Related Experiment Video
Updated: Aug 9, 2026

08:34
Visualization of High Speed Liquid Jet Impaction on a Moving Surface
Published on: April 17, 2015
Kinetic description of avalanching systems
M Gedalin1, M Balikhin, D Coca
1Ben-Gurion University, Beer-Sheva, Israel.
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|October 26, 2005
Summary
This study introduces a kinetic description for avalanching systems using cluster distribution functions. This approach offers a more detailed understanding beyond mean-field approximations for phenomena like magnetic reconnection.
Area of Science:
- Physics
- Complex Systems
- Astrophysics
Background:
- Avalanching systems are often analyzed using renormalization group or mean-field methods.
- Mean-field approximations overlook the inhomogeneous distribution of active and passive sites.
Purpose of the Study:
- To develop a more detailed kinetic description of avalanching systems.
- To incorporate the distribution function of active site clusters into the analysis.
- To apply this formalism to specific physical systems, such as Earth's magnetosphere.
Main Methods:
- Derivation of a general kinetic equation for the temporal evolution of the cluster distribution function.
- Analysis of cluster growth and shrinking probabilities.
- Application of the kinetic formalism to a burning model and a model for magnetic reconnection.
Main Results:
- A general kinetic equation for avalanching systems is derived.
- The stationary distribution of clusters is obtained for a broad class of systems.
- The kinetic approach provides a more nuanced description than traditional methods.
Conclusions:
- The proposed kinetic description offers a powerful framework for understanding avalanching systems.
- This method enhances the analysis of complex phenomena like magnetic reconnection.
- The approach is applicable to diverse avalanching systems across various dimensions.
More Related Videos
Related Concept Videos
Kinematic Equations - I
When an object moves with constant acceleration, the velocity of the object changes at a constant rate throughout the motion. The kinematic equations of motions are derived for such cases where the acceleration of the object is constant. The first kinematic equation gives an insight into the relationship between velocity, acceleration, and time. We can see, for example:
Free-falling Bodies: Example
An object falling without any air resistance under the influence of gravitational force is said to be in free-fall. For free-falling bodies, the acceleration due to gravity is constant, irrespective of their mass. Free-fall is experienced not only by objects falling downward, but also by all objects whose motion is influenced by gravitational force alone. The dynamics of free-fall motion can be calculated using kinematic equations of motion, since free-fall acceleration is constant.
The...
The...
Energy Diagrams - I
The dynamics of a mechanical system can be easily understood by interpreting a potential energy diagram. Since energy is a scalar quantity, the interpretation of the dynamics of the system becomes even simpler.
Take the example of a skater on a parabolic ramp. The potential energy at different points along the ramp will be proportional to the height of the ramp, which varies quadratically with the horizontal position on the ramp. As the skater moves down the ramp from the highest position,...
Take the example of a skater on a parabolic ramp. The potential energy at different points along the ramp will be proportional to the height of the ramp, which varies quadratically with the horizontal position on the ramp. As the skater moves down the ramp from the highest position,...
Energy Diagrams - II
Energy diagrams are important to understand the dynamics of a system. The topology of an energy diagram helps illustrate the equilibrium points of the system.
The point in the energy diagram at which the system’s potential energy is the lowest is known as the local minima. The system tends to stay in this position indefinitely unless acted upon by a net force. The slope of the potential energy diagram at the local minima is zero, indicating that zero net force is acting on the system. The slope...
The point in the energy diagram at which the system’s potential energy is the lowest is known as the local minima. The system tends to stay in this position indefinitely unless acted upon by a net force. The slope of the potential energy diagram at the local minima is zero, indicating that zero net force is acting on the system. The slope...
Elastic Collisions: Introduction
An elastic collision is one that conserves both internal kinetic energy and momentum. Internal kinetic energy is the sum of the kinetic energies of the objects in a system. Truly elastic collisions can only be achieved with subatomic particles, such as electrons striking nuclei. Macroscopic collisions can be very nearly, but not quite, elastic, as some kinetic energy is always converted into other forms of energy such as heat transfer due to friction and sound. An example of a nearly...
Design Example: Designing Water Slide
When designing a water slide, controlling the speed of water flow is crucial for rider safety while maintaining an exciting experience. As water flows down the slide, gravity causes it to accelerate, with its speed at the bottom depending on the height from which it starts. The higher the slide, the more potential energy the water has at the top, which is converted into kinetic energy as it descends, increasing its speed.
Bernoulli's principle determines the water's velocity along the slide.
Bernoulli's principle determines the water's velocity along the slide.

