNA unbinding unless sufficient homology is present

    ΔT<sub>m</sub> as a function of the position of single mismatches.

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    <p>The sequence is shown at the top of the figure The single base pair mismatch replacements are shown below in colors corresponding to the colors of the curves shown in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0130875#pone.0130875.g001" target="_blank">Fig 1D and 1E</a>. The cyan, black, and purple lines and symbols correspond to the systems shown in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0130875#pone.0130875.g001" target="_blank">Fig 1i, ii, and iii</a>, respectively. The solid triangles represent the L data. The hollow circles correspond to the R data. The solid lines connect the data points from R measurements, except for the T<sub><b>m</b></sub> mismatch at position 30, which is derived from the L data. The arrows on the right (left) side of the graph indicate T<sub><b>m</b></sub> values calculated from R (L) measurements for a mismatch at position 30(8). For the undivided probe, the fluorophore pair nearest the mismatch separates at a significantly lower temperature than the true T<sub><b>m</b></sub>, but for the divided probe the ends melt at the true T<sub><b>m</b></sub>.</p
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