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000041514 0247_ $$2DOI$$a10.1103/PhysRevE.70.051804
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000041514 084__ $$2WoS$$aPhysics, Fluids & Plasmas
000041514 084__ $$2WoS$$aPhysics, Mathematical
000041514 1001_ $$0P:(DE-HGF)0$$aLamura, A.$$b0
000041514 245__ $$aHelical polymer in cylindrical confining geometries
000041514 260__ $$aCollege Park, Md.$$bAPS$$c2004
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000041514 440_0 $$04924$$aPhysical Review E$$v70$$x1539-3755
000041514 500__ $$aRecord converted from VDB: 12.11.2012
000041514 520__ $$aUsing an algorithm for simulating equilibrium configurations, we study a fluctuating helical polymer either (i) contained in a cylindrical pore or (ii) wound around a cylindrical rod. We work in the regime where both the contour length and the persistence length of the helical polymer are much larger than the diameter of the cylinder. In case (i) we calculate the free energy of confinement and interpret it in terms of a wormlike chain in a pore with an effective diameter that depends on the parameters of the helix. In case (ii) we consider the possibility that one end of the helical polymer escapes from the rod and wanders away. The average numbers of turns at which the helix escapes or intersects the rod are measured in the simulations, as a function of the pitch p(o). The behavior for large and small p(o) is explained with simple scaling arguments.
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000041514 7001_ $$0P:(DE-HGF)0$$aBurkhardt, T. W.$$b1
000041514 7001_ $$0P:(DE-Juel1)130665$$aGompper, G.$$b2$$uFZJ
000041514 77318 $$2Crossref$$3journal-article$$a10.1103/physreve.70.051804$$bAmerican Physical Society (APS)$$d2004-11-18$$n5$$p051804$$tPhysical Review E$$v70$$x1539-3755$$y2004
000041514 773__ $$0PERI:(DE-600)2844562-4$$a10.1103/PhysRevE.70.051804$$gVol. 70, p. 051804$$n5$$p051804$$q70<051804$$tPhysical review / E$$v70$$x1539-3755$$y2004
000041514 8567_ $$uhttp://hdl.handle.net/2128/1508$$uhttp://dx.doi.org/10.1103/PhysRevE.70.051804
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000041514 999C5 $$1P.-G. de Gennes$$2Crossref$$9-- missing cx lookup --$$a10.1063/1.2914118$$y1979
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