Related Experiment Video
Updated: Mar 8, 2026

11:03
An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
Published on: December 4, 2017
9.1K
Overdamped stochastic thermodynamics with multiple reservoirs
Yûto Murashita1, Massimiliano Esposito2
1Department of Physics, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo, 113-0033, Japan.
Physical Review. E
|January 14, 2017
Summary
We developed a new theory for stochastic thermodynamics in overdamped systems with multiple heat reservoirs, revealing differences from naive theories. This work clarifies heat conduction in complex systems.
Area of Science:
- Statistical Mechanics
- Non-equilibrium Thermodynamics
- Soft Matter Physics
Background:
- Stochastic thermodynamics describes heat, work, and entropy in small systems.
- Existing theories often simplify systems to single reservoirs or overdamped dynamics.
- The behavior of systems with multiple reservoirs and underdamped dynamics is less understood.
Purpose of the Study:
- To derive the overdamped limit of stochastic thermodynamics for systems with multiple reservoirs.
- To compare this derived theory with naive approaches based on overdamped Langevin or Fokker-Planck equations.
- To investigate the fundamental fluctuation theorems and heat statistics in these systems.
Main Methods:
- Established stochastic thermodynamics for underdamped Langevin systems coupled to multiple reservoirs.
- Employed timescale separation techniques to derive the corresponding overdamped limit.
- Analyzed heat statistics for a Brownian particle on a ring with two reservoirs and a nonconservative force.
Main Results:
- The derived overdamped theory differs from naive theories, especially with multiple reservoirs.
- This discrepancy arises because fast momentum dynamics reach a non-equilibrium state, enabling heat conduction.
- Both underdamped and overdamped theories satisfy fundamental fluctuation theorems.
Conclusions:
- The study provides a more accurate stochastic thermodynamic framework for overdamped systems with multiple reservoirs.
- The findings highlight the importance of considering non-equilibrium momentum dynamics in coarse-grained descriptions.
- Analytical predictions for heat statistics in a model system confirm the validity of the derived theories.
Related Concept Videos
Types of Damping
7.9K
If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
7.9K
Damped Oscillations
7.4K
In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Although friction and other non-conservative...
7.4K
Entropy Change in Reversible Processes
3.3K
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.
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.
3.3K
Second Order systems II
445
In an underdamped second-order system, where the damping ratio ζ is between 0 and 1, a unit-step input results in a transfer function that, when transformed using the inverse Laplace method, reveals the output response. The output exhibits a damped sinusoidal oscillation, and the difference between the input and output is termed the error signal. This error signal also demonstrates damped oscillatory behavior. Eventually, as the system reaches a steady state, the error diminishes to zero.
445
Second Law of Thermodynamics
27.4K
In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Processes that involve an increase in entropy of the system (ΔS > 0) are very often spontaneous; however, examples to the contrary are plentiful. By expanding consideration of entropy changes to include the surroundings, a significant conclusion regarding the relation between this property and spontaneity may be reached. In thermodynamic models, the...
27.4K
Second Law of Thermodynamics
70.0K
The Second Law of Thermodynamics states that entropy, or the amount of disorder in a system, increases each time energy is transferred or transformed. Each energy transfer results in a certain amount of energy that is lost—usually in the form of heat—that increases the disorder of the surroundings. This can also be demonstrated in a classic food web. Herbivores harvest chemical energy from plants and release heat and carbon dioxide into the environment. Carnivores harvest the...
70.0K

