Brownian motion near an elastic cell membrane: A theoretical study
arXiv:1709.04915 · doi:10.1140/epje/i2018-11627-6
Abstract
Elastic confinements are an important component of many biological systems and dictate the transport properties of suspended particles under flow. In this chapter, we review the Brownian motion of a particle moving in the vicinity of a living cell whose membrane is endowed with a resistance towards shear and bending. The analytical calculations proceed through the computation of the frequency-dependent mobility functions and the application of the fluctuation-dissipation theorem. Elastic interfaces endow the system with memory effects that lead to a long-lived anomalous subdiffusive regime of nearby particles. In the steady limit, the diffusional behavior approaches that near a no-slip hard wall. The analytical predictions are validated and supplemented with boundary-integral simulations.
16 pages, 7 figures and 161 references. Contributed chapter to the flowing matter book
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Cited by in corpus (11)
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- A reciprocal theorem for the prediction of the normal force induced on a particle translating parallel to an elastic membrane
- Frequency-dependent higher-order Stokes singularities near a planar elastic boundary: implications for the hydrodynamics of an active microswimmer near an elastic interface
- Hydrodynamic coupling and rotational mobilities near planar elastic membranes
- Creeping motion of a solid particle inside a spherical elastic cavity
- Creeping motion of a solid particle inside a spherical elastic cavity. II. Asymmetric motion
- Axisymmetric Stokes flow due to a point-force singularity acting between two coaxially positioned rigid no-slip disks
- Theory of active particle penetration through a planar elastic membrane
- Asymmetric Stokes flow induced by a transverse point-force acting near a finite-sized elastic membrane
- A note on forces exerted by a Stokeslet on confining boundaries
- Dynamics of a simple model microswimmer in an anisotropic fluid: implications for alignment behavior and active transport in a nematic liquid crystal