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Reversible and Irreversible Processes01:14

Reversible and Irreversible Processes

The thermodynamic processes can be classified into reversible and irreversible processes. The processes that can be restored to their initial state are called reversible processes. It is only possible if the process is in quasi-static equilibrium, i.e., it takes place in infinitesimally small steps, and the system remains at equilibrium However, these are ideal processes and do not occur naturally. An ideal system undergoing a reversible process is always in thermodynamic equilibrium within...
Thermodynamic Processes01:25

Thermodynamic Processes

A thermodynamic process is a path through a sequence of states that takes a system from an initial state to a final state. In a cyclic process, the system returns to its initial state, so the changes in state properties and state functions (ΔT, Δp, ΔV, ΔU, ΔH) over one complete cycle are zero. However, heat and work transfers can still occur during the cycle, and the net heat and net work over the cycle need not be zero.A reversible process occurs when the system is infinitesimally close to...
Cyclic Processes And Isolated Systems01:19

Cyclic Processes And Isolated Systems

A thermodynamic system with zero heat exchange and work is an isolated system. For these systems, the internal energy remains constant.
In the case of a non-isolated system, the change in the internal energy is zero only if the process is cyclic. A thermodynamic process is considered cyclic if the system undergoes a series of changes and returns to its initial state. 
Consider a cyclic process that returns to its initial state, undergoing a four-step process. The heat transfer along each path...
Non-equilibrium in the Cell01:16

Non-equilibrium in the Cell

An important concept in studying metabolism and energy is that of chemical equilibrium. Most chemical reactions are reversible. They can proceed in both directions, releasing energy into their environment in one direction, and absorbing it from the environment in the other direction. The same is true for the chemical reactions involved in cell metabolism, such as the breaking down and building up of proteins into and from individual amino acids, respectively. Reactants within a closed system...
Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

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.
Free Energy Changes for Nonstandard States03:25

Free Energy Changes for Nonstandard States

The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:

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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
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Far-from-equilibrium processes without net thermal exchange via energy sorting.

Jose M G Vilar1, J Miguel Rubi

  • 1Biophysics Unit (CSIC-UPV/EHU) and Department of Biochemistry and Molecular Biology, University of the Basque Country, 48080 Bilbao, Spain. j.vilar@ikerbasque.org

The Journal of Chemical Physics
|February 25, 2012
PubMed
Summary

Scientists discovered "ghost equilibrium," a new far-from-equilibrium process that controls microscale systems without disturbing thermal properties. This method enables precise energy manipulation in nanoscale devices by suppressing environmental heat exchange.

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Area of Science:

  • Microscale physics
  • Statistical mechanics
  • Non-equilibrium thermodynamics

Background:

  • Many microscale processes require far-from-equilibrium conditions.
  • Energy inputs for these conditions often disrupt thermal properties and system control.
  • Existing methods lack precise control over thermal exchange.

Purpose of the Study:

  • To introduce a novel class of far-from-equilibrium processes.
  • To demonstrate a method for suppressing net thermal exchange with the environment.
  • To enable controlled energy manipulation at the microscale.

Main Methods:

  • Statistical cancellation of nonequilibrated degrees of freedom.
  • Microscale energy sorting process.
  • Analysis of Maxwell-Boltzmann velocity distribution maintenance.
  • Application to rotational dipoles and trapped particle gases.

Main Results:

  • A phenomenon termed "ghost equilibrium" was identified.
  • Ghost equilibrium suppresses net thermal exchange while maintaining equilibrium velocity distribution.
  • Autonomous generation of superheated and subcooled degrees of freedom.
  • Demonstrated control over energy in microscale systems.

Conclusions:

  • Ghost equilibrium offers a new paradigm for far-from-equilibrium processes.
  • This phenomenon allows for precise control of microscale systems.
  • Potential applications in mesoscopic bioreactors, nanoscopic rotors, and nanoscale mass conveyors.