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Plenarvorträge - DPG-Tagungen

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Arbeitskreis Biologische Physik Freitag<br />

AKB 50.41 Fr 10:30 B<br />

Overdamped Buckling Dynamics — •Oskar Hallatschek 1 , Erwin<br />

Frey 1,2 , and Klaus Kroy 1 — 1 Abteilung Theorie, Hahn-Meitner<br />

Institut, Glienicker Str. 100, 14109 Berlin, Germany — 2 Fachbereich<br />

Physik, Freie Universität,14195 Berlin, Germany<br />

We discuss the generic relaxation dynamics of a weakly bending incompressible<br />

rod in a viscous environment. We show that the decay of the<br />

initially imposed transverse undulations creates two expanding boundary<br />

layers that grow at the cost of a longitudinally inert bulk. In the bulk,<br />

longitudinal expansion is completely suppressed by the viscous friction<br />

on the boundary regions. We have calculated tension profiles based on<br />

coarse grained equations of motion for the position dependent tension,<br />

from which all other relevant observables can be calculated. We find that<br />

the different scenarios of tension release can conveniently be classified<br />

in terms of a roughness exponent β as a measure for the type of initial<br />

excitation.<br />

AKB 50.42 Fr 10:30 B<br />

Linear response of a grafted semiflexible polymer to a uniform<br />

field — •Panayotis Benetatos 1 and Erwin Frey 1,2 — 1 Hahn-<br />

Meitner-Institut, Abteilung Theorie, Berlin — 2 Fachbereich Physik, Freie<br />

Universitaet, Berlin<br />

We study the linear response of a semiflexible polymer to a uniform<br />

force field. We use the worm-like chain model and we consider a polymer<br />

which has one end grafted and the other free. In contrast to a force<br />

applied at the free end, the field introduces a nonlocal interaction along<br />

the polymer contour. Because of this nonlocality, using the free chain<br />

propagator (two-point orientational probability density) for the calculation<br />

of the linear response of the polymer extension in the direction of<br />

the field fails. We can apply the propagator method, however, in order to<br />

calculate the linear response of the end-point tangent vector orientation<br />

where locality is restored. We then use this result and make an Ansatz<br />

to obtain the linear response of the extension. Our analytic results are<br />

functions of the total contour length, the persistence length, and the orientation<br />

of the field. We discuss how the response to a field differs from<br />

that to a force.<br />

AKB 50.43 Fr 10:30 B<br />

Depinning of weakly bending semiflexible polymers —<br />

•Panayotis Benetatos 1 and Erwin Frey 1,2 — 1 Hahn-Meitner-<br />

Institut, Abteilung Theorie, Berlin — 2 Fachbereich Physik, Freie<br />

Universitaet, Berlin<br />

We present a simple theoretical model for the thermal depinning of a<br />

weakly bending semiflexible polymer in 1+1 dimensions. We consider a<br />

discrete sequence of pinning sites along the polymer contour. Each pinning<br />

site is characterized by a binding energy, a transverse width, and<br />

an angular width. We use the necklace model of phase transitions in<br />

quasi-one-dimensional systems and we obtain a phase transition in the<br />

thermodynamic limit where the density of pinning sites goes to infinity<br />

and the widths of a pinning site go to zero. This novel way to take<br />

the thermodynamic limit is consistent with the weakly bending approximation<br />

which is valid when the total contour length of the polymer is<br />

smaller than its persistence length. We also consider the depinning in<br />

1+d dimensions.<br />

AKB 50.44 Fr 10:30 B<br />

Random walks of molecular motors — •Stefan Klumpp 1 ,<br />

Theo M. Nieuwenhuizen 1,2 , and Reinhard Lipowsky 1 —<br />

1 Max-Planck-Institut für Kolloid- und Grenzflächenforschung, 14424<br />

Potsdam — 2 Instituut voor Theoretische Fysica, Valckenierstraat 65,<br />

1018 XE Amsterdam<br />

Processive molecular motors perform directed walks along cytoskeletal<br />

filaments. Upon unbinding from the filaments, they undergo non-directed<br />

Brownian motion until they rebind to the same or another filament. The<br />

random walks that result from the interplay of bound and unbound motors<br />

movements are studied theoretically. These random walks exhibit<br />

anomalous drift behaviour in open compartments and stationary concentration<br />

profiles characterized by a balance of bound and unbound motor<br />

currents in closed compartments [1]. Mutual exclusion of motors from<br />

the binding sites of the filaments leads to traffic jams and a maximal<br />

motor current at an intermediate motor concentration. These transport<br />

phenomena mimic transport phenomena in cells and are accessible to in<br />

vitro experiments.<br />

[1] R. Lipowsky, S. Klumpp, and T. M. Nieuwenhuizen,<br />

Phys. Rev. Lett. 87, 108101 (2001).<br />

AKB 50.45 Fr 10:30 B<br />

Gating charge effects for nerve excitation — •Gerhard Schmid,<br />

Igor Goychuk, and Peter Hänggi — Institut für Physik, Universität<br />

Augsburg<br />

Voltage dependent ion channels mainly determine the electric properties<br />

of axonal cell membranes. The ion channels thereby do not only allow<br />

passage of ions trough the cell membrane, but they also contribute to the<br />

membrane capacity, since the switching of the channel gates between an<br />

open and a closed configuration is always connected with movement of<br />

charge within the cell membrane. Especially, in case of moderately large<br />

densities of ion channels, which are found, for example, in the nodes of<br />

Ranvier, this may play a crucial role for nerve excitation. Our model system<br />

is a modified Hodgkin-Huxley model which takes into account the<br />

change in the membrane capacity. Additional terms, which are proportional<br />

to the number of ion channels resp. the number of gates, extend the<br />

original Hodgkin-Huxley model and allow the consideration of a – due<br />

to the gating charges – time-dependent membrane capacity. Surprisingly,<br />

the gating charge do not dramatically change the excitation behavior<br />

even for extreme dense ion channel assemblies, instead, the membrane<br />

capacity at rest exhibits a bell-shaped dependence on the ion channel<br />

density. This work is supported by DFG (SFB 486).<br />

AKB 50.46 Fr 10:30 B<br />

Membrane mechanics and polymer decoration — •Thorsten<br />

Auth and Gerhard Gompper — Institut für Festkörperforschung,<br />

Forschungszentrum Jülich, 52425 Jülich<br />

Polymers embedded into or attached to lipid bilayer membranes modify<br />

the membrane’s mechanical properties. A prominent example of a<br />

polymer-membrane system is the red blood cell [1]. The lipid bilayer<br />

membrane can be modeled by a mathematical surface and a set of material<br />

constants: bending rigidity, saddle-splay modulus, spontaneous curvature.<br />

In many cases the effect of attached, adsorbed or free polymers<br />

can be described by effective curvature elastic constants (see e. g. [2]).<br />

The excluded-volume interaction is well known to strongly affect the<br />

scaling behaviour of polymer chains. We have therefore developed a<br />

Monte Carlo simulation method to investigate the effects of self-avoidance<br />

and different polymer architectures on the curvature elastic constants for<br />

low polymer coverage [3]. The method will be introduced, results for the<br />

effective curvature constants will be presented and discussed together<br />

with implications on the behaviour of membrane systems.<br />

[1] N. Gov, A. G. Zilman and S. Safran; Phys. Rev. Lett. 90, 228101<br />

(2003)<br />

[2] C. Hiergeist and R. Lipowsky; J. Phys. II (France) 6, 1465 (1996)<br />

[3] T. Auth and G. Gompper; Phys. Rev. E 68, 051801 (2003)<br />

AKB 50.47 Fr 10:30 B<br />

Elastic and caloric properties of model membranes at the chain<br />

melting transition — •Wolfgang Manglkammer and Jan K.<br />

Krüger — Universität des Saarlandes, Experimentalphysik, Postfach<br />

151150, D-66041 Saarbrücken, GERMANY<br />

One remarkable feature of lipid membranes, which often serve as a<br />

model for ’real’ biological membranes, is the so-called main transition,<br />

but its nature is not yet clear. When the hydrocarbon chains are melting,<br />

the lipid bilayer transforms from the gel phase into the fluid Lα phase.<br />

We investigated the hypersonic properties of oriented, solid supported<br />

Phosphatidylcholine bilayer stacks of different chain length by Brillouin<br />

spectroscopy as a function of hydration and temperature. The elastic<br />

moduli show huge steps which accompany several phase transitions.<br />

Therefore the transition points can easily be defined, what allows us<br />

to draw a temperature-composition phase diagram.<br />

The elastic behaviour near the main transition is related to the specific<br />

heat as obtained from multi-lamellar vesicles by quasi-isothermal Temperature<br />

Modulated DSC. The heat capacity shows critical behaviour on<br />

both sides of the transition. Such pre-critical features were not found<br />

for the high frequency elastic moduli, although they were reported in<br />

literature for low frequency elastic experiments.<br />

AKB 50.48 Fr 10:30 B<br />

Vesicle adhesion and cohesion at finite temperature — •Thomas<br />

Gruhn and Reinhard Lipowsky — MPI for Colloids and Interfaces<br />

14424 Potsdam<br />

Biological cells are the fundamental building blocks of living organisms.<br />

They are surrounded by a closed membrane surface that serves as<br />

an interface to the outside world. In many cases cells act very similar

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