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Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel
We measure the thermal fluctuation of the internal segments of a piece of DNA confined in a nanochannel about 50[Image: see text]100 nm wide. This local thermodynamic property is key to accurate measurement of distances in genomic analysis. For DNA in [Image: see text]100 nm channels, we observe a c...
Autores principales: | , , , |
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Formato: | Texto |
Lenguaje: | English |
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Public Library of Science
2011
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3057976/ https://www.ncbi.nlm.nih.gov/pubmed/21423606 http://dx.doi.org/10.1371/journal.pone.0016890 |
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author | Su, Tianxiang Das, Somes K. Xiao, Ming Purohit, Prashant K. |
author_facet | Su, Tianxiang Das, Somes K. Xiao, Ming Purohit, Prashant K. |
author_sort | Su, Tianxiang |
collection | PubMed |
description | We measure the thermal fluctuation of the internal segments of a piece of DNA confined in a nanochannel about 50[Image: see text]100 nm wide. This local thermodynamic property is key to accurate measurement of distances in genomic analysis. For DNA in [Image: see text]100 nm channels, we observe a critical length scale [Image: see text]10 [Image: see text]m for the mean extension of internal segments, below which the de Gennes' theory describes the fluctuations with no fitting parameters, and above which the fluctuation data falls into Odijk's deflection theory regime. By analyzing the probability distributions of the extensions of the internal segments, we infer that folded structures of length 150[Image: see text]250 nm, separated by [Image: see text]10 [Image: see text]m exist in the confined DNA during the transition between the two regimes. For [Image: see text]50 nm channels we find that the fluctuation is significantly reduced since the Odijk regime appears earlier. This is critical for genomic analysis. We further propose a more detailed theory based on small fluctuations and incorporating the effects of confinement to explicitly calculate the statistical properties of the internal fluctuations. Our theory is applicable to polymers with heterogeneous mechanical properties confined in non-uniform channels. We show that existing theories for the end-to-end extension/fluctuation of polymers can be used to study the internal fluctuations only when the contour length of the polymer is many times larger than its persistence length. Finally, our results suggest that introducing nicks in the DNA will not change its fluctuation behavior when the nick density is below 1 nick per kbp DNA. |
format | Text |
id | pubmed-3057976 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2011 |
publisher | Public Library of Science |
record_format | MEDLINE/PubMed |
spelling | pubmed-30579762011-03-21 Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel Su, Tianxiang Das, Somes K. Xiao, Ming Purohit, Prashant K. PLoS One Research Article We measure the thermal fluctuation of the internal segments of a piece of DNA confined in a nanochannel about 50[Image: see text]100 nm wide. This local thermodynamic property is key to accurate measurement of distances in genomic analysis. For DNA in [Image: see text]100 nm channels, we observe a critical length scale [Image: see text]10 [Image: see text]m for the mean extension of internal segments, below which the de Gennes' theory describes the fluctuations with no fitting parameters, and above which the fluctuation data falls into Odijk's deflection theory regime. By analyzing the probability distributions of the extensions of the internal segments, we infer that folded structures of length 150[Image: see text]250 nm, separated by [Image: see text]10 [Image: see text]m exist in the confined DNA during the transition between the two regimes. For [Image: see text]50 nm channels we find that the fluctuation is significantly reduced since the Odijk regime appears earlier. This is critical for genomic analysis. We further propose a more detailed theory based on small fluctuations and incorporating the effects of confinement to explicitly calculate the statistical properties of the internal fluctuations. Our theory is applicable to polymers with heterogeneous mechanical properties confined in non-uniform channels. We show that existing theories for the end-to-end extension/fluctuation of polymers can be used to study the internal fluctuations only when the contour length of the polymer is many times larger than its persistence length. Finally, our results suggest that introducing nicks in the DNA will not change its fluctuation behavior when the nick density is below 1 nick per kbp DNA. Public Library of Science 2011-03-15 /pmc/articles/PMC3057976/ /pubmed/21423606 http://dx.doi.org/10.1371/journal.pone.0016890 Text en Su et al. http://creativecommons.org/licenses/by/4.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are properly credited. |
spellingShingle | Research Article Su, Tianxiang Das, Somes K. Xiao, Ming Purohit, Prashant K. Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel |
title | Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel |
title_full | Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel |
title_fullStr | Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel |
title_full_unstemmed | Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel |
title_short | Transition between Two Regimes Describing Internal Fluctuation of DNA in a Nanochannel |
title_sort | transition between two regimes describing internal fluctuation of dna in a nanochannel |
topic | Research Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3057976/ https://www.ncbi.nlm.nih.gov/pubmed/21423606 http://dx.doi.org/10.1371/journal.pone.0016890 |
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