2017
DOI: 10.1103/physrevlett.119.188103
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Nucleation of Multiple Buckled Structures in Intertwined DNA Double Helices

Abstract: We study the statistical-mechanical properties of intertwined double-helical DNAs (DNA braids). In magnetic tweezers experiments we find that torsionally-stressed stretched braids supercoil via an abrupt buckling transition, which is associated with nucleation of a braid end loop, and that the buckled braid is characterized by proliferation of multiple domains. The experimental results are in accord with the predictions of a statistical-mechanical model.

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Cited by 8 publications
(11 citation statements)
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“…[34]. DNA braids have the same geometry as plectonemes, however experimentally studied braids [4042] are force extended, while plectonemes are buckled structures that do not have force-extension energy [Appendix A].…”
Section: Supercoiled Defect-free Dnamentioning
confidence: 99%
“…[34]. DNA braids have the same geometry as plectonemes, however experimentally studied braids [4042] are force extended, while plectonemes are buckled structures that do not have force-extension energy [Appendix A].…”
Section: Supercoiled Defect-free Dnamentioning
confidence: 99%
“…[34]. DNA braids have the same geometry as plectonemes, however experimentally studied braids [40][41][42] are force extended, while plectonemes are buckled structures that do not have force-extension energy [Appendix A].…”
Section: Thermal Fluctuationsmentioning
confidence: 99%
“…On theoretical grounds it has been predicted that highly twisted braids should tend to form smaller plectonemic domains than supercoiled single DNAs due to the greater bulk (cross-sectional area) of braided DNAs [24]. Our experimental reports of the buckling dynamics of braid shave indirectly observed the effects of multiple small domains [31]. Future experiments using fluorescence visualization of braid supercoiling would be desirable to allow direct observation of the size and dynamics of braid-plectoneme domains.…”
mentioning
confidence: 69%
“…The torque increased with Ca until reached a plateau of ~58 pNꞏnm at Ca=52.For the widest intertether braid (d/L=0.54) held by an 8.03 pN force, the torque increased from 0 to a peak of 76 pNꞏnm when the catenation was increased from 0 to Ca=30 or =0.53(Figure 2d). At 2 pN force and Ca=20, the torques were 31, 21 and 15 pNꞏnm in braids of large (0.54 L), mid (0.31 L) and small (0.26 L) intertether distances, respectively(Figure 2b).Theoretical calculations generating the extension-catenation curves(Figures 3d and 4d)were carried out based on a statistical-mechanical model for braids (SeeSupplementary Material)[24,31]. The torques from the model(Figures 3e and 4e)were obtained from the derivative of the free energy as a function of catenation.…”
mentioning
confidence: 99%