Javascript must be enabled to continue!
Brownian motion of soft particles near a fluctuating lipid bilayer
View through CrossRef
The dynamics of a soft particle suspended in a viscous fluid can be changed by the presence of an elastic boundary. Understanding the mechanisms and dynamics of soft–soft surface interactions can provide valuable insights into many important research fields, including biomedical engineering, soft robotics development, and materials science. This work investigates the anomalous transport properties of a soft nanoparticle near a visco-elastic interface, where the particle consists of a polymer assembly in the form of a micelle and the interface is represented by a lipid bilayer membrane. Mesoscopic simulations using a dissipative particle dynamics model are performed to examine the impact of micelle’s proximity to the membrane on its Brownian motion. Two different sizes are considered, which correspond to ≈10−20nm in physical units. The wavelengths typically seen by the largest micelle fall within the range of wavenumbers where the Helfrich model captures fairly well the bilayer mechanical properties. Several independent simulations allowed us to compute the micelle trajectories during an observation time smaller than the diffusive time scale (whose order of magnitude is similar to the membrane relaxation time of the largest wavelengths), this time scale being hardly accessible by experiments. From the probability density function of the micelle normal position with respect to the membrane, it is observed that the position remains close to the starting position during ≈0.05τd (where τd corresponds to the diffusion time), which allowed us to compare the negative excess of mean-square displacement (MSD) to existing theories. In that time range, the MSD exhibits different behaviors along parallel and perpendicular directions. When the micelle is sufficiently close to the bilayer (its initial distance from the bilayer equals approximately twice its gyration radius), the micelle motion becomes quickly subdiffusive in the normal direction. Moreover, the temporal evolution of the micelle MSD excess in the perpendicular direction follows that of a nanoparticle near an elastic membrane. However, in the parallel direction, the MSD excess is rather similar to that of a nanoparticle near a liquid interface.
AIP Publishing
Title: Brownian motion of soft particles near a fluctuating lipid bilayer
Description:
The dynamics of a soft particle suspended in a viscous fluid can be changed by the presence of an elastic boundary.
Understanding the mechanisms and dynamics of soft–soft surface interactions can provide valuable insights into many important research fields, including biomedical engineering, soft robotics development, and materials science.
This work investigates the anomalous transport properties of a soft nanoparticle near a visco-elastic interface, where the particle consists of a polymer assembly in the form of a micelle and the interface is represented by a lipid bilayer membrane.
Mesoscopic simulations using a dissipative particle dynamics model are performed to examine the impact of micelle’s proximity to the membrane on its Brownian motion.
Two different sizes are considered, which correspond to ≈10−20nm in physical units.
The wavelengths typically seen by the largest micelle fall within the range of wavenumbers where the Helfrich model captures fairly well the bilayer mechanical properties.
Several independent simulations allowed us to compute the micelle trajectories during an observation time smaller than the diffusive time scale (whose order of magnitude is similar to the membrane relaxation time of the largest wavelengths), this time scale being hardly accessible by experiments.
From the probability density function of the micelle normal position with respect to the membrane, it is observed that the position remains close to the starting position during ≈0.
05τd (where τd corresponds to the diffusion time), which allowed us to compare the negative excess of mean-square displacement (MSD) to existing theories.
In that time range, the MSD exhibits different behaviors along parallel and perpendicular directions.
When the micelle is sufficiently close to the bilayer (its initial distance from the bilayer equals approximately twice its gyration radius), the micelle motion becomes quickly subdiffusive in the normal direction.
Moreover, the temporal evolution of the micelle MSD excess in the perpendicular direction follows that of a nanoparticle near an elastic membrane.
However, in the parallel direction, the MSD excess is rather similar to that of a nanoparticle near a liquid interface.
Related Results
Between the Classes of Soft Open Sets and Soft Omega Open Sets
Between the Classes of Soft Open Sets and Soft Omega Open Sets
In this paper, we define the class of soft ω0-open sets. We show that this class forms a soft topology that is strictly between the classes of soft open sets and soft ω-open sets, ...
Weaker Forms of Soft Regular and Soft T2 Soft Topological Spaces
Weaker Forms of Soft Regular and Soft T2 Soft Topological Spaces
Soft ω-local indiscreetness as a weaker form of both soft local countability and soft local indiscreetness is introduced. Then soft ω-regularity as a weaker form of both soft regul...
Brownian Particles and Matter Waves
Brownian Particles and Matter Waves
In view of the remarkable progress in microrheology to monitor the random motion of Brownian particles with size as small as few nanometers, in association that de Broglie matter w...
Brownian Particles and Matter Waves
Brownian Particles and Matter Waves
In view of the remarkable progress in microrheology to monitor the random motion of Brownian particles with size as small as few nanometers, in association that de Broglie matter w...
From Challenges to Advancement for Bilayer Tablet Technology as Drug Delivery System
From Challenges to Advancement for Bilayer Tablet Technology as Drug Delivery System
Bilayer tablet technology is in focus because it advantageous for combination therapy, for combining two different release profile and it gives patent novelty to existing dosage. H...
Soft Complete Continuity and Soft Strong Continuity in Soft Topological Spaces
Soft Complete Continuity and Soft Strong Continuity in Soft Topological Spaces
In this paper, we introduce soft complete continuity as a strong form of soft continuity and we introduce soft strong continuity as a strong form of soft complete continuity. Sever...
Soft Semi ω-Open Sets
Soft Semi ω-Open Sets
In this paper, we introduce the class of soft semi ω-open sets of a soft topological space (X,τ,A), using soft ω-open sets. We show that the class of soft semi ω-open sets contains...
Convex Hull of Brownian Motion and Brownian Bridge
Convex Hull of Brownian Motion and Brownian Bridge
In this article we study the convex hull spanned by the union of trajectories of a standard planar Brownian motion, and an independent standard planar Brownian bridge. We find the...

