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Related Concept Videos

Work Done in an Adiabatic Process01:20

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Consider the adiabatic compression of an ideal gas in the cylinder of an automobile diesel engine. The gasoline vapor is injected into the cylinder of an automobile engine when the piston is in its expanded position. The temperature, pressure, and volume of the resulting gas-air mixture are 20 °C, 1.00 x 105 N/m2, and 240 cm3 , respectively. The mixture is then compressed adiabatically to a volume of 40 cm3. Note that, in the actual operation of an automobile engine, the compression is not...
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When an ideal gas is compressed adiabatically, that is, without adding heat, work is done on it, and its temperature increases. In an adiabatic expansion, the gas does work, and its temperature drops. Adiabatic compressions actually occur in the cylinders of a car, where the compressions of the gas-air mixture take place so quickly that there is no time for the mixture to exchange heat with its environment. Nevertheless, because work is done on the mixture during the compression, its...
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Free expansion of a gas is an adiabatic process. However, there are few differences between free expansion and adiabatic expansion. During free expansion, no work is done, and there is no change in internal energy. But, for an adiabatic expansion, work is done, and there is a change in internal energy. During an adiabatic process, the relation between the pressure and volume is obtained from the condition for the adiabatic process, that is,
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The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
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Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
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Calculating work in adiabatic two-level quantum Markovian master equations: a characteristic function method.

Fei Liu1

  • 1School of Physics and Nuclear Energy Engineering, Beihang University, Beijing 100191, China.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|October 15, 2014
PubMed
Summary
This summary is machine-generated.

We developed a new method to calculate work probability distributions in quantum systems. This approach reveals that work fluctuations in driven systems mirror those in isolated systems, offering insights into quantum thermodynamics.

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Area of Science:

  • Quantum thermodynamics
  • Quantum information theory
  • Statistical mechanics

Background:

  • Quantum Markovian master equations describe open quantum systems.
  • Adiabatic processes involve slow parameter changes.
  • Work in quantum systems is a key observable in thermodynamics.

Purpose of the Study:

  • To develop a characteristic function method for calculating work probability distributions.
  • To investigate the fluctuation properties of work in driven quantum systems.
  • To connect work fluctuations in open systems to those in isolated systems.

Main Methods:

  • Characteristic function method derived from quantum jump interpretation.
  • Application to adiabatic two-level quantum Markovian master equations.
  • Analysis of fluctuation properties using symmetry of characteristic functions.

Main Results:

  • The method successfully calculates probability density functions for inclusive work.
  • Fluctuation properties of work exhibit symmetry, similar to isolated systems.
  • A periodically driven two-level model validates the theoretical framework.

Conclusions:

  • The characteristic function method provides a robust tool for analyzing quantum work.
  • Symmetry in work fluctuations offers a universal characteristic across different quantum systems.
  • This work deepens the understanding of thermodynamics in open quantum systems.