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Related Concept Videos

Non-conservative Forces01:17

Non-conservative Forces

Non-conservative forces are dissipative forces such as friction or air resistance. These forces take energy away from a system as it progresses. Unlike conservative forces, non-conservative forces do not have potential energy associated with them. This is because the energy is lost to the system and cannot be turned into useful work later.
Also unlike their conservative counterparts, they are path-dependent; where the object starts and stops does matter. For example, a grinding wheel applies a...
Work Done on a System by External Force01:11

Work Done on a System by External Force

The work done by an external force on a particle changes its kinetic energy. However, internal forces must also be considered for a system of interacting particles. The potential energy formulation helps formulate the effect of internal forces. The net work done by an external force can be written in terms of the total change of mechanical energy, which includes both kinetic and potential energies.
In the presence of a non-conservative opposing force, like friction, some part of the work done...
Internal and External Forces01:12

Internal and External Forces

Newton's first law states that a net external force causes a change in motion. External forces act on an object or system, originating outside of the object or system. In contrast, internal forces originate inside the system of interest and do not lead to any acceleration. In simpler words, internal forces are forces that act on one part of an object and are exerted by another part of the same object. External forces are forces that act on an object due to some other object. Therefore, when...
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Work and Energy for Variable Forces

When an object is acted upon by a variable force, the amount of work done and the change in energy of the object can be more complex to calculate compared to when a constant force is applied. Work is the product of force and displacement, while energy is the capacity of a system to do work. When a constant force is applied to an object, the work done can be calculated as the product of the force and the distance moved in the direction of the force. However, when a variable force is applied, the...
Basic Continuous Time Signals01:22

Basic Continuous Time Signals

Basic continuous-time signals include the unit step function, unit impulse function, and unit ramp function, collectively referred to as singularity functions. Singularity functions are characterized by discontinuities or discontinuous derivatives.
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Mean free path and Mean free time01:22

Mean free path and Mean free time

Consider the gas molecules in a cylinder. They move in a random motion as they collide with each other and change speed and direction. The average of all the path lengths between collisions is known as the "mean free path."

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Age-dependent Dynamics of Locomotion in Caenorhabditis elegans: A Lyapunov Exponent Analysis
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Age-dependent Dynamics of Locomotion in Caenorhabditis elegans: A Lyapunov Exponent Analysis

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Continuous time random walk with generic waiting time and external force.

Kwok Sau Fa1, K G Wang

  • 1Departamento de Física, Universidade Estadual de Maringá, Av. Colombo 5790, 87020-900 Maringá, PR, Brazil. kwok@dfi.uem.br

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|September 28, 2010
PubMed
Summary
This summary is machine-generated.

This study introduces a new diffusion equation for continuous time random walks, applicable to various waiting times and forces. It demonstrates that the generalized Einstein relation holds universally for any waiting time distribution.

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Area of Science:

  • Physics
  • Statistical Mechanics
  • Physical Chemistry

Background:

  • Continuous Time Random Walks (CTRWs) are fundamental models for anomalous diffusion.
  • Existing diffusion equations often rely on specific assumptions about waiting time distributions.
  • Understanding diffusion under external forces requires a generalized theoretical framework.

Purpose of the Study:

  • To derive a generalized integrodifferential diffusion equation for CTRRWs.
  • To analyze diffusion behavior for various waiting time probability density functions (WTPDFs) under a harmonic trap.
  • To investigate the applicability of the second Einstein relation for arbitrary WTPDFs.

Main Methods:

  • Derivation of an integrodifferential diffusion equation for CTRRWs.
  • Analysis of specific WTPDFs: exponential, power law + Mittag-Leffler, and sum of exponentials.
  • Study of diffusion under a harmonic external potential.

Main Results:

  • The derived equation is valid for generic WTPDFs and external forces.
  • Exponential and power law + Mittag-Leffler WTPDFs reproduce standard and fractional diffusion results.
  • A sum of exponentials WTPDF exhibits complex diffusion patterns.
  • The second Einstein relation is shown to hold universally for any WTPDF.

Conclusions:

  • The generalized diffusion equation provides a unified framework for CTRRWs.
  • The choice of WTPDF significantly impacts diffusion dynamics.
  • The universality of the second Einstein relation is confirmed, offering broad applicability.