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Related Concept Videos

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...
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.
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...
Damped Oscillations01:07

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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.
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Oscillations about an Equilibrium Position01:04

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Stability is an important concept in oscillation. If an equilibrium point is stable, a slight disturbance of an object that is initially at the stable equilibrium point will cause the object to oscillate around that point. For an unstable equilibrium point, if the object is disturbed slightly, it will not return to the equilibrium point. There are three conditions for equilibrium points—stable, unstable, and half-stable. A half-stable equilibrium point is also unstable, but is named so because...

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Related Experiment Video

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Fabrication and Testing of Microfluidic Optomechanical Oscillators
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Published on: May 29, 2014

Exact folded-band chaotic oscillator.

Ned J Corron1, Jonathan N Blakely

  • 1U. S. Army RDECOM, RDMR-WSS, Redstone Arsenal, Alabama 35898, USA. ned.corron@us.army.mil

Chaos (Woodbury, N.Y.)
|July 5, 2012
PubMed
Summary

This study presents an exactly solvable chaotic oscillator with a folded-band structure, demonstrating provably chaotic behavior and an exact solution derived from its hybrid dynamics. The findings reveal a connection between the folded-band topology and symbol grammar.

Area of Science:

  • Dynamical Systems
  • Chaos Theory
  • Nonlinear Dynamics

Background:

  • Chaotic oscillators are fundamental in understanding complex systems.
  • Hybrid dynamical systems offer unique behaviors not found in purely continuous or discrete systems.
  • Folded-band dynamics, observed in systems like Rössler's oscillator, are crucial for complex chaotic behavior.

Purpose of the Study:

  • To introduce and analyze an exactly solvable chaotic oscillator.
  • To investigate the properties of its folded-band dynamics.
  • To establish a connection between the oscillator's dynamics and symbolic representations.

Main Methods:

  • The study employs a hybrid dynamical system combining a linear ordinary differential equation with a nonlinear switching condition.

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  • Exact solutions are derived using linear convolution of a basis pulse and a binary sequence.
  • Symbolic dynamics are obtained from the exact solution.
  • Main Results:

    • The bounded oscillations of the hybrid system are proven to be chaotic.
    • A one-dimensional piecewise-linear return map with segments of positive and negative slopes is generated from waveform maxima.
    • The continuous-time dynamics exhibit a folded-band topology.
    • An exact solution is formulated, enabling the derivation of equivalent symbolic dynamics.

    Conclusions:

    • The developed oscillator is exactly solvable and exhibits chaotic behavior.
    • The folded-band topology is intrinsically linked to the symbol grammar of the system.
    • This work provides a novel model for studying chaotic phenomena in hybrid systems.