2010
DOI: 10.1103/physreve.82.041801
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Fluctuations of a long, semiflexible polymer in a narrow channel

Abstract: We consider an inextensible, semiflexible polymer or wormlike chain, with persistence length P and contour length L, fluctuating in a cylindrical channel of diameter D. In the regime D Ӷ P Ӷ L, corresponding to a long, tightly confined polymer, the average length of the channel ͗R ʈ ͘ occupied by the polymer and the mean-square deviation from the average vary as ͗R ʈ ͘ = ͓1−␣ ‫ؠ‬ ͑D / P͒ 2/3 ͔L and ͗⌬R ʈ 2 ͘ = ␤ ‫ؠ‬ ͑D 2 / P͒L, respectively, where ␣ ‫ؠ‬ and ␤ ‫ؠ‬ are dimensionless amplitudes. In earlier work w… Show more

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Cited by 75 publications
(142 citation statements)
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“…The variance exhibits linear behavior over the central portion of the plot, consistent with the polymer models for confinement. 16,32,35 There is some deviation at the smaller molecular weights, which we can attribute to the difficulty in accurately measuring small distances between labels and the systematic error introduced by 250 bp bins for small molecular weights, and scatter at higher molecular weights, which arises from the sampling error (even after binning the data). It is possible that the deviation from linearity at smaller distances is physically relevant, since simulations clearly indicate that the asymptotic scaling for the variance in extension is not achieved until the chain is long enough, of the order of 185 kbp, and that the variance increases sub-linearly with molecular weight for small molecular weights.…”
Section: Resultsmentioning
confidence: 99%
“…The variance exhibits linear behavior over the central portion of the plot, consistent with the polymer models for confinement. 16,32,35 There is some deviation at the smaller molecular weights, which we can attribute to the difficulty in accurately measuring small distances between labels and the systematic error introduced by 250 bp bins for small molecular weights, and scatter at higher molecular weights, which arises from the sampling error (even after binning the data). It is possible that the deviation from linearity at smaller distances is physically relevant, since simulations clearly indicate that the asymptotic scaling for the variance in extension is not achieved until the chain is long enough, of the order of 185 kbp, and that the variance increases sub-linearly with molecular weight for small molecular weights.…”
Section: Resultsmentioning
confidence: 99%
“…Although there are challenges in using DNA beyond those discussed here, for example the inability to tune the system so that different confinement regimes span multiple decades in channel size [39,74], DNA remains the most convenient model system for studying confined polymers. While it may ultimately prove challenging to use DNA to test the existing models down to the prefactors for the scaling laws [23,25,[41][42][43], there is no better experimental system to directly visualize the effects of confinement at the single molecule level and investigate the universal properties of confined polymers at the scaling level.…”
Section: Discussionmentioning
confidence: 99%
“…In some cases, the prefactors for the scaling laws are known exactly [41][42][43]. These thermodynamic quantities depend on the contour length L of the polymer, its persistence length l p , the effective width w of the polymer backbone, and the channel size D. The persistence length and effective width of DNA, which are affected by the relative amount of screening of electrostatics by the ionic environment, can be obtained from polyelectrolyte theory [44][45][46][47], albeit with some uncertainty arising from the effect of the intercalating dye [48][49][50][51][52][53][54].…”
Section: Introductionmentioning
confidence: 99%
“…[34] As in the extended de Gennes regime, circular DNA in the Odijk regime can be treated as two strands going in opposite directions.…”
Section: Theory For the Odijk Regimementioning
confidence: 99%