72 research outputs found
Influence of fluctuations in actin structure on myosin V step size
We study the influence of disorder in the helical actin structure on the
myosin V step size, predicted from the elastic lever arm model. We show that
fluctuations of +-5 degrees per actin subunit, as proposed by Egelman et al.,
significantly alter the distribution of step sizes and improve the agreement
with experimental data.Comment: 5 pages, 4 figures, to appear in J. Chem. Inf. Mode
The binding dynamics of tropomyosin on actin
We discuss a theoretical model for the cooperative binding dynamics of
tropomyosin to actin filaments. Tropomyosin binds to actin by occupying seven
consecutive monomers. The model includes a strong attraction between attached
tropomyosin molecules. We start with an empty lattice and show that the binding
goes through several stages. The first stage represents fast initial binding
and leaves many small vacancies between blocks of bound molecules. In the
second stage the vacancies annihilate slowly as tropomyosin molecules detach
and re-attach. Finally the system approaches equilibrium. Using a grain-growth
model and a diffusion-coagulation model we give analytical approximations for
the vacancy density in all regimes.Comment: REVTeX, 10 pages, 9 figures; to appear in Biophysical Journal; minor
correction
Efficiency limits of the three-sphere swimmer
We consider a swimmer consisting of a collinear assembly of three spheres
connected by two slender rods. This swimmer can propel itself forward by
varying the lengths of the rods in a way that is not invariant under time
reversal. Although any non-reciprocal strokes of the arms can lead to a net
displacement, the energetic efficiency of the swimmer is strongly dependent on
the details and sequences of these strokes, and also the sizes of the spheres.
We define the efficiency of the swimmer using Lighthill's criterion, i.e., the
power that is needed to pull the swimmer by an external force at a certain
speed, divided by the power needed for active swimming with the same average
speed. Here, we determine numerically the optimal stroke sequences and the
optimal size ratio of the spheres, while limiting the maximum extension of the
rods. Our calculation takes into account both far-field and near-field
hydrodynamic interactions. We show that, surprisingly, the three-sphere swimmer
with unequal spheres can be more efficient than the equally-sized case. We also
show that the variations of efficiency with size ratio is not monotonic and
there exists a specific size ratio at which the swimmer has the highest
efficiency. We find that the swimming efficiency initially rises by increasing
the maximum allowable extension of the rods, and then converges to a maximum
value. We calculate this upper limit analytically and report the highest value
of efficiency that the three-sphere swimmer can reach.Comment: 7 pages, 3 figure
Elastically coupled molecular motors
We study the influence of filament elasticity on the motion of collective
molecular motors. It is found that for a backbone flexibility exceeding a
characteristic value (motor stiffness divided through the mean displacement
between attached motors), the ability of motors to produce force reduces as
compared to rigidly coupled motors, while the maximum velocity remains
unchanged. The force-velocity-relation in two different analytic approximations
is calculated and compared with Monte-Carlo simulations. Finally, we extend our
model by introducing motors with a strain-dependent detachment rate. A
remarkable crossover from the nearly hyperbolic shape of the Hill curve for
stiff backbones to a linear force-velocity relation for very elastic backbones
is found. With realistic model parameters we show that the backbone flexibility
plays no role under physiological conditions in muscles, but it should be
observable in certain in vitro assays.Comment: REVTeX, 13 pages, 11 figures; presentation improved; to appear in
European Physical Journal B; a Java applet showing the simulation is
accessible at http://www.physik.tu-muenchen.de/~avilfan/ecmm
Lorentz Reciprocal Theorem in Fluids with Odd Viscosity
The Lorentz reciprocal theorem -- that is used to study various transport
phenomena in hydrodynamics -- is violated in chiral active fluids that feature
odd viscosity with broken time-reversal and parity symmetries. Here we show
that the theorem can be generalized to fluids with odd viscosity by choosing an
auxiliary problem with the opposite sign of the odd viscosity. We demonstrate
the application of the theorem to two categories of microswimmers. Swimmers
with prescribed surface velocity are not affected by odd viscosity, while those
with prescribed active forces are. In particular, a torque-dipole can lead to
directed motion.Comment: 10 pages, 3 figure
Nonreciprocal interactions give rise to fast cilium synchronisation in finite systems
Motile cilia beat in an asymmetric fashion in order to propel the surrounding
fluid. When many cilia are located on a surface, their beating can synchronise
such that their phases form metachronal waves. Here, we computationally study a
model where each cilium is represented as a spherical particle, moving along a
tilted trajectory with a position-dependent active driving force and a
position-dependent internal drag coefficient. The model thus takes into account
all the essential broken symmetries of the ciliary beat. We show that taking
into account the near-field hydrodynamic interactions, the effective coupling
between cilia can become nonreciprocal: the phase of a cilium is more strongly
affected by an adjacent cilium on one side than by a cilium at the same
distance in the opposite direction. As a result, synchronisation starts from a
seed at the edge of a group of cilia and propagates rapidly across the system,
leading to a synchronisation time that scales proportionally to the linear
dimension of the system. We show that a ciliary carpet is characterised by
three different velocities: the velocity of fluid transport, the phase velocity
of metachronal waves and the group velocity of order propagation. Unlike in
systems with reciprocal coupling, boundary effects are not detrimental for
synchronisation, but rather enable the formation of the initial seed.Comment: 14 pages, 7 figures, 2 ancillary video
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