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Polymers in Confined Geometry.pdf

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Chapter 3<br />

<strong>Polymers</strong> <strong>in</strong> conf<strong>in</strong>ed geometry<br />

In this chapter we are go<strong>in</strong>g to <strong>in</strong>vestigate the conformational behavior of polymer<br />

cha<strong>in</strong>s <strong>in</strong> a conf<strong>in</strong><strong>in</strong>g geometry. First a short experimental motivation is given,<br />

after which heuristic scal<strong>in</strong>g relations are derived. This is followed by a more<br />

detailed analytical calculation, start<strong>in</strong>g from the limit of stiff cha<strong>in</strong>s <strong>in</strong> the weaklybend<strong>in</strong>g<br />

rod approximation. In particular we <strong>in</strong>vestigate the cyl<strong>in</strong>drical harmonic<br />

potential as a generic model for conf<strong>in</strong><strong>in</strong>g environments with similar a symmetry.<br />

3.1 Motivation<br />

The <strong>in</strong>terest <strong>in</strong> conf<strong>in</strong>ement of polymers <strong>in</strong>to nano-sized structures emerges ma<strong>in</strong>ly<br />

from biotechnology. As discussed <strong>in</strong> the <strong>in</strong>troduction, there are various applications<br />

encourag<strong>in</strong>g our work on the problem of conf<strong>in</strong>ement.<br />

One direct application is that of conf<strong>in</strong>ement elongation. The advantage is<br />

that upon conf<strong>in</strong><strong>in</strong>g the cha<strong>in</strong> stretches already <strong>in</strong> its equilibrium conformation.<br />

There is no need of a stretch<strong>in</strong>g flow or elongat<strong>in</strong>g external force, which drives the<br />

polymer out of its static conformation <strong>in</strong>to a stretched non-equilibrium conformation.<br />

Here we can try to understand the mechanisms lead<strong>in</strong>g from the unconf<strong>in</strong>ed<br />

to the conf<strong>in</strong>ed static equilibrium conformation.<br />

An application with a large potential impact is the determ<strong>in</strong>ation of the<br />

contour-length L of a polymer by measur<strong>in</strong>g its equilibrium apparent end-toend<br />

distance <strong>in</strong> an conf<strong>in</strong><strong>in</strong>g tube of the order of the persistence length or less.<br />

Up to now gel-electrophoresis is the tool for this sort of measurements, but it has<br />

its problems. It is slow—a measurement takes <strong>in</strong> the order of a day—and it is<br />

relatively imprecise. The advantage of the idea of the conf<strong>in</strong>ement measurement<br />

seems therefore a faster way to obta<strong>in</strong> the data. It is a matter of m<strong>in</strong>utes to<br />

do the actual measurement and it is <strong>in</strong> pr<strong>in</strong>ciple possible to make the results<br />

arbitrarily accurate, by just tak<strong>in</strong>g more pictures of equilibrium configurations.<br />

The basic experiments are performed <strong>in</strong> nano-sized channels with a near<br />

square geometry <strong>in</strong> the group of Bob Aust<strong>in</strong> [38, 44]. They have succeeded<br />

21

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