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Related Concept Videos

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.
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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
Concept of Resonance and its Characteristics01:19

Concept of Resonance and its Characteristics

If a driven oscillator needs to resonate at a specific frequency, then very light damping is required. An example of light damping includes playing piano strings and many other musical instruments. Conversely, to achieve small-amplitude oscillations as in a car's suspension system, heavy damping is required. Heavy damping reduces the amplitude, but the tradeoff is that the system responds at more frequencies. Speed bumps and gravel roads prove that even a car's suspension system is not immune...
Damped Oscillations01:07

Damped Oscillations

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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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Fabrication and Testing of Microfluidic Optomechanical Oscillators
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Periodic patterns in a ring of delay-coupled oscillators.

P Perlikowski1, S Yanchuk, O V Popovych

  • 1Institute of Mathematics, Humboldt University of Berlin, 10099 Berlin, Germany.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|January 15, 2011
PubMed
Summary
This summary is machine-generated.

Coupling delays in oscillator rings create new rotating waves by splitting existing ones. Increasing oscillator numbers can replace these delay effects, impacting neural network models.

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Area of Science:

  • Nonlinear dynamics
  • Complex systems theory
  • Computational neuroscience

Background:

  • Spatiotemporal periodic patterns, such as rotating waves, are crucial in various natural phenomena.
  • Understanding the stability and formation of these patterns in coupled systems is a key challenge.
  • Delayed couplings introduce complex dynamics not present in instantaneous coupling models.

Purpose of the Study:

  • To investigate the impact of coupling delays on rotating waves in unidirectional oscillator rings.
  • To analyze the mechanisms underlying the splitting of rotating waves due to delays.
  • To explore alternative methods for controlling or replicating the effects of coupling delays.

Main Methods:

  • Analysis of Hopf bifurcations in systems with delayed couplings.
  • Numerical simulations using Stuart-Landau oscillators.
  • Modeling of coupled FitzHugh-Nagumo systems representing neural networks with chemical synapses.

Main Results:

  • Delayed couplings induce the splitting of single rotating waves into multiple new ones.
  • The onset of rotating waves is governed by Hopf bifurcations from a symmetric equilibrium.
  • Increasing the number of oscillators can effectively substitute for the influence of coupling delays.

Conclusions:

  • Coupling delays significantly alter the behavior of rotating waves in oscillator networks.
  • The number of oscillators is a critical parameter that can modulate the system's dynamics, mimicking delay effects.
  • Findings are applicable to understanding neuronal network synchronization and pattern formation.