Power, chaos, and energy extraction in active nematics
ORAL
Abstract
Active nematics are an important class of fluids with both
orientational (i.e. nematic) order and an internal energy source
(i.e. activity). This energy source can drive complex fluid motion,
including chaotic advection. A prototypical example of an active
nematic consists of long filamentous bundles of microtubules
crosslinked by molecular motors which are powered by ATP. Here, we
explore the relationship between the power injected via the ATP and
the resulting chaotic mixing of the system, as measured by the
Lyapunov exponent. We see that the power and Lyapunov exponent are
proportional to one another, which helps explain why these systems
always exhibit chaotic advection in the laboratory. We also discuss
how extracting work from such a system should lower the amount of
chaotic mixing. We address these questions via theoretical
arguments, numerical simulation, and analysis of experimental data.
orientational (i.e. nematic) order and an internal energy source
(i.e. activity). This energy source can drive complex fluid motion,
including chaotic advection. A prototypical example of an active
nematic consists of long filamentous bundles of microtubules
crosslinked by molecular motors which are powered by ATP. Here, we
explore the relationship between the power injected via the ATP and
the resulting chaotic mixing of the system, as measured by the
Lyapunov exponent. We see that the power and Lyapunov exponent are
proportional to one another, which helps explain why these systems
always exhibit chaotic advection in the laboratory. We also discuss
how extracting work from such a system should lower the amount of
chaotic mixing. We address these questions via theoretical
arguments, numerical simulation, and analysis of experimental data.
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Presenters
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Kevin A Mitchell
University of California, Merced
Authors
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Kevin A Mitchell
University of California, Merced