Related Experiment Video
Updated: Aug 23, 2026

A Protocol for Real-time 3D Single Particle Tracking
Published on: January 3, 2018
Neural optimization of the most probable paths of three-dimensional active Brownian particles
Bin Zheng1, Zhongqiang Xiong1, Changhao Li1,2,3
1University of Chinese Academy of Sciences, Zhejiang Key Laboratory of Soft Matter Biomedical Materials, Wenzhou Institute, Wenzhou, Zhejiang 325001, China.
Abstract:
We develop a variational neural-network framework to determine the most probable path (MPP) of a 3D active Brownian particle (ABP) by directly minimizing the Onsager-Machlup integral (OMI). To obtain the OMI, we use the Onsager-Machlup variational principle for active systems and construct the Rayleighian of the ABP by including its active power. This approach reveals geometric transitions of the MPP from in-plane I- and U-shaped paths to 3D helical paths as the final time and net displacement are varied. We also demonstrate that the initial and final boundary conditions have a significant impact on the MPPs. Our results show that neural optimization combined with the Onsager-Machlup variational principle provides an efficient and versatile framework for exploring optimal transition pathways in active and nonequilibrium systems.
Related Concept Videos
Actin Polymerization and Cell Motility
Actin cytoskeleton dynamics can produce pushing, pulling, and resistance forces that help the cell to migrate.
Three-Dimensional Force System:Problem Solving
To solve a three-dimensional force system, first resolve each force into its respective scalar components. Do this using...
Actin Treadmilling
Action Potential
Membrane potential in neurons
Neurons typically have a resting membrane potential of about -70 millivolts (mV). When they receive...
Principle of Linear Impulse and Momentum for a Single Particle: Problem Solving
Maxwell-Boltzmann Distribution: Problem Solving
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
