| Autor: |
Misselwitz AP; Center for Protein Assemblies (CPA) and Department of Bioscience, School of Natural Sciences, Technische Universität München, Garching b. München 85748, Germany., Lafon S; Paris-Saclay University, CNRS, Solid State Physics Laboratory, Orsay 91405, France.; Max Planck Institute for Dynamics and Self-Organization, Göttingen 37077, Germany., Julien JD; Max Planck Institute for Dynamics and Self-Organization, Göttingen 37077, Germany., Alim K; Center for Protein Assemblies (CPA) and Department of Bioscience, School of Natural Sciences, Technische Universität München, Garching b. München 85748, Germany.; Max Planck Institute for Dynamics and Self-Organization, Göttingen 37077, Germany. |
| Abstrakt: |
Models of pulse formation in nerve conduction have provided manifold insight not only into neuronal dynamics but also the nonlinear dynamics of pulse formation in general. Recent observation of neuronal electrochemical pulses also driving mechanical deformation of the tubular neuronal wall, and thereby generating ensuing cytoplasmic flow, now question the impact of flow on the electrochemical dynamics of pulse formation. Here, we theoretically investigate the classical Fitzhugh-Nagumo model, now accounting for advective coupling between the pulse propagator typically describing membrane potential and triggering mechanical deformations, and thus governing flow magnitude, and the pulse controller, a chemical species advected with the ensuing fluid flow. Employing analytical calculations and numerical simulations, we find that advective coupling allows for a linear control of pulse width while leaving pulse velocity unchanged. We therefore uncover an independent control of pulse width by fluid flow coupling. |
