Abstract

DNA cyclization is a powerful technique to gain insight into the nature of DNA bending. While the wormlike chain model provides a good description of small to moderate bending fluctuations, it is expected to break down for large bending. Recent cyclization experiments on strongly bent shorter molecules indeed suggest enhanced flexibility over and above that expected from the wormlike chain. Here, we use a coarse-grained model of DNA to investigate the subtle thermodynamics of DNA cyclization for molecules ranging from 30 to 210 base pairs. As the molecules get shorter, we find increasing deviations between our computed equilibrium j-factor and the classic wormlike chain predictions of Shimada and Yamakawa for a torsionally aligned looped molecule. These deviations are due to sharp kinking, first at nicks, and only subsequently in the body of the duplex. At the shortest lengths, substantial fraying at the ends of duplex domains is the dominant method of relaxation. We also estimate the dynamic j-factor measured in recent FRET experiments. We find that the dynamic j-factor is systematically larger than its equilibrium counterpart—with the deviation larger for shorter molecules—because not all the stress present in the fully cyclized state is present in the transition state. These observations are important for the interpretation of recent cyclization experiments, suggesting that measured anomalously high j-factors may not necessarily indicate non-WLC behavior in the body of duplexes.

Highlights

  • The mechanics of DNA plays an important role in its biological capacities: looping in the Lac operon regulates gene expression;[1] DNA supercoiling is part of the circadian cycle in cyanobacteria;[2] and the dynamically variable wrapping of DNA around histone proteins.[3]

  • We show jeoqxDNA values, calculated from our measured values of Kecyqc and Kedqim using eq 1, for 81 different lengths in the range Nbp = 30−207 for fixed Ns = 10 using the average-base parametrization of oxDNA. These results are compared to jeWqLC predictions based on the Shimada and Yamakawa (SY) expression[60] using previously calculated values for the relevant structural and mechanical properties of oxDNA.[29]

  • Cyclization is a system-dependent manifestation of the general thermodynamics of strong DNA bending.[26]

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Summary

Introduction

The mechanics of DNA plays an important role in its biological capacities: looping in the Lac operon regulates gene expression;[1] DNA supercoiling is part of the circadian cycle in cyanobacteria;[2] and the dynamically variable wrapping of DNA around histone proteins.[3]. The wormlike chain (WLC) model provides a good description of small-to-moderate bending fluctuations in DNA.[6−9] there is a consensus that for sufficiently strong bending the stress will be localized within small regions, often termed “kinks”, much about this crossover to non-WLC behavior remains controversial. A recent review by Vologodskii et al.[10] highlighted a number of open questions, including what is the free energy cost of kink formation, how does the free-energy of a kink depend on bend angle, what is the critical curvature that causes the double helix

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