Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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