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Related Concept Videos

Entropy01:18

Entropy

The first law of thermodynamics is quantitatively formulated via an equation relating the internal energy of a system, the heat exchanged by it, and the work done on it. A quantitative formulation of the second law of thermodynamics leads to defining a state function, the entropy.
When an ideal gas expands isothermally, the disorder in the gas increases. From the molecular perspective, the gas molecules have more volume to move around in.
Consider an infinitesimal step in the expansion, which...
Entropy02:39

Entropy

Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
Random Variables01:09

Random Variables

A random variable is a single numerical value that indicates the outcome of a procedure. The concept of random variables is fundamental to the probability theory and was introduced by a Russian mathematician, Pafnuty Chebyshev, in the mid-nineteenth century.
Uppercase letters such as X or Y denote a random variable. Lowercase letters like x or y denote the value of a random variable. If X is a random variable, then X is written in words, and x is given as a number.
For example, let X = the...
The Entropy as a State Function01:14

The Entropy as a State Function

Consider an arbitrary process that moves between two specific states (A and B) in a cyclic manner. This process is reversible and broken down into smaller parts that each follow a Carnot cycle. A Carnot cycle has two isothermal (constant temperature) processes. During these processes, the ratio of the amount of heat transferred to their respective temperature remains constant. The other two processes in the Carnot cycle are also reversible but adiabatic, which means they occur without any heat...
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.
Entropy Changes Accompanying Specific Processes01:21

Entropy Changes Accompanying Specific Processes

Entropy, a measure of disorder in a system, changes during phase transitions like freezing or boiling. At the transition temperature Ttrs, where two phases are in equilibrium, the phase transition is a reversible process. The entropy change can be calculated from a substance's enthalpy of transition using the equation ΔStrs = ΔtrsH /Ttrs.When a perfect gas expands isothermally from one volume to another, entropy increases logarithmically with volume. Conversely, isothermal compression results...

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Updated: Jun 18, 2026

Measuring the Subjective Value of Risky and Ambiguous Options using Experimental Economics and Functional MRI Methods
13:04

Measuring the Subjective Value of Risky and Ambiguous Options using Experimental Economics and Functional MRI Methods

Published on: September 19, 2012

Boolean chaos.

Rui Zhang1, Hugo L D de S Cavalcante, Zheng Gao

  • 1Department of Physics and Center for Nonlinear and Complex Systems, Duke University, Durham, North Carolina 27708, USA. rz10@phy.duke.edu

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|November 13, 2009
PubMed
Summary
This summary is machine-generated.

Researchers discovered deterministic chaos in electronic logic gates without clock signals, creating ultrawideband signals up to 2 GHz. This electronic Boolean chaos could be used for ultrawideband radio wave generation.

Related Experiment Videos

Last Updated: Jun 18, 2026

Measuring the Subjective Value of Risky and Ambiguous Options using Experimental Economics and Functional MRI Methods
13:04

Measuring the Subjective Value of Risky and Ambiguous Options using Experimental Economics and Functional MRI Methods

Published on: September 19, 2012

Area of Science:

  • Nonlinear dynamics
  • Electronic circuits
  • Chaos theory

Background:

  • Deterministic chaos is a complex behavior observed in nonlinear systems.
  • Electronic logic gates are fundamental components in digital systems.
  • Clocking signals are typically used to synchronize operations in digital circuits.

Purpose of the Study:

  • To investigate the emergence of deterministic chaos in a simple network of electronic logic gates operating without a clock signal.
  • To characterize the power spectrum of the chaotic signals generated.
  • To develop a model that can qualitatively reproduce the observed chaotic behavior.

Main Methods:

  • Experimental observation of signal behavior in an asynchronous electronic logic gate network.
  • Analysis of the power spectrum of the generated signals.
  • Development and simulation of an autonomously updating Boolean model incorporating history-dependent propagation times and pulse filtering.

Main Results:

  • Deterministic chaos was observed in the asynchronous electronic logic gate network.
  • The resulting power spectrum was ultrawideband, extending from DC to over 2 GHz.
  • The Boolean model qualitatively reproduced the experimental observations, including the effects of signal history and pulse filtering.

Conclusions:

  • Asynchronous electronic logic gate networks can exhibit deterministic chaos.
  • This phenomenon generates ultrawideband signals with potential applications.
  • Electronic Boolean chaos offers a novel approach for ultrawideband radio wave generation.