Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Region of Convergence of Laplace Tarnsform01:20

Region of Convergence of Laplace Tarnsform

692
The Region of Convergence (ROC) is a fundamental concept in signal processing and system analysis, particularly associated with the Laplace transform. The ROC represents an area in the complex plane where the Laplace transform of a given signal converges, determining the transform's applicability and utility.
Consider a decaying exponential signal that begins at a specific time. When deriving its Laplace transform, the time-domain variable is replaced with a complex variable. This...
692
Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

2.7K
In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
2.7K
Path Between Thermodynamics States01:21

Path Between Thermodynamics States

3.3K
Consider the two thermodynamic processes involving an ideal gas that are represented by paths AC and ABC in Figure 1:
3.3K
Entropy02:39

Entropy

31.0K
Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
31.0K
Thermodynamic Systems01:06

Thermodynamic Systems

5.4K
A thermodynamic system is a set of objects whose thermodynamic properties are of interest. The system is considered to be embedded in its surroundings or the environment. The system and its environment can exchange heat and do work on each other through a boundary that separates them. However, the immediate surroundings of the system interact with it directly and therefore have a much stronger influence on its behavior and properties.
Consider an example of  tea boiling in a kettle. The...
5.4K
Reynolds Transport Theorem01:24

Reynolds Transport Theorem

1.3K
The Reynolds transport theorem provides a framework to relate the time rate of change of an extensive property within a system to that in a control volume, which is crucial for analyzing fluid dynamics. Extensive properties, such as mass, velocity, acceleration, temperature, and momentum, can be expressed in terms of the mass of a fluid portion. These properties are called extensive because they depend on the system's size, while intensive properties are their corresponding values per unit...
1.3K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Trotter transition in Bardeen-Cooper-Schrieffer pairing dynamics.

Physical review. E·2026
Same author

Impact of on-site potentials on q breathers in nonlinear chains.

Physical review. E·2025
Same author

Prethermalization in Fermi-Pasta-Ulam-Tsingou chains.

Physical review. E·2025
Same author

Flat band fine-tuning and its photonic applications.

Nanophotonics (Berlin, Germany)·2024
Same author

Dynamical chaos in the integrable Toda chain induced by time discretization.

Chaos (Woodbury, N.Y.)·2024
Same author

Thermalization slowing down in multidimensional Josephson junction networks.

Physical review. E·2024

Related Experiment Video

Updated: Sep 6, 2025

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

8.6K

Thermalization dynamics of macroscopic weakly nonintegrable maps.

Merab Malishava1, Sergej Flach1

  • 1Center for Theoretical Physics of Complex Systems, Institute for Basic Science (IBS), Daejeon 34126, South Korea.

Chaos (Woodbury, N.Y.)
|July 1, 2022
PubMed
Summary

This study reveals two thermalization regimes in nonlinear lattice dynamics. It characterizes network coupling and ergodization times, offering insights into macroscopic thermalization.

More Related Videos

Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package
06:37

Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package

Published on: September 17, 2021

4.6K
Spatiotemporal Mapping of Motility in Ex Vivo Preparations of the Intestines
12:00

Spatiotemporal Mapping of Motility in Ex Vivo Preparations of the Intestines

Published on: January 27, 2016

10.5K

Related Experiment Videos

Last Updated: Sep 6, 2025

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

8.6K
Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package
06:37

Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package

Published on: September 17, 2021

4.6K
Spatiotemporal Mapping of Motility in Ex Vivo Preparations of the Intestines
12:00

Spatiotemporal Mapping of Motility in Ex Vivo Preparations of the Intestines

Published on: January 27, 2016

10.5K

Area of Science:

  • Physics
  • Nonlinear Dynamics
  • Statistical Mechanics

Background:

  • Studying thermalization in nonlinear systems is crucial for understanding complex dynamics.
  • Weakly nonintegrable systems offer a unique window into the transition from order to chaos.
  • Lattice dynamics provide a fundamental model for exploring emergent phenomena.

Purpose of the Study:

  • To identify and characterize distinct thermalization regimes in weakly nonintegrable nonlinear unitary lattice dynamics.
  • To investigate the relationship between network coupling (long-range vs. short-range) and observable types.
  • To compare thermalization timescales with Lyapunov exponents for a comprehensive understanding.

Main Methods:

  • Analysis of thermalization in nonlinear unitary lattice dynamics near integrable limits.
  • Computation of the variance of finite-time average distributions for extended and local observables.
  • Complementary analysis of Lyapunov spectra and comparison with ergodization time scales.

Main Results:

  • Identification of two distinct thermalization regimes: one associated with linear dynamics and long-range networks, the other with disconnected lattices and short-range networks.
  • Extraction of the ergodization time scale (T_E) marking the onset of thermalization.
  • Characterization of network types through the decay of variance (σ(T)) and comparison of T_E with Lyapunov time (T_L).

Conclusions:

  • A complete classification of weakly nonintegrable macroscopic thermalization dynamics is established.
  • The study provides a detailed picture of how different network structures influence thermalization processes.
  • The findings bridge the gap between microscopic dynamics and macroscopic thermal behavior in complex systems.