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Related Concept Videos

Work and Heat01:30

Work and Heat

Work and heat are fundamental concepts in thermodynamics, denoting the transfer of energy. Work is the energy transferred due to the movement of an object under force, represented as the dot product of the force and displacement vectors. An example can be seen in a gas confined by a frictionless piston. The gas performs work on its surroundings when the piston moves outward, reducing the system's energy.This infinitesimal amount of work (dw) performed by the system against a constant external...
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As a system undergoes a change, its internal energy can change, and energy can be transferred from the system to the surroundings, or from the surroundings to the system.
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Thermodynamic systems undergoing phase transitions or temperature changes experience energy transfer in the form of heat (q) and work (w). For a reversible phase change at constant temperature (T) and pressure (p), the process involves no chemical reaction but results in energy exchange between distinct phases.The heat transferred during this process corresponds to the latent heat of transition, which is the amount of heat energy absorbed or released by a substance when it changes from one...
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State Function, Exact and Inexact Differentials

A state function is a thermodynamic property that depends solely on the current state of a system, irrespective of its history or how it arrived at that state. These functions are represented by capital letters, such as U, H, and S, which stand for internal energy, enthalpy, and entropy, respectively.For instance, the value of internal energy depends on the system's state variables and remains unaffected by the process path. This means that whether the system underwent a linear process or a...
Calculation of First-Law Quantities II01:24

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The first law of thermodynamics establishes that the change in internal energy of a system is given by ΔU = q + w, where q is the heat exchanged, and w is the work performed. For a perfect gas, both internal energy (U) and enthalpy (H) depend solely on temperature. Consequently, for any change of state, whether reversible or irreversible, the internal energy change is determined by integrating the heat capacity at constant volume, and the enthalpy change by integrating the heat capacity at...
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Work is done when energy is transferred from one object to another. In other words, work is when a force acts on something that undergoes a displacement from one position to another. Forces can vary as a function of position, and displacements can be along various paths between two points. The increment of work (dW) done by a force acting through an infinitesimal displacement can be defined as the dot product of force () and displacement () vectors.
The dot product can be expressed in terms of...

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Fluctuation symmetries for work and heat.

Marco Baiesi1, Tim Jacobs, Christian Maes

  • 1Instituut voor Theoretische Fysica, KU Leuven, Celestijnenlaan 200D, B-3001 Leuven, Belgium.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|October 10, 2006
PubMed
Summary

This study examines a particle in a medium using a Langevin equation. It identifies conditions for exact work fluctuation symmetry and discusses corrections to heat fluctuation theorems.

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Area of Science:

  • Statistical Mechanics
  • Non-equilibrium Thermodynamics
  • Physical Chemistry

Background:

  • The Langevin equation describes particle dynamics in a medium, influenced by random forces and friction.
  • Fluctuation theorems in non-equilibrium systems relate work and heat under specific conditions.

Purpose of the Study:

  • To investigate the conditions under which fluctuations of dissipative work satisfy an exact symmetry.
  • To analyze the validity of fluctuation theorems for dissipated heat, considering temporal boundary effects.

Main Methods:

  • Utilizing a Langevin equation with a time-dependent potential driven by an external protocol.
  • Deriving and analyzing the fluctuation theorems for dissipative work and heat.

Main Results:

  • Identified specific conditions on the potential and external protocol for exact work fluctuation symmetry.
  • Presented counterexamples where these conditions are not met, violating the standard fluctuation theorem.
  • Derived a corrected fluctuation relation for dissipated heat, accounting for temporal boundary terms, which holds generally.

Conclusions:

  • The study provides precise conditions for the validity of work fluctuation theorems in driven systems.
  • A generalized fluctuation relation for dissipated heat is established, addressing limitations of standard theorems.