Related Experiment Video
Updated: Jan 29, 2026

10:52
Direct Imaging of Laser-driven Ultrafast Molecular Rotation
Published on: February 4, 2017
10.2K
Self-Driven Fractional Rotational Diffusion of the Harmonic Three-Mass System
Ori Saporta Katz1, Efi Efrati1
1Department of Physics of Complex Systems, Weizmann Institute of Science, Rehovot 76100, Israel.
Physical Review Letters
|February 6, 2019
Summary
Chaotic internal dynamics in isolated nonrigid systems can cause a rotational random walk, mimicking thermal motion. This study models this phenomenon using a three-mass system, revealing Lévy walk behavior and fractional rotational diffusion.
Area of Science:
- Physics
- Nonlinear Dynamics
- Statistical Mechanics
Background:
- Isolated nonrigid systems can change orientation due to internal dynamics and angular momentum conservation laws.
- Chaotic internal dynamics in such systems can lead to macroscopic rotational behavior.
- Understanding these dynamics is crucial for modeling complex physical phenomena.
Purpose of the Study:
- To investigate the relationship between chaotic internal dynamics and macroscopic rotational behavior in isolated nonrigid systems.
- To model rotational random walk and Lévy walk phenomena using a simplified physical system.
- To analyze the statistical properties of orientation reversals and their impact on rotational diffusion.
Main Methods:
- Studied the classical harmonic three-mass system in the strongly nonlinear regime.
- Analyzed system dynamics at low, intermediate, and high energies.
- Investigated zero angular momentum rotation and chaotic dynamics.
- Examined orientation reversal statistics and rotational diffusion.
Main Results:
- At low energies, the system exhibits regular rotation with constant angular momentum.
- At high energies, a rotational random walk is observed.
- Intermediate energies show ballistic rotation bouts interrupted by orientation reversals, modeling Lévy walks.
- Orientation reversal statistics demonstrate fractional rotational diffusion.
Conclusions:
- Chaotic internal dynamics can induce macroscopic rotational random walk in isolated nonrigid systems.
- The harmonic three-mass system serves as a simple physical model for Lévy walks and fractional rotational diffusion.
- The study bridges the gap between microscopic chaotic dynamics and macroscopic emergent behavior.
Related Concept Videos
Harmonic Mean
3.7K
The arithmetic mean is usually skewed towards the larger values in the data set. Therefore, to avoid this inherent bias towards smaller values, the harmonic mean is used.
Take the example of the speed of a car, which is the measure of the rate of distance traveled. If the vehicle traverses the same distance back-and-forth, its average speed equals the total distance traveled divided by the total time taken. However, if the car moves with varying speeds, then the arithmetic mean is more skewed...
Take the example of the speed of a car, which is the measure of the rate of distance traveled. If the vehicle traverses the same distance back-and-forth, its average speed equals the total distance traveled divided by the total time taken. However, if the car moves with varying speeds, then the arithmetic mean is more skewed...
3.7K
Diffusion
218.0K
Diffusion is the passive movement of substances down their concentration gradients—requiring no expenditure of cellular energy. Substances, such as molecules or ions, diffuse from an area of high concentration to an area of low concentration in the cytosol or across membranes. Eventually, the concentration will even out, with the substance moving randomly but causing no net change in concentration. Such a state is called dynamic equilibrium, which is essential for maintaining overall...
218.0K
Diffusion
6.4K
Diffusion is a type of passive transport. In passive transport, a substance tends to move from an area of high concentration to an area of low concentration until the concentration is equal across the space. For example, take the diffusion of substances through the air. When someone opens a perfume bottle in a room filled with people, the perfume is at its highest concentration in the bottle and is at its lowest at the edges of the room. The perfume vapor will diffuse, or spread away, from the...
6.4K
Atomic Mass
70.1K
Atoms — and the protons, neutrons, and electrons that compose them — are extremely small. For example, a carbon atom weighs less than 2 × 10−23 g. When describing the properties of tiny objects such as atoms, we use appropriately small units of measure, such as the atomic mass unit (amu). The amu was originally defined based on hydrogen, the lightest element, then later in terms of oxygen. Since 1961, it has been defined with regard to the most abundant isotope of carbon, atoms of which...
70.1K
Simple Harmonic Motion
15.1K
Simple harmonic motion is the name given to oscillatory motion for a system where the net force can be described by Hooke's law. If the net force can be described by Hooke's law and there is no damping (by friction or other non-conservative forces), then a simple harmonic oscillator will oscillate with equal displacement on either side of the equilibrium position. To derive an equation for period and frequency, the equation of motion is used. The period of a simple harmonic oscillator is given...
15.1K
Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion
31.3K
Although gaseous molecules travel at tremendous speeds (hundreds of meters per second), they collide with other gaseous molecules and travel in many different directions before reaching the desired target. At room temperature, a gaseous molecule will experience billions of collisions per second. The mean free path is the average distance a molecule travels between collisions. The mean free path increases with decreasing pressure; in general, the mean free path for a gaseous molecule will be...
31.3K

