Anomalous scaling in nanopore translocation of structured heteropolymers

Author

Malcolm McCauley 1, Robert Forties 1, Ulrich Gerland 2 and Ralf Bundschuh 3

Affiliations

1 Department of Physics, The Ohio State University, 191 West Woodruff Avenue, Columbus, OH 43210-1117, USA
2 Arnold-Sommerfeld Center for Theoretical Physics and Center for Nanoscience (CeNS), LMU München, Theresienstrasse 37, 80333 München, Germany
3 Departments of Physics and Biochemistry and Center for RNA Biology, The Ohio State University, 191 West Woodruff Avenue, Columbus, OH 43210-1117, USA

E-mail

gerland@lmu.de bundschuh@mps.ohio-state.edu

Journal

Physical Biology Create an alert RSS this journal

Issue

Volume 6, Number 3

Citation

Malcolm McCauley et al 2009 Phys. Biol. 6 036006

doi: 10.1088/1478-3975/6/3/036006


 
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Abstract

Translocation through nanopores has emerged as a new experimental technique to probe the physical properties of biomolecules. The question of how the typical translocation time for a single unstructured polymer depends on its length has already triggered many theoretical and computational studies. Here, we address the same question, but for structured RNA molecules where the breaking of base-pairing patterns is the main barrier for translocation. Within a simple model, we calculate the typical time for single-stranded RNAs with random sequences to translocate through an idealized nanopore. It is believed that with respect to secondary structure formation, such a random RNA is typically either frozen into a single dominant structure (glassy phase) or many different structures with similar total energies coexist (molten phase), depending on the temperature and the base-pairing energetics. We find that these two phases can be clearly distinguished by their translocation behavior in the absence of an external voltage bias. In both cases, the typical translocation time depends on the sequence length as a power law with an exponent that exceeds the naively expected exponent of two for purely diffusive translocation. However, whereas in the molten phase the exponent is constant, at a value of 5/2, the exponent increases rapidly with decreasing temperature in the glassy phase. We explain the behavior in the molten phase and the qualitative trend in the glassy phase theoretically.

 
PACS

87.85.Qr Nanotechnologies-design

87.15.B- Structure of biomolecules

87.14.G- Nucleic acids

36.20.Fz Constitution (chains and sequences)

87.15.Cc Folding: thermodynamics, statistical mechanics, models, and pathways

Subjects

Soft matter, liquids and polymers

Atomic and molecular physics

Biological physics

Dates

Issue 3 ( 1 September 2009)

Received 21 January 2009 , accepted for publication 1 April 2009

Published 1 May 2009

 
Image from Anomalous scaling in nanopore translocation of structured heteropolymers


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