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Damped Oscillations01:07

Damped Oscillations

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In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
6.0K
Types of Damping01:20

Types of Damping

6.7K
If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
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Fast Decoupled and DC Powerflow01:24

Fast Decoupled and DC Powerflow

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The fast decoupled power flow method addresses contingencies in power system operations, such as generator outages or transmission line failures. This method provides quick power flow solutions, essential for real-time system adjustments. Fast decoupled power flow algorithms simplify the Jacobian matrix by neglecting certain elements, leading to two sets of decoupled equations:
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Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

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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.
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Forced Oscillations01:06

Forced Oscillations

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When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
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Energy Considerations in Open Channel Flow01:27

Energy Considerations in Open Channel Flow

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Open channel flow, where a fluid flows with a free surface exposed to the atmosphere, is primarily governed by gravitational and surface effects, distinguishing it from closed conduit or pipe flow. In open channels such as rivers, canals, and artificial channels, energy analysis provides valuable insights into flow behavior and the relationship between depth, velocity, and slope.Specific Energy and Flow DepthIn open channel flow, the specific energy, E, combines the gravitational potential...
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Related Experiment Video

Updated: Sep 6, 2025

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

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Non-Floquet engineering in periodically driven dissipative open quantum systems.

Huan-Yu Wang1, Xiao-Ming Zhao2, Lin Zhuang3

  • 1Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|June 27, 2022
PubMed
Summary
This summary is machine-generated.

We introduce non-Floquet theory to characterize topological phases in open quantum systems. This new framework reveals how driving Floquet states can control localization and design quantum phase detectors.

Keywords:
Wannier–Stark ladderdynamical pseudo-Hermiticitynon-Floquet engineering

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Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Topological states of matter

Background:

  • Floquet engineering is crucial for dynamical topological states but limited to non-dissipative Hermitian systems.
  • Open quantum systems often exhibit non-Hermitian processes, complicating topological phase characterization.
  • Characterizing topological phases in time-periodic open quantum systems using Floquet Hamiltonians is an open challenge.

Purpose of the Study:

  • To develop a theoretical framework for characterizing topological phases in time-periodic open quantum systems.
  • To extend the understanding of Floquet engineering to non-Hermitian and dissipative systems.
  • To explore the design of quantum detectors for topological phases in dissipative oscillating fields.

Main Methods:

  • Proposing and applying the non-Floquet theory to continuously time-periodic non-Hermitian bipartite chains.
  • Utilizing a temporal non-unitary transformation on Floquet states.
  • Analyzing the resulting Floquet spectrum and localization behavior.

Main Results:

  • The non-Floquet theory transforms the Floquet spectrum into a Wannier-Stark ladder.
  • Different driving period start points lead to distinct localization behaviors.
  • Demonstrated the potential for designing quantum detectors of phases in dissipative oscillating fields.

Conclusions:

  • The non-Floquet theory provides a robust method for describing topological features in dynamical open quantum systems.
  • This approach is applicable to various driving types and can aid in constructing novel dynamical topological materials.
  • The findings open new avenues for exploring topological phenomena in open quantum systems.