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Related Concept Videos

Damped Oscillations01:07

Damped Oscillations

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...
Forced Oscillations01:06

Forced Oscillations

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.
Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
RLC Circuit as a Damped Oscillator01:30

RLC Circuit as a Damped Oscillator

An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
Design Example: Underdamped Parallel RLC Circuit01:17

Design Example: Underdamped Parallel RLC Circuit

Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
Time and frequency -Domain Interpretation of Phase-lag Control01:21

Time and frequency -Domain Interpretation of Phase-lag Control

Phase-lag controllers are widely used in control systems to improve stability and reduce steady-state errors. A dimmer switch controlling the brightness of a light bulb serves as a practical example of phase-lag control, gradually adjusting the bulb's brightness. Mathematically, phase-lag control or low-pass filtering is represented when the factor 'a' is less than 1.
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Fabrication and Testing of Microfluidic Optomechanical Oscillators
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Changing dynamical complexity with time delay in coupled fiber laser oscillators.

Anthony L Franz1, Rajarshi Roy, Leah B Shaw

  • 1Department of Physics, University of Maryland, College Park, Maryland 20742, USA.

Physical Review Letters
|October 13, 2007
PubMed
Summary

We studied coupled systems with delays, finding that short delays reduce complexity. Increasing coupling delay logarithmically increases dynamical complexity in these systems.

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Area of Science:

  • Nonlinear Dynamics
  • Complex Systems
  • Optical Engineering

Background:

  • Mutually coupled systems exhibit complex behaviors.
  • Internal and coupling delays significantly influence system dynamics.
  • Understanding delay effects is crucial for controlling complex systems.

Purpose of the Study:

  • To investigate the impact of coupling delay on the dynamical complexity of two mutually coupled systems.
  • To quantify complexity changes across four orders of magnitude of coupling delay.
  • To analyze the relationship between delay duration and system complexity.

Main Methods:

  • Karhunen-Loève decomposition applied to spatiotemporal data of fiber laser intensity.
  • Analysis of eigenvalue spectra and significant orthogonal modes.
  • Shannon information computed from eigenvalue spectra to quantify complexity.

Main Results:

  • Dynamical complexity is reduced at short coupling delays.
  • A logarithmic growth in complexity is observed as coupling delay increases.
  • Eigenvalue spectra and orthogonal modes reveal changes in system dynamics with delay.

Conclusions:

  • Coupling delay is a critical parameter influencing the complexity of mutually coupled systems.
  • Short delays can stabilize systems by reducing complexity.
  • Longer delays lead to a predictable increase in dynamical complexity.