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Related Concept Videos

Applications of Integration to Probability Density Functions01:27

Applications of Integration to Probability Density Functions

Continuous probability distributions are used to model random variables that can take on any real value within a specified range. These variables do not take on isolated or countable values but rather exist on a continuum. For example, the height of an individual can be measured with increasing precision—such as 163.5 or 165.25 centimeters—demonstrating that height is a continuous random variable.The behavior of such variables is described using a probability density function (PDF), which...
Probability Distributions01:32

Probability Distributions

The probability of a random variable x  is the likelihood of its occurrence. A probability distribution represents the probabilities of a random variable using a formula, graph, or table. There are two types of probability distribution– discrete probability distribution and continuous probability distribution.
A discrete probability distribution is a probability distribution of discrete random variables. It can be categorized into binomial probability distribution and Poisson probability...
Propagation of Uncertainty from Random Error00:59

Propagation of Uncertainty from Random Error

An experiment often consists of more than a single step. In this case, measurements at each step give rise to uncertainty. Because the measurements occur in successive steps, the uncertainty in one step necessarily contributes to that in the subsequent step. As we perform statistical analysis on these types of experiments, we must learn to account for the propagation of uncertainty from one step to the next. The propagation of uncertainty depends on the type of arithmetic operation performed on...
Propagation of Uncertainty from Systematic Error01:10

Propagation of Uncertainty from Systematic Error

The atomic mass of an element varies due to the relative ratio of its isotopes. A sample's relative proportion of oxygen isotopes influences its average atomic mass. For instance, if we were to measure the atomic mass of oxygen from a sample, the mass would be a weighted average of the isotopic masses of oxygen in that sample. Since a single sample is not likely to perfectly reflect the true atomic mass of oxygen for all the molecules of oxygen on Earth, the mass we obtain from this particular...
Central Limit Theorem01:14

Central Limit Theorem

The central limit theorem, abbreviated as clt, is one of the most powerful and useful ideas in all of statistics. The central limit theorem for sample means says that if you repeatedly draw samples of a given size and calculate their means, and create a histogram of those means, then the resulting histogram will tend to have an approximate normal bell shape. In other words, as sample sizes increase, the distribution of means follows the normal distribution more closely.
The sample size, n, that...
Uniform Distribution01:19

Uniform Distribution

The uniform distribution is a continuous probability distribution of events with an equal probability of occurrence. This distribution is rectangular.Two essential properties of this distribution are The area under the rectangular shape equals 1. There is a correspondence between the probability of an event and the area under the curve.Further, the mean and standard deviation of the uniform distribution can be calculated when the lower and upper cut-offs, denoted as a and b,...

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Related Experiment Video

Updated: Jun 5, 2026

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

Unifying approach for fluctuation theorems from joint probability distributions.

Reinaldo García-García1, Daniel Domínguez, Vivien Lecomte

  • 1Centro Atómico Bariloche and Instituto Balseiro, 8400 S. C. de Bariloche, Argentina.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|January 15, 2011
PubMed
Summary

This study reveals a generalized detailed fluctuation theorem for Markovian systems, unifying various fluctuation theorems for perturbed nonequilibrium steady states. The findings simplify applications by avoiding dual probability distributions and apply to system and reservoir trajectory entropies.

Related Experiment Videos

Last Updated: Jun 5, 2026

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

Area of Science:

  • Statistical Mechanics
  • Non-equilibrium Thermodynamics
  • Physical Chemistry

Background:

  • Fluctuation theorems are crucial for understanding non-equilibrium systems.
  • Existing theorems often require specific conditions or dual distributions.
  • Trajectory entropy production is a key quantity in non-equilibrium statistical mechanics.

Purpose of the Study:

  • To establish a unified and generalized detailed fluctuation theorem for trajectory entropy production in Markovian systems.
  • To demonstrate that this theorem simplifies applications by not requiring dual probability distributions.
  • To show that various existing fluctuation theorems are special cases of this general result.

Main Methods:

  • Decomposition of total trajectory entropy production.
  • Analysis of joint probability distributions.
  • Investigation of time-reversal symmetry properties.

Main Results:

  • A generalized detailed fluctuation theorem is derived for any decomposition of trajectory entropy production in Markovian systems.
  • The theorem holds when all contributing terms are odd with respect to time reversal.
  • The joint probability distribution of system and reservoir trajectory entropies satisfies a detailed fluctuation theorem for all times.
  • Several fluctuation theorems for perturbed nonequilibrium steady states are shown to be particular cases of this general framework.

Conclusions:

  • The derived generalized fluctuation theorem offers a unified perspective on non-equilibrium statistical mechanics.
  • The simplified expression facilitates broader applications in studying complex systems.
  • The results extend the applicability of fluctuation theorems to system and reservoir dynamics.