Strongly Bent Double-Stranded DNA: Reconciling Theory and Experiment

The strong bending of polymers is poorly understood. We propose a general quantitative framework of polymer bending that includes both the weak and strong bending regimes on the same footing, based on a single general physical principle. As the bending deformation increases beyond a certain (polymer...

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Main Authors: Aleksander V. Drozdetski, Abhishek Mukhopadhyay, Alexey V. Onufriev
Format: Article
Language:English
Published: Frontiers Media S.A. 2019-11-01
Series:Frontiers in Physics
Subjects:
DNA
Online Access:https://www.frontiersin.org/article/10.3389/fphy.2019.00195/full
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spelling doaj-0c4884fcb10c4edcaa594566ab3f39a92020-11-25T00:04:11ZengFrontiers Media S.A.Frontiers in Physics2296-424X2019-11-01710.3389/fphy.2019.00195481978Strongly Bent Double-Stranded DNA: Reconciling Theory and ExperimentAleksander V. Drozdetski0Abhishek Mukhopadhyay1Alexey V. Onufriev2Alexey V. Onufriev3Alexey V. Onufriev4Department of Physics, Virginia Tech, Blacksburg, VA, United StatesDepartment of Physics, Virginia Tech, Blacksburg, VA, United StatesDepartment of Physics, Virginia Tech, Blacksburg, VA, United StatesDepartment of Computer Science, Virginia Tech, Blacksburg, VA, United StatesCenter for Soft Matter and Biological Physics, Virginia Tech, Blacksburg, VA, United StatesThe strong bending of polymers is poorly understood. We propose a general quantitative framework of polymer bending that includes both the weak and strong bending regimes on the same footing, based on a single general physical principle. As the bending deformation increases beyond a certain (polymer-specific) point, the change in the convexity properties of the effective bending energy of the polymer makes the harmonic deformation energetically unfavorable: in this strong bending regime the energy of the polymer varies linearly with the average bending angle as the system follows the convex hull of the deformation energy function. For double-stranded DNA, the effective bending deformation energy becomes non-convex for bends greater than ~ 2° per base-pair, equivalent to the curvature of a closed circular loop of ~ 160 base pairs. A simple equation is derived for the polymer loop energy that covers both the weak and strong bending regimes. The theory shows quantitative agreement with recent DNA cyclization experiments on short DNA fragments, while maintaining the expected agreement with experiment in the weak bending regime. Counter-intuitively, cyclization probability (j-factor) of very short DNA loops is predicted to increase with decreasing loop length; the j-factor reaches its minimum for loops of ≃ 45 base pairs. Atomistic simulations reveal that the attractive component of the short-range Lennard-Jones interaction between the backbone atoms can explain the underlying non-convexity of the DNA effective bending energy, leading to the linear bending regime. Applicability of the theory to protein-DNA complexes, including the nucleosome, is discussed.https://www.frontiersin.org/article/10.3389/fphy.2019.00195/fullpolymer bendingDNAconvex hulldeformationcyclizationj-factor
collection DOAJ
language English
format Article
sources DOAJ
author Aleksander V. Drozdetski
Abhishek Mukhopadhyay
Alexey V. Onufriev
Alexey V. Onufriev
Alexey V. Onufriev
spellingShingle Aleksander V. Drozdetski
Abhishek Mukhopadhyay
Alexey V. Onufriev
Alexey V. Onufriev
Alexey V. Onufriev
Strongly Bent Double-Stranded DNA: Reconciling Theory and Experiment
Frontiers in Physics
polymer bending
DNA
convex hull
deformation
cyclization
j-factor
author_facet Aleksander V. Drozdetski
Abhishek Mukhopadhyay
Alexey V. Onufriev
Alexey V. Onufriev
Alexey V. Onufriev
author_sort Aleksander V. Drozdetski
title Strongly Bent Double-Stranded DNA: Reconciling Theory and Experiment
title_short Strongly Bent Double-Stranded DNA: Reconciling Theory and Experiment
title_full Strongly Bent Double-Stranded DNA: Reconciling Theory and Experiment
title_fullStr Strongly Bent Double-Stranded DNA: Reconciling Theory and Experiment
title_full_unstemmed Strongly Bent Double-Stranded DNA: Reconciling Theory and Experiment
title_sort strongly bent double-stranded dna: reconciling theory and experiment
publisher Frontiers Media S.A.
series Frontiers in Physics
issn 2296-424X
publishDate 2019-11-01
description The strong bending of polymers is poorly understood. We propose a general quantitative framework of polymer bending that includes both the weak and strong bending regimes on the same footing, based on a single general physical principle. As the bending deformation increases beyond a certain (polymer-specific) point, the change in the convexity properties of the effective bending energy of the polymer makes the harmonic deformation energetically unfavorable: in this strong bending regime the energy of the polymer varies linearly with the average bending angle as the system follows the convex hull of the deformation energy function. For double-stranded DNA, the effective bending deformation energy becomes non-convex for bends greater than ~ 2° per base-pair, equivalent to the curvature of a closed circular loop of ~ 160 base pairs. A simple equation is derived for the polymer loop energy that covers both the weak and strong bending regimes. The theory shows quantitative agreement with recent DNA cyclization experiments on short DNA fragments, while maintaining the expected agreement with experiment in the weak bending regime. Counter-intuitively, cyclization probability (j-factor) of very short DNA loops is predicted to increase with decreasing loop length; the j-factor reaches its minimum for loops of ≃ 45 base pairs. Atomistic simulations reveal that the attractive component of the short-range Lennard-Jones interaction between the backbone atoms can explain the underlying non-convexity of the DNA effective bending energy, leading to the linear bending regime. Applicability of the theory to protein-DNA complexes, including the nucleosome, is discussed.
topic polymer bending
DNA
convex hull
deformation
cyclization
j-factor
url https://www.frontiersin.org/article/10.3389/fphy.2019.00195/full
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